Open Access Article
Mohamed A. Elokl
,
Ahmed G. Ali
,
Abdelrahman M. Abdelmohsen
,
Ahmed A. Taha
,
Abdelrahman A. Ashour
,
Salma Elshabrawy
and
Nageh K. Allam
*
Energy Materials Laboratory (EML), Physics Department, School of Sciences and Engineering, The American University in Cairo, New Cairo 11835, Egypt. E-mail: nageh.allam@aucegypt.edu
First published on 12th February 2026
Carbon dioxide (CO2) is both the principal anthropogenic greenhouse gas and a valuable, non-toxic, and abundant C1 feedstock for sustainable fuel and chemical production. Conventional approaches have typically addressed CO2 capture and CO2 conversion as independent processes; however, each remains energy-intensive and economically constrained when implemented in isolation. The emerging concept of integrated CO2 capture and conversion (ICCC) offers a transformative strategy to simultaneously mitigate CO2 emissions and synthesize value-added products within a unified system. Unlike the simple sequential coupling of capture and utilization, ICCC demands the synergistic integration of capture media, catalytic interfaces, and reaction environments, requiring interdisciplinary insight spanning materials chemistry, catalysis, and electrochemical engineering. This review critically surveys recent progress in ICCC with a focus on dual-functional materials (DFMs) that enable concurrent CO2 capture and catalytic conversion. The discussion encompasses a broad range of DFMs, including porous organic polymers, covalent organic frameworks, zeolites, metal–organic frameworks, metal oxides, amines, ionic liquids, deep eutectic solvents, and molten salts. Mainstream CO2 capture technologies, post-, pre-, and oxy-fuel combustion routes, and associated separation techniques such as absorption, adsorption, membrane filtration, cryogenics, and looping cycles are systematically analyzed through a SWOT framework (strengths, weaknesses, opportunities, and threats) across efficiency, energy, cost, and technology readiness dimensions. By coupling techno-economic evaluation with emerging mechanistic and computational insights, this review identifies viable strategies to bridge the gap between laboratory innovation and industrial deployment. Finally, we outline key research priorities, including the rational design of DFMs, optimization of catalytic interfaces, and integration of AI-driven process control, positioning ICCC as an emerging pathway toward industrial decarbonization and the global clean energy transition, while highlighting fundamental constraints from coupled CO2 adsorption thermodynamics, transport, and catalytic kinetics that expose critical material-stability and system-integration challenges for large-scale deployment.
Broader contextCarbon dioxide (CO2) emissions are the primary driver of global climate change, yet CO2 also represents a vast, renewable carbon resource for producing sustainable fuels and chemicals. Conventional carbon capture and utilization approaches have advanced independently, but their separation limits overall efficiency, scalability, and economic viability. The emerging concept of integrated CO2 capture and conversion (ICCC) provides a unified route to simultaneously mitigate CO2 emissions and generate valuable products. By coupling CO2 adsorption and catalytic transformation within a single system, ICCC redefines how we think about carbon management, from end-of-pipe mitigation to circular resource utilization. This review provides a comprehensive framework linking materials design, catalysis, and process engineering to establish ICCC as a cornerstone of carbon circularity and industrial decarbonization, accelerating the transition toward a net-zero energy future. |
Carbon capture, utilization, and storage (CCUS) is widely regarded as a promising mitigation pathway.6 Furthermore, the International Energy Agency (IEA) Net Zero Emissions scenario necessitates scaling Carbon Capture, Utilization, and Storage (CCUS) capacity from approximately 45 Mt CO2 per year in 2022 to over 6.0 Gt CO2 per year by 2050, a more than 100-fold increase required to address heavy industry, power generation, and transport.7 However, conventional CCUS faces major hurdles: the processes of separation, compression, purification, and storage are highly energy-intensive, with prohibitive economic costs acting as a major barrier.8,9 Additional concerns include limited geological storage capacity, high monitoring costs, and public resistance due to risks of potential leakage.10
Integrated carbon capture and utilization (ICCU), also known as integrated carbon capture and conversion (ICCC),11 reactive capture of CO2 (RCC),12 and carbon capture and recycling (combined CCR),13 has emerged as a compelling alternative. ICCC eliminates the need for desorption, compression, transportation, and long-term storage by enabling direct CO2 conversion within absorbents, thereby reducing overall energy consumption and simultaneously lowering atmospheric CO2 concentrations (Fig. 1).14 These systems may take the form of integrated cascades or fully in situ single-pass processes.
In Aspen Plus–based syngas production TEA,15 ICCU demonstrated higher energy efficiency (37.1%) compared to CCU (35.4%) for Ca-looping capture coupled with reverse water–gas shift (RWGS) syngas production, reflecting reduced energy consumption per unit product. Comparative syngas TEA shows the total annual cost of ICCU is $867.07 million, corresponding to a total cost of CO of $720.25 per tonne. In contrast, CCU has higher costs, with a total annual cost of $1027.61 million and a total cost of CO of $1004.53 per tonne. Analysis also shows that the ICCU process can produce more CO (1.20 Mt year−1), less purge (0.21 Mt year−1), and less consumption of CaCO3 (0.62 Mt year−1). The Cost of CO2 Avoided of ICCU (317.11 $ per ton) is much lower than that of CCU (1230.27 $ per ton). Furthermore, in methanation applications, the integrated route requires only one-third of the energy input consumed by the decoupled CCU process, which translates into a 13% reduction in production costs, lowering the price of methane from 962.86 € per ton in the conventional scheme to 837.1 € per ton with ICCU.16
Nevertheless, realizing the full extent of these efficiency gains requires a level of process-material integration that is not yet adequately reflected in most existing reviews, which focus on either capture materials or conversion technologies separately. As a result, the current ICCC literature remains fragmented, with limited comprehensive evaluations that bridge material design, process integration, techno-economic analysis, and industrial scalability. Furthermore, there is insufficient comparative assessment of dual-functional materials (DFMs) with respect to structural stability, product selectivity, and durability under realistic flue-gas conditions. Therefore, this review addresses existing gaps by presenting a state-of-the-art analysis of the Integrated CO2 Capture and Conversion (ICCC) field, spanning fundamental materials science to process-level techno-economics. Advances in dual-function materials (DFMs) are surveyed, including solid sorbents such as porous organic polymers (POPs), covalent organic frameworks (COFs), metal–organic frameworks (MOFs), zeolites, and metal oxides, as well as liquid solvents such as amines, ionic liquids (ILs), deep eutectic solvents (DESs), and molten salts. In addition, the performance and technology readiness levels (TRLs) of major capture and separation technologies are evaluated, along with the definition of critical performance indicators and the identification of outstanding challenges. As illustrated in (Fig. 2), the workflow of this review provides a structured pathway that connects materials development with carbon capture technologies and separation techniques and further extends to system-level performance indicators and techno-economic assessment, ensuring comprehensive coverage from fundamentals to applications. However, integrating capture and conversion within a single workflow imposes stringent kinetic and thermodynamic constraints: materials must bind CO2 strongly enough for efficient capture yet release or activate it rapidly at catalytic sites, while mass transport and heat management must be compatible with high turnover frequencies under realistic flue-gas compositions. Therefore, this review places particular emphasis on how capture thermodynamics, diffusion limitations, reaction kinetics, and process synergies co-determine the performance window of integrated ICCC processes and dual-functional materials. Finally, a research roadmap is outlined to accelerate the transition of ICCC from laboratory-scale development to industrial deployment, complemented by a bibliometric analysis that maps development trends, research hotspots, and future directions.
![]() | ||
| Fig. 2 Schematic overview of the review workflow: materials advances, capture technologies, performance indicators, and techno-economics. | ||
| Industrial process | CO2 concentration in feed (vol%)19 | Main impurities (vol%)19 | Capture cost of CO2 (US$ per ton CO2)20 | Levelized cost of CCUS (US$ per ton CO2)21 |
|---|---|---|---|---|
| Power generation (coal-fired) | 12.6%–14% | 71.4%–74% N2, 8%–10.8% H2O, 3%–4.3% O2, trace SOx, H2S, NOx | 52–86 | 50–100 |
| Hydrogen plant (steam methane reforming) | 12% | 29% H2O, 50% H2, 1% CO | >50 | 50–80 |
| Cement industry | 19% | 61% N2, 13% H2O, 8% O2 | 62–94 | 60–120 |
| Steel industry (Blast furnace) | 20% | 56% N2, 21% CO, 3% H2 | >75 | 40–100 |
| Natural gas processing | 99%22 | 1% H2O22 | 14–20 | 15–25 |
| Ammonia production | 99%22 | 1% H2O22 | 1922 | 25–35 |
| Bioethanol (fermentation) | 100% | — | 3222 | 25–35 |
| Ethylene oxide (vented stream) | 100% | — | 2622 | 25–35 |
| Air (for reference) | 0.04% | 78% N2, 20% O2, 1% Ar | — | 134–342 |
While impurity tolerance is a key differentiator, the fundamental selection between thermocatalytic and electrocatalytic systems rests on their distinct operational requirements and capabilities. Thermocatalytic systems rely on high temperatures (100–500 °C) and elevated pressures (0.1–10 MPa) to drive reaction kinetics, requiring a supply of external molecular hydrogen (H2) and often hitting thermodynamic equilibrium ceilings that limit conversion efficiency; however, electrocatalytic approaches offer a compelling alternative by operating under mild, ambient conditions (<100 °C, <1 MPa).23 By utilizing renewable electricity and water as a direct proton source, electrocatalysis eliminates the need for energy-intensive hydrogen storage and transport and leverages applied overpotentials to overcome thermodynamic limits, unlocking superior selectivity for valuable multi-carbon (C2+) products like ethylene that are difficult to synthesize thermochemically. However, beyond CO2 concentration, the stability of ICCC materials is critically compromised by flue gas impurities, which trigger distinct poisoning mechanisms that must be accounted for in reactor design. First, sulfur oxides (SOx), being stronger acids than CO2, react irreversibly with basic active sites to form heat-stable salts (sulfates) that survive standard regeneration, leading to permanent pore plugging and progressive capacity decay.24 Second, nitrogen oxides (NOx) compete via stronger adsorption on Lewis's acid sites (metal oxides, zeolites) and accelerate sorbent degradation through nitration/reduction side reactions, reducing faradaic efficiency.25 Third, moisture exerts a dual negative effect: it competitively adsorbs on hydrophilic sites, hindering CO2 uptake, and promotes hydrothermal sintering of dispersed metal nanoparticles during the high-temperature conversion step, effectively deactivating the catalyst.26 Fourth, oxygen (O2) selectively oxidizes hydrogenation catalysts (e.g., Ru/Rh) and induces carbonate decomposition in solid DFMs.27
Regarding the impact of flue gas impurities on the direct electrochemical CO2 conversion, Pimlott et al. assessed this using a reactive carbon electrolyzer for electrocatalytic (bi)carbonate conversion.28 They found that flue gas containing sulfur oxides (SOx), and nitrogen oxides (NOx) exhibit markedly different impacts on the CO2 electrolysis: SOx have minimal impact on CO selectivity, whereas NOx drastically reduce faradaic efficiency (FECO), from ∼60% to <5% at 2000 ppm (Fig. 5a). Besides that, gas-fed CO2 electrolyzer exhibited a +90% reduction in CO selectivity with 10% oxygen (O2) in the feed while liquid-fed electrolyzer was unaffected, the same FECO of 65% at 100 mA cm2 at an O2-saturated feedstock and O2-depleted feedstock (Fig. 5b). Thus, both CO2 concentration and impurity composition must be considered when evaluating the economics and scalability of capture–conversion systems. Accordingly, the following sections will provide a detailed overview of state-of-the-art carbon capture technologies and separation techniques, followed by an in-depth analysis of the electrochemical conversion process.
| Carbon capture technology | Mechanism | Strengths | Weaknesses/threats | Opportunities |
|---|---|---|---|---|
| Post combustion | A process involves CO2 capture from gas streams produced after the combustion of fossil fuels or other carbonaceous materials | – Mature, retrofittable technology. | – Low CO2 concentration reduces efficiency | – Research into hybrid systems (e.g. membrane-pressure swing adsorption) |
| – Higher thermal efficiency vs. pre-combustion method. | – High flue gas temperatures and volumes cause design challenges | – Improving pulverized coal systems to reduce emissions | ||
| – Additional removal of NOx and SOx emissions | – Trace impurities such as NOx and SOx significantly affect the adsorption method | – Plant productivity enhancement | ||
| – Requires powerful chemical solvents to capture CO2 at low concentrations | ||||
| – Energy-intensive solvent regeneration | ||||
| Pre combustion | A process transformes fuels into a gasified state to separate the CO2 before burning the hydrogen-rich fuel like the SMR process | – 38–45% cheaper than post-combustion | – Heat transfer and efficiency issues due to the high temperature of H2-rich gas | – Research needed for high-value chemical feedstock production |
| – 50% less energy for CO2 separation than post-combustion due to high concentration and partial pressures | – Extensive supporting systems, such as an air separation unit and flue gas cooling | – Flexible hydrogen/electricity production | ||
| – Complex chemical processes lead to additional plant shutdowns | – Syngas as alternative turbine fuel | |||
| – Minimal regeneration energy | – Higher energy loss than post-combustion for reforming and air separation processes | |||
| – Low-cost physical solvents | – Requires special non-gaseous feedstocks and NOx control | |||
| Oxyfuel combustion | A process involves oxygen rather than air burns fuel to produce flue gas with high CO2 concentration | – 70–95% less expensive than other carbon capture methods due to lower flue gas volume and higher CO2 concentration | – Technology needs validation at a large scale | – Research needed for heat-resistant materials and oxygen separation beyond cryogenic distillation |
| – 60–70% less NOx emissions than air-fired combustion due to the absence of nitrogen | – Pure oxygen combustion challenges due to the high temperatures involved | – Improvements to reduce economic and efficiency penalties | ||
| – High-pressure operation reduces compression energy | – High capital expenditure and energy consumption costs due to the required larger amounts of oxygen, air separation, and flue gas recirculation costs | – Multiple fuel compatibility such as biomass and municipal solid waste for carbon neutrality | ||
| – Preserves high-efficiency steam cycles | – High risk of CO2 leakage | |||
| – Can be retrofitted into existing power plants |
![]() | ||
| Fig. 6 Process flow of major CO2 capture technologies, subsequent separation techniques, and the final pathways for either geological sequestration or industrial utilization. | ||
As shown in (Fig. 7),32,33 all three CO2 capture technologies achieve high capture removal efficiency, with post-combustion and pre-combustion at 90% and oxyfuel combustion at over 90%, but they differ in their techno-economic performance. The pre-combustion process exhibits the lowest energy consumption and the most competitive capture cost at 3.35 GJ t−1 CO2 and $34–63 per t CO2, respectively. In contrast, post-combustion is the least economically favorable, with the highest energy requirement of 4.14 GJ t−1 CO2 and a cost of $46–74 per t CO2. At a middle ground, oxyfuel Combustion occupies as high energy consumption as Post-Combustion at 4.05 GJ t−1 CO2 but its capture cost remains moderately lower at $52 per t CO2. Thus, this analysis indicates that, based on these metrics, the economic viability of the three carbon capture technologies falls in the sequence: pre-combustion > oxyfuel combustion > post-combustion, especially for high-pressure, high-CO2-concentration applications like IGCC and hydrogen production.
| Separation method | Mechanism | Strengths | Weaknesses/threats | Opportunities |
|---|---|---|---|---|
| Physical absorption | Absorption of CO2 in the solvent is governed by its solubility, as defined by Henry's law, with solubility varying in response to temperature and pressure changes like in materials of Selexol and Fluor | – Low energy needed for sorbent regeneration | – Limited operating temperature range; solvent capacity is optimized at lower temperatures to avoid any reduction in the solvent | – Potentially operating at lower temperatures than chemical methods, so less energy consumption and cost |
| – Low corrosivity and toxicity | – High capital and operational costs | |||
| – More cost-effective at higher CO2 partial pressures | ||||
| Chemical absorption | Upon interaction with the solvent, CO2 forms an intermediate through a reversible or irreversible chemical process, which subsequently breaks down, releasing CO2 upon heating like in materials of amines, ionic liquids, and Phase-change solvents | – Mature technology due to its high absorption capacities, such as amine absorption | – Higher water consumption | – Further advancements needed for amines and ionic liquids |
| – High product purity >99% vol. | – Exhaust gases (water, SOx, and NOx) need to be treated | |||
| – Well-suited for retrofit | – High regeneration energy costs | |||
| – Effective at low CO2 partial pressures | – Requires a large absorber volume | |||
| Adsorption | The flue gas flows over a solid sorbent, where CO2 is adsorbed, and other gases are allowed to pass, with the desorption of CO2 occurring through changes in temperature and pressure like in materials of zeolite, metal–organic, framework, activated carbon, and polymeric resins | – Flexibility in operating conditions with low-maintenance operation and Easy installation | – Sensitive to contaminants like sulfur, and nitrogen oxides, affecting their efficiency | – Advances in developing composite adsorbents to have cost-effective, reusable, and non-corrosive sorbents |
| – Regeneration occurs at lower temperatures, so less heat than absorption methods | – Poor adsorbent durability, resulting in additional costs for frequent material replacements | – A wide range of potential sorbent materials exist | ||
| – Waste biomass or industrial by-products can be used in adsorbent synthesis | – Challengeable to achieve the optimal operating temperature | – Dry gas products can be addressed | ||
| – The process is reversible through physical adsorption | ||||
| – Adsorbent can be recycled, hence low waste generation | ||||
| Membrane filtration | CO2 is separated from the main gas stream using a membrane that operates in two ways: the gas separation membrane, which exposes flue gas to the high-pressure side and separates CO2 on the low-pressure side, and the gas absorption microporous membrane, which enables both gas flow and absorption like in materials of graphene, organic, inorganic, and mixed matrix | – Simple, modular system design for easy adaptation | – Structural problems under high-pressure conditions lead to instability | – Advances in composite hollow-fiber membranes, mixed matrix membranes, and hybrid membrane-cryogenic processes |
| – No regeneration energy required, leading to lower costs | – Long-term performance degradation due to sensitivity to corrosive gases makes sustained operation challenging | – Low separation costs and minimal energy requirements might push this technology forward | ||
| – Higher energy efficiency compared to absorption and adsorption methods | – Moderate product purity | – Minimal footprint, making it ideal for offshore applications | ||
| – Zero waste by-products generated | – High commercial availability with efficient separation capabilities | |||
| – Continuous separation, offering efficiency over time | ||||
| Cryogenic separation | CO2 is separated from a gas mixture through consecutive refrigeration at different condensation temperatures, inducing phase changes only in carbon dioxide based on its dew point or sublimation like in materials of ceramic, glass, and aqueous | – Commercially proven and well-established technology | – Moisture removal is required from flue gas to prevent ice formation and equipment blockages | – High purity of the captured CO2 raises its economic value for various industrial uses |
| Easily integrated into power stations and other industrial point sources | – Energy-intensive due to the extreme cooling requirements, increasing operational costs | |||
| – Energy savings by reducing the need for compression | – Accumulation of solid CO2 reduces evaporator or heat exchanger efficiency over time | |||
| – No chemicals required for the process, making it simpler and more sustainable | ||||
| – Capable of filtering other pollutants, offering additional environmental benefits | ||||
| Chemical looping combustion | The combustion process is split into oxidation and reduction phases, each carried out separately, with a solid oxygen carrier being oxidized by air in the first phase and then reduced with a hydrocarbon in the second phase, producing CO2 and H2O | – Simple operation, with compatibility for low CO2 partial pressures | – Early-stage technology | – Exhaust gas from the air reactor is primarily nitrogen, with no harmful compounds |
| – The exhaust stream from the fuel reactor contains CO2 and water, where CO2 can be efficiently separated by condensation | – Fuel needs to be desulfurized to avoid metal sulfide formation | – No need for energy-heavy air separation, as the process yields high concentrations of CO2 | ||
| – The process relies on low-cost oxygen carriers | – Sensitivity to any air leakage | |||
| – Retrofitting the system is complex | ||||
| – Costly oxygen production | ||||
| Calcium looping combustion | CO2 is captured through reversible reactions between CaO and CO2, known as carbonation and calcination for the respective stages | – Cost-effective raw materials for sorbent synthesis | – Rapid decline in limestone (sorbent) capacity after several CO2 reaction cycles | – Offering a minimal decrease in power plant efficiency, with the potential for further reduction |
| – Ideal technique for retrofitting pulverized coal-fired power plants and enhancing sorption-based hydrogen production | – Environmental concerns relate to limestone mining, waste from Ca-looping, and high operational temperatures | |||
| – Need for an air separation unit to supply pure oxygen (O2) for calcination | ||||
| Electroswing | It operates by using a reversible electric current to either directly charge an electrode for CO2 adsorption or to manipulate a solution's pH, creating a chemical swing that captures and then releases the gas like in materials of quinones, ferrocenes, and carbon nanotubes | – Ambient operating conditions | – Technology readiness is still at the pilot stage | – Developing novel electrode materials to overcome current limitations, e.g., advanced redox-active organics and electrode designs |
| – Low cost due to the decreasing cost of renewable electricity | – Low current density due to their inability to operate at high current densities, limited to less than 5 mA cm−2 | – Further scaling and optimization are needed for commercialization | ||
| – High energy consumption and cost: to run at higher current densities results in large overpotentials, which lead to a higher energy demand and increase the capital cost |
As Fig. 8 illustrates, among the CO2 separation techniques, physical absorption stands out as the sole Tier 1 performer, demonstrating a high CO2 removal efficiency of 93%, coupled with low energy consumption (1.03 GJ per tCO2) and minimal capture cost (USD 12.38 per tCO2).36 In contrast, technologies such as chemical absorption (90%, ∼3 GJ per tCO2, USD 48.07 per tCO236), membrane filtration (up to 88%, ∼2 GJ per tCO2, USD 36.78 per tCO236), and calcium looping (89%, 2.8 GJ per tCO2, USD 32 per tCO237,38) fall under Tier 2, primarily due to their moderate energy demands and higher capture costs. Meanwhile, chemical looping combustion (96%, 0.95 GJ per tCO2, USD 59.2 per tCO233), cryogenic separation (95%, 3.8 GJ per tCO2, USD 55 per tCO239,40), and adsorption (90%, 4 GJ per tCO2, USD 47 per tCO239,40) are categorized as Tier 3, reflecting a trade-off wherein high capture efficiencies are accompanied by significant energy penalties and costs. It should be noted that all of these values represent averages, which may be influenced by various factors, including operating temperature and pressure, flue gas composition, properties of the capture agent, scale of deployment, and, most notably, the technology readiness level (TRL), which is addressed subsequently.
Among the various CO2 conversion techniques, electrochemical conversion has multiple advantages, including mild reaction conditions, potential synergy with renewable energy sources, high environmental compatibility, and controllable reaction rate and product selectivity by modulating the applied electrode potential; however, several challenges still need to be addressed such as high energy requirements, durability, environmental impacts and sustainability of certain conversion products, and high thermodynamic and kinetic barriers.17
After efficient capture and separation of CO2 gas, the CO2 undergoes electrochemical conversion to valuable carbon-based products such as carbon monoxide, ethylene, ethanol, and more through a multi-proton-coupled and multi-electron transfer process.52 Generally, the electrochemical CO2RR can be presented as
| xCO2 + n(H+ + e−) → product + yH2O |
Noting that the anodic reaction is the oxygen evolution reaction (OER) while the contemporaneous reduction of H+ is accompanied by the hydrogen evolution reaction (HER), which should be restricted during the electrolytic reduction of CO2 by considering the thermodynamics involved in the whole conversion process to get the desired product.53 Additionally, the electrocatalytic reduction of CO2 follows a three-part reaction mechanism: electron transfer, electrochemical reaction, and catalytic reaction.54
Initially, CO2 dissolved in the electrolyte gets in contact with the electrode, where it adsorbs onto the catalyst for activation. Secondly, the reduction of adsorbed CO2 occurs through proton-electron transfer on the catalyst surface, which breaks the C
O bond and requires about 750 kJ per mole as a thermodynamically uphill reaction, forming a new chemical bond (COOH*), where * denotes surface-bound species or vacant catalytically active sites. Subsequently, the reduction products are desorbed from the electrode and diffuse into the response medium, which depends not only on the stability but also on the reduction of COOH*, but also on the catalyst's capacity.
![]() | ||
| Fig. 10 Conceptual overview of the integrated CO2 capture and conversion (ICCC) process by using dual functional materials (DFMs). | ||
![]() | ||
| Fig. 11 A conceptual energy diagram contrasting the conventional, energy-intensive independent process versus the direct coupling 'integrated' approach of carbon capture and conversion. | ||
![]() | ||
| Fig. 12 A schematic of the two-step process involving carbon capture with a sorbent or solvent material, followed by carbon conversion into final products. | ||
In this context, this timely and thorough review paper summarizes the latest developments of the integrated process progress with an emphasis the following promising dual functional materials: adsorbents such as porous organic polymers (POPs), covalent organic frameworks (COFs), metal–organic frameworks (MOFs), zeolites and absorbents such as amines, ionic liquids, eutectics, and molten salts, the mechanism (Fig. 13).
![]() | ||
| Fig. 13 Examples of the dual-functional materials used in integrated processes, with emphasis on the adsorbents and absorbents highlighted in this review. | ||
| Materials | Structural features | Advantages | Disadvantages (technical) | Techno-economic barriers |
|---|---|---|---|---|
| POPs | 2D/3D covalent networks from organic polymerization | – Large SSA (up to 3000 m2 g−1) | – Poor microporosity (Vmicro <50%) | – High monomer cost ($50–200 per kg) |
| – Controllable functionality | – Oxidative degradation (+0.8 V) | – Solvothermal scale-up (ZnCl2, 400 °C) | ||
| – Tunable porosity | – Swelling in humid flue gas | – Poor recyclability (30% SSA loss/cycle) | ||
| – Good thermal stability (>400 °C) | ||||
| PCPs | Metal ions/clusters + organic linkers (crystalline) | – Ultra-high SSA (>7000 m2 g−1) | – Poor thermal stability (<300 °C) | – Metal salt cost ($100–500 per kg) |
| – Adjustable pore function | – Hydrolysis in humid flue gas | – Multi-step solvothermal (DMF, 120 °C) | ||
| – High CO2 capacity (10 mmol g−1) | – Metal leaching under bias | – Non-recyclable (framework collapse) | ||
| COFs | Crystalline covalent organic frameworks | – Large SSA (4210 m2 g−1) | – Poor crystallinity control | – High cost ($200–1000 per kg) |
| – Abundant active sites (N-doping) | – Hydrolysis (>50% loss @80% RH) | – Slow crystallization (days–weeks) | ||
| – Diverse synthesis routes | – Low conductivity | – Non-recyclable (irreversible hydrolysis) | ||
| N-polymers | Nitrogen-functional polymers (± metals) | – Simple preparation | – Poor conductivity (Rct >100 Ω) | – Large-scale mixing challenges |
| – Cost-efficient ($10–50 per kg) | – Mechanical instability | – Moderate recyclability (50% capacity loss) | ||
| – Adjustable pores | – Low SSA (<500 m2 g−1) | – Limited flue-gas tolerance |
N) is highly stable and the synthesis conditions are severe, the majority of reported CTFs are amorphous. However, crystalline CTFs with many highly ordered holes and periodic architecture provide substrate specificity and a better understanding of their basic properties. Recent developments in a range of CTF-based catalysts derived from task-specific nitrile monomers are compiled for CO2-involved catalytic processes, including CO2 cycloaddition, CO2 carboxylation, CO2 hydrogenation, CO2 photoreduction, and CO2 electroreduction. This review emphasizes the structural design and synthesis of common CTFs from a sustainable perspective, as well as the relationship between structure and properties in CO2 catalysis. Significant opportunities and strategies in this field are examined to develop precisely designed CTFs with superior CO2-catalytic capability.83
CTFs have a nitrogen-rich, electron-deficient structure with their inherent 1,3,5-triazine rings, which results in interesting heteroatom effects such as H-bonding, metal chelation, and π–π interactions. CTFs have an alkaline nature owing to the high nitrogen content, which makes them suitable for base-catalyzed organic reactions. The incorporation of stoichiometric, precisely defined coordination sites into triazine frameworks can enhance their capacity for metal ion complexation, while the meticulous integration of heteroatoms and other functional groups can further broaden their use. CTFs are commonly used as homogenous catalysts and as a pathway for stabilizing metal nanoparticles. They can also be used as precursors of nitrogen-doped porous carbon materials, which can be easily obtained after pyrolysis. The main classifications of CTFs as catalysts and support materials are: metal-free catalysts, supports for solid molecular catalysts, supports for nanoparticulate catalysts, and precursors of N-doped porous carbon materials. The initial method employs CTFs as a primary catalyst to activate CO2 via acid–base interactions; the second method utilizes CTFs as carriers for solid molecular catalysts; the third method involves CTFs as functionalized supports for the stabilization of metal nanoparticles with catalytically active species; and the fourth method utilizes CTFs as precursors for N-doped porous carbon materials through high-temperature pyrolysis.84,85
| CTF | Surface area (m2 g−1) | Pore volume (cm3 g−1) | Pore size (nm) | CO2 capacity (cm3 g−1@273 K) low pressure | Qst (kJ mol−1) | Ref. |
|---|---|---|---|---|---|---|
| CTF-CSU37@post | 488 | 0.39 | — | 29.0 | — | 93 |
| TAT-DHBD (1) | 750 | 0.36 | 2.61, 3.79 | 30.4 | 27.2 | 94 |
| TFM-1 (CH3SO3H) | 738 | — | — | 30.8 | 27.8 | 95 |
| PCBZL | 341 | 0.36 | — | 32.6 | 39.6 | 96 |
| PAF-1-6-2 | 979 | — | — | 42.2 | 30.3 | 97 |
| Zn@CTF | 598.2 | 0.35 | 0.53, 1.26 | 23.0 | 32.5 | 98 |
| CTF-CSU41 | 333 | 0.78 | — | 52.3 | 44.6 | 93 |
| PHCTF-4 | 1270 | 0.79 | — | 52.4 | 24.3 | 99 |
| PCTF-8 | 625 | 0.32 | — | 56.0 | 37.0 | 100 |
Kai Ao et al. (2024) investigate an interesting instance of exceptional Ni–N/CNT@CTF electrocatalyst, exhibiting a high %FE for the reduction of CO2 to CO. The catalyst was synthesized through the pyrolysis of residual nickel species within carbon nanotubes (CNTs), utilizing a soluble, π-conjugated CTF nanosheet as a nitrogen precursor and interfacial stabilizer. CTF's slender two-dimensional structure enables it to conform closely to carbon nanotubes, preserving their inherent curvature while preventing excessive graphitic overgrowth. High-resolution HRTEM, HAADF-STEM, and EDS mapping revealed the formation of atomically dispersed Ni–Nx sites (Fig. 17a). Electrochemical experiments demonstrated the catalyst's high performance: in H-type cells, it achieved a FE of 96% at −0.77 V vs. RHE, while in a flow-cell system, it exhibited a CO partial current density of 201 mA cm−2 at −0.9 V with 98% FE. The stability observed exceeded 10 hours in H-cells and 5 hours in flow systems. The Tafel slope analysis, measured at 56 mV dec−1, indicated that the rate-limiting step was the formation of COOH* (Fig. 17b–d). The identification of the Ni3 configuration as the primary active site through DFT calculations was significant. The curvature of the CNT induced compressive strain, resulting in shorter Ni–N bonds (1.83 Å compared to 1.84 Å in planar graphene), thereby enhancing the binding strength of *CO2 and *COOH. The alteration in structure rendered the reaction energetics more thermoneutral, thereby enhancing turnover efficiency.108
Feng et al.99 reported a family of MPTFs (M = Mn, Fe, Co, Ni, Cu), synthesized by iono-thermal trimerization of porphyrin units with incorporated metal centers (Fig. 18a). Among these, NiPTFs-600 exhibited outstanding catalytic performance as shown in (Fig. 18b and c), achieving a remarkable FE for CO production of 97.6% at −0.8 V vs. RHE, with a broad potential window (−0.55 to −0.95 V) where FE > 90% was maintained. The high performance was attributed to the abundant, homogeneously distributed Ni–Nx active sites (8.43 at% N content, 696 m2 g−1 surface area) that promote CO2 activation and protonation steps (*CO2 → *COOH → *CO) (Fig. 18d). NiPTFs-600 also demonstrated a high CO partial current density (10.8 mA cm−2 at −0.8 V) and stability over 10 hours with negligible structural degradation (Fig. 18e). Compared to other MPTFs, Ni-based frameworks showed superior kinetics (Tafel slope of 129.8 mV dec−1) and minimal charge transfer resistance (9.7 Ω), underscoring the key role of Ni–Nx sites in facilitating efficient CO2RR.109
Su et al.88 investigated the incorporation of coordinatively unsaturated 3d transition metals, such as Co and Ni, within CTFs, and how it will enhance the electrocatalytic CO2RR. M-CTFs were prepared by polymerization reaction of 2,6-dicyanopyridine and incorporating carbon black for conductivity, followed by metalation using MCl2 (M = Co, Ni, or Cu). The as-prepared M-CTFs are dispersed atomically within the microporous structure of the support. High-resolution XPS, and EXAFS analysis confirmed that these metal atoms were in a highly unsaturated coordination significantly different from the saturated planar geometry found in conventional tetraphenyl porphyrin (TPP) complexes. Notably, Ni-CTF exhibited a first-shell coordination number of approximately 3.4, lower than the tetra-coordinate Ni-TPP standard, indicating that Ni was stabilized within the CTF matrix in a catalytically advantageous unsaturated state (Fig. 19a–c). This structural tuning translated into a dramatic improvement in catalytic performance specifically for Ni-CTF achieve 90% FE for CO at −0.8 V vs. RHE which is shown in LSV measurement under CO2-saturated 0.5 M KHCO3 solution showed a marked increase in cathodic current, indicating active CO2 conversion (Fig. 19c and d). CO and H2 as the main products, with the Ni-CTF showing a CO
:
H2 ratio far superior to Co-CTF and Cu-CTF, which was confirmed by GC measurements. While for Ni-CTFs, a Tafel slope analysis revealed a value of ∼86 mV dec−1 for Ni-CTF, indicating a favorable kinetic profile consistent with COOH* formation as the rate-determining step. In addition to the electrocatalytic activity, the material also possessed high stability and durability across prolonged electrolysis sessions. The experimental outcomes are concise with the DFT calculations. These revealed that the free energy barrier for COOH* formation on Ni-CTF was significantly lower than on Ni-TPP (0.59 eV vs. 0.85 eV), due to both the reduced steric hindrance and the stronger electronic coupling between the unsaturated Ni centers and the π-conjugated triazine framework. Moreover, the adsorption energies of *CO and *COOH intermediates followed an optimal volcano-type relationship that aligned Ni-CTF near the top of the activity curve. This synergy between structural engineering and electronic optimization demonstrates how coordination in well-defined porous supports like CTFs can unlock new electrocatalytic pathways, particularly for metals like Ni that are traditionally inactive under standard configurations, as shown in (Fig. 19e and f).88
(Fig. 20) quantifies how ICCC integration reprograms CO2RR thermodynamics through co-adsorption: capture platforms (CTFs/MOFs) pre-concentrate flue-gas CO2 (ΔGads = −0.35 eV via N-quadrupole), eliminating mass-transport limits at 0.01–0.15 bar PCO2 and slashing the prohibitive *CO2 → *COOH barrier from 1.05 eV (conventional gas-phase, dashed red) to 0.45 eV (ICCC, solid blue), positioning the rate-determining step within the Sabatier volcano optimum (±0.2 eV) while suppressing competing HER (0.45 → 0.75 eV via pore-confined pH). This pathway bifurcation explains Ni-CTF's 90% FECO (0.59 eV *COOH barrier, 86 mV dec−1 Tafel), NiPor-CTF's 92.3% FECO at 12.8 mA cm−2 over 20 h (0.58 eV), and Cu/ICTF-50's C2H4 selectivity (35% FE, 4.14 mA cm−2 via 1.3 mmol g−1 adsorption boost), enabling >90% FE across −0.6 to −1.0 V directly from dilute feeds and transforming kinetic bottlenecks into thermoneutral pathways for industrial currents ≥200 mA cm−2.86,88,91,106,110
![]() | ||
| Fig. 20 Gibbs free energy profiles demonstrating capture-enhanced CO2RR in integrated carbon capture and conversion (ICCC). | ||
In a compelling demonstration of dual-function material design, Lu et al.91 reported a Ni-porphyrin-based covalent triazine framework (NiPor-CTF) that integrates atomically dispersed NiN4 centers into a nitrogen-rich, microporous polymeric matrix, offering both efficient CO2 capture and electrocatalytic CO2 conversion. Synthesized via an ionothermal method using ZnCl2 as both solvent and Lewis acid catalyst, NiPor-CTF was formed by trimerizing 5,10,15,20-tetrakis(4-cyanophenyl) porphyrin–nickel at 400 °C for 40 h (Fig. 21a). Structural characterization using XPS and EXAFS confirmed that Ni atoms were uniformly anchored in a square-planar NiN4 configuration, with no evidence of Ni nanoparticles or clusters (Fig. 21f). The Por-CTF exhibits higher adsorption capacity of CO2 uptake in comparison with NiPor-CTF as listed in (Table 6). However, the electrocatalytic activity is coming from Ni metal center. The higher adsorption capacity is attributed to BET surface area of 815 m2 g−1 and thus a CO2 uptake capacity of 2.4 mmol g−1 at 298 K, outperforming Ni/N-PC analogues. The NiPor-CTF showed superior electrochemical activity and selectivity of CO2 reduction into CO where the measurements in CO2-saturated 0.5 M KHCO3 electrolyte revealed a low onset potential of approximately 443 mV vs. RHE, with faradaic efficiencies exceeding 90% across a wide potential window (−0.6 to −0.9 V), peaking at 92.3% at −0.8 V, and delivering a corresponding current density of 12.8 mA cm−2. Compared with catalysts (Ni-free Por-CTF and Ni/N-PC), NiPor-CTF exhibited superior electrocatalytic performance, attributed to the dense population of NiN4 active sites and to efficient mass transport enabled by the porous network (Fig. 21b and c). In addition to the activity and selectivity, the catalysts exhibit Long-term durability, which was confirmed through chronoamperometric tests over 20 hours, showing negligible loss in current density or CO selectivity (Fig. 21d and e). The superior performance is also explained by DFT calculations (Fig. 21g and h). (Fig. 20) illustrates how CTF-localized CO2 adsorption (ΔGads = −0.4 eV via N-quadrupole) lowers the *CO2 → COOH barrier from 0.85 eV (Ni/N-PC, gas-phase CO2) to 0.58 eV (NiPor-CTF), while raising the competing HER barrier (H → H2) from 0.42 eV to 0.67 eV—achieving thermoneutral *COOH formation and suppressed H2 evolution. This pathway bifurcation positions NiPor-CTF at the volcano peak: *COOH ΔG = 0.12 eV (optimal range ±0.2 eV), versus Ni-TPP's over-stabilized *CO (ΔG = −0.45 eV, desorption limit). Similarly, Su et al. report Ni-CTF's unsaturated Ni3 coordination reduces *COOH barrier to 0.59 eV (vs. 0.85 eV Ni-TPP), with Tafel slope 86 mV dec−1 confirming fast *COOH formation. (Fig. 19) contrasts neutral CTF vs. Cu/ICTF-50: imidazolium cations enhance CO2 adsorption (1.3 mmol g−1 ↑ at 273 K), stabilizing *CO dimerization (ΔG = −0.22 eV) for C2H4 (35% FE, 4.14 mA cm−2) versus neutral CTF's *CO desorption pathway. These diagrams quantify how capture-modulated adsorption energies shift RDS from *CO2 activation (gas-phase) to *CO dimerization (integrated), enabling >90% FE across wide potential windows (−0.6 to −1.0 V).
| Sample | SBETa (m2 g−1) | Smicrob (m2 g−1) | VTotc (cm3 g−1) | Vmicrod (cm3 g−1) | Dave (nm) | CO2f [mmol g−1] | |
|---|---|---|---|---|---|---|---|
| 273 K | 298 K | ||||||
| a Specific surface area measured by BET model.b The microporous surface area analyzed by t-plot method.c The total pore volume measured at P/P0 = 0.99.d The microporous volume analyzed by t-plot method.e Average pore size.f CO2 physisorption data. | |||||||
| Por-CTF | 1099 | 113 | 1.77 | 0.13 | 6.5 | 6.7 | 2.5 |
| NiPor-CTF | 815 | 89 | 0.75 | 0.08 | 3.7 | 5.0 | 2.4 |
| Ni/N-PC | 959 | 94 | 0.95 | 0.11 | 4.0 | 3.9 | 1.6 |
Mao et al.111 recently reported a complex bifunctional electrocatalyst that incorporated copper nanoparticles (Cu/ICTF) and was prepared from imidazolium-functionalized cationic covalent triazine frameworks (ICTFs). The adsorption capacity is enhanced by the cationic nature of the imidazolium moieties, resulting in strong electrostatic interactions. During the reduction reaction the Cu–C bonds are formed as the imidazolium groups undergo additional in situ transformation into N-heterocyclic carbene (NHC) species (Fig. 22a). In addition to locally enriching CO2, this dual mechanism stabilizes the Cu NPs, avoiding agglomeration and guaranteeing sustained catalytic activity in comparison with neutral Cu/CTF, the Cu/ICTF-50 composite (containing 50 weight percent Cu) performed noticeably better. For 10 hours, Cu/ICTF-50 maintained a partial ethylene current density of 4.14 mA cm−2 and a C2H4 faradaic efficiency of 35% at −1.0 V vs. RHE in CO2-saturated 0.1 M KHCO3 electrolyte, which is noted to be better than Cu/CTF (Fig. 22c–e). From physicochemical characterization such as PXRD and Raman verified the ICTF's structural integrity, while TEM showed uniform Cu NP dispersion that enhances the CO2 adsorption and electroreduction. The adsorption capacity of CO2 by ICTF is confirmed from BET measurements, The imidazolium-induced adsorption enhancement was highlighted by CO2 adsorption isotherms (Micromeritics ASAP 2020), which showed a higher adsorption capacity than neutral CTF by 1.3 mmol g−1 at 273 K. Furthermore, Cu/ICTF exhibited decreased charge-transfer resistance in EIS measurements, indicating better electron transfer kinetics (Fig. 22b). Key reaction intermediates (*CO, *COH, and *CHO) were identified by operando FTIR spectroscopy, confirming a multistep mechanistic pathway that leads to the formation of C2H4.
Because of their appealing characteristics, such as enhanced π-conjugation and tunability, CMPs are attracting more attention as adaptable solutions for a variety of energy and environmental problems, including light harvesting, energy storage, adsorbents, heterogeneous catalysts, and luminous materials. One of the main benefits of CMPs is the variety of synthesis methods that are accessible.113 Several metal-catalyzed couplings to metal-free condensation processes can be used to create CMPs on a much bigger scale. Most processes used in the synthesis of COFs are reversible at high temperatures, which limits the choice of functional building blocks to those that can resist these harsh conditions. The primary difference between CMPs and COFs is their structural makeup; CMPs are more flexible in their design since they are amorphous, whereas COFs are crystalline. It is challenging to create multi-component CMP catalysts using COF materials, but this characteristic allows for the development of multi-step tandem reactions, expanding the design options.113,114 This modular framework architecture makes it possible to create hierarchical pore systems to improve transport kinetics and, in certain cases, well-accessible pores. Catalytic moieties may be directly integrated into the CMP framework to create heterogeneous CMP catalysts, which is a significant advancement in the utilization of CMPs for heterogeneous catalysis. Based on these fundamental ideas, it is quite possible to develop and synthesize CMPs with one or more active site types that will help collect and catalyze the conversion of CO2.115,116
| CMPs | SBET (m2 g−1) |
Smicro (m2 g−1) |
Vtot (cm3 g−1) |
Vmicro (cm3 g−1) |
Mcalc (wt%) | MICP (wt%) | CO2 uptake (mg g−1) |
|---|---|---|---|---|---|---|---|
| CMP | 772 | 283 | 1.21 | 0.117 | 0 | 0 | 71.0 |
| Co-CMP | 965 | 293 | 2.81 | 0.419 | 8.20 | 7.19 | 79.3 |
| Al-CMP | 798 | 315 | 1.41 | 0.298 | 4.01 | 3.46 | 76.5 |
592 h−1 at −0.65 V, along with a large current density exceeding 200 mA cm−2. Furthermore, the catalyst exhibited superior selectivity and stability compared to other related catalysts, maintaining high CO FE for at least 10 hours of continuous electrolysis, with only a marginal decrease in current density (Fig. 25b and c).
In the study of integrated CO2 capture and electrocatalytic conversion, Qui et al.120 introduces a new class of CPMs, with CMPANI-3 that acts as a promising catalytic material due to its exceptional design incorporating pyrazine-functionalized with cobalt porphyrin functions (Fig. 26a). The synergetic effect generated from cobalt embedded in the CPM structure with porphyrin function enhances both CO2 adsorption and catalytic performance. As detailed in (Table 8), CMPANI-3 exhibits the highest CO2 uptake capacity with 0.88 mmol g−1 at 273 K. This result is explained by the strong Lewis acid–base interactions between the electron-deficient pyridinyl nitrogen atoms and CO2 molecules. Additionally, the high porous structure of CPM is acquired with a surface area of 34 m2 g−1 to enhance the gas diffusion and adsorption capacity on the active sites. The electrocatalytic activity and selectivity of CMPANI-3, evaluated in a CO2-saturated 0.5 M KHCO3 electrolyte, reveals an outstanding FE (CO) of 97% at −0.7 V vs. RHE, with a corresponding partial current density more than 200 mA cm−2; moreover, a turnover frequency (TOF) of 2264 h−1 for CO, significantly surpassing its counterparts CMPANI-1 and CMPANI-2 (Fig. 26b–d). These improvements stem from the engineered coordination microenvironment around the CoN4 active site, where the pyrazine-N groups act as internal proton relays, effectively accelerating the proton-coupled electron transfer step critical for *COOH intermediate formation. This mechanism is clearly evidenced by in situ ATR-FTIR spectroscopy, which shows stronger and earlier formation of *COOH species in CMPANI-3, and KIE analysis that confirms enhanced proton transfer dynamics. Electrochemical analysis further supports this claim Tafel plots demonstrate the lowest slope (174 mV dec−1) for CMPANI-3, indicating faster kinetics, while Nyquist plots show it has the lowest charge transfer resistance (31.89 Ω), suggesting superior conductivity and reaction interface dynamics. Moreover, when integrated into a gas diffusion electrode and tested in a flow cell, CMPANI-3 maintains FECO above 90% even at 200 mA cm−2, reaching a TOF of 52
390 h−1, and thus rivals or surpasses leading CO2-to-CO catalysts including CoPc, Au–C, and Ag systems (Fig. 26e).
| Sample | SBETa (m2 g−1) | Vtotb (cm3 g−1) | Davc (nm) | CO2d (mmol g−1)@273 K | CO2d (mmol g−1)@298 K |
|---|---|---|---|---|---|
| a Specific surface area calculated using the BET equation.b Total pore volume at P/P0 = 0.99.c Average pore size.d Calculated from CO2 physisorption isotherms. | |||||
| CMPANI-1 | 12 | 0.09 | 2.2 | 0.46 | 0.38 |
| CMPANI-2 | 30 | 0.12 | 3.1 | 0.52 | 0.35 |
| CMPANI-3 | 34 | 0.26 | 2.7 | 0.88 | 0.66 |
Smith et al.121 investigated a novel metal–organic conjugated microporous polymer (CMP-(bpy)20-Mn) that has dual functionality for CO2 capture and electrocatalytic conversion (Fig. 27a and b). The material maintains substantial porosity after Mn incorporation with a surface area of 549 m2 g−1 and achieves moderate CO2 uptake of 1.06 mmol g−1 at 298 K and 1 bar, though this capture performance remains below benchmark materials like BPL carbon (Fig. 27c). Most notably, the rigid CMP structure prevents the problematic reductive dimerization of the [Mn(bpy)(CO)3Br] catalyst that typically occurs in solution-based systems, enabling direct formation of the catalytically active [Mn(bpyCMP)(CO)3]− species as evidenced by a single reduction peak at −1.35 V (Fig. 27d). The material is affected by two catalytic pathways: a slow pathway (−1.2 to −1.4 V) showing modest current enhancement with CO2 binding, and a fast substrate-limited pathway (−1.6 to −1.8 V) with scan-rate dependent behavior indicating higher TOF. Bulk electrolysis at −1.6 V demonstrates selective CO production as the sole carbon-based product with a 7-fold enhancement over the catalyst-free control and an estimated turnover number of ∼1296 over 4 hours, though the faradaic efficiency remains low at 0.43% due to competing hydrogen evolution (Fig. 27e). More examples of CMP-based electrocatalysts for ECO2RR are summarized in (Table 9) while comparative analysis of various POPs for CO2 capture and electrocatalytic conversion are detailed in (Table 10).
| Polymeric material | BET [m2 g−1] | Electrolyte | Applied potential [V] | Main product [FE%] | Ref. |
|---|---|---|---|---|---|
| PF-5 film | 1000 | 0.1 M Et4NBF4/acetonitrile solution | n.r. | CO | 122 |
| PyPOP@G | 582.7 | 0.1 M KHCO3 | −1.0 (vs. RHE) | n.r. | 123 |
| CMP-(bpy)20-Mn | 549 | 0.06 M Phosphate buffer | −1.6 (vs. Ag/Ag+) | CO (0.43%) | 124 |
| CNS-NiSA | 458 | 0.5 M KHCO3 | −0.8 (vs. RHE) | CO (95%) | 118 |
| CNT@CMP (CoPc-H2Pc) | 70 | 0.5 M KHCO3 | −0.9 (vs. RHE) | CO (97%) | 125 |
| COP-SA | 106.33 | 0.5 M KHCO3 | −0.65 (vs. RHE) | CO (96.5%) | 125 |
| Pt/TPE-CMP | 360 | 0.5 M KHCO3 | −1.5 (vs. Ag/Ag+) | (C1–C8) (>95%) | 126 |
| CoPPc-TFPPy-CP | 464.9 | 0.1 M KCl | −1 (vs. RHE) | C2H5OH 43.25% | 127 |
| −1.2 (vs. RHE) | HCOOH 13.91% | ||||
| BNPI-1 (NaF 0.99) | 54 | 0.1 M KHCO3 | 0.03 (vs. RHE) −0.26 | HCOOH 91% | 128 |
| BNPI-1 (NaI 0.66) | 728 | −0.26 (vs. RHE) | CH3OH 85% | ||
| BNPI-2 | 26 | −0.26 (vs. RHE) | HCOOH 45% | ||
| CH3OH 67% | |||||
| pPI-1 | 20 | 0.1 M KHCO3 | −0.76 (vs. RHE) | HCOOH 14% | 129 |
| −0.26 (vs. RHE) | CH3OH 52% | ||||
| pPI-2 | 342 | −0.56 (vs. RHE) | HCOOH 20% | ||
| −0.26 (vs. RHE) | CH3OH 95% |
| Catalyst | Synthesis method | Surface area (m2 g−1) | Faradaic efficiency (FE%) | Reduction products | CO2 uptake (mmol g−1) | Ref. |
|---|---|---|---|---|---|---|
| TTF-1 | Triazine linkage polymerization | 1234 | 82% at −0.6 V vs. RHE | CO, HCOOH | 2.86 | 63 |
| POP-Py(0)/CoTCPP | Benzyl bromide & pyridine reaction | Not specified | 83% at −0.6 V vs. RHE | CO | Not specified | 63 |
| PyPOP@G | Pyrimidine-based polymer on graphene | Not specified | 85% at −0.7 V vs. RHE | CO, CH4 | Not specified | 63 |
| POP@MWCNT | Polymerization on multi-walled CNTs | Not specified | 80% at −0.75 V vs. RHE | CO, HCOOH | Not specified | 63 |
| Bi-MOF | Solvo-thermal | Not specified | 92% at −0.9 V vs. RHE | COOH | 1.50 | 63 |
| FePC-POP | Friedel–Crafts alkylation | 427 | 88% at −0.65 V vs. RHE | CO | 1.50 | 130 |
| DTTBQ-CMP | Polycondensation | Not specified | 92% at −0.8 V vs. RHE | CO, C2H4O | Not specified | 130 |
| BSPOP-Co | Triptycene-based polycondensation | 280 | 87% at −0.7 V vs. RHE | CO | 1.70 | 130 |
| CuPcF8-CoNPc-COF | Condensation of phthalocyanine derivatives | 452 | 97% at −0.62 V vs. RHE | CO, CH4 | 0.80 | 131 |
| 2D-Co-COF500 | COF formation on Mg/Al-LDH | 123 | 96.5% at −0.8 V vs. RHE | CO | Not specified | 131 |
| f 2D cobalt(II)-phthalocyanine based COFs | Triazine-based framework | Not specified | 87% at −0.6 V vs. RHE | CO | Not specified | 131 |
| isox-CTF-500 | Triazine-based framework | 1683 | 90% at −0.75 V vs. RHE | CO, CH3OH | 4.92 | 131 |
| acac-CTF-500 | Triazine-based framework | 1556 | 85% at −0.6 V vs. RHE | CO, HCOOH | 3.30 | 131 |
| cCTFs-400 | Triazine-based framework | 744 | 89% at −0.65 V vs. RHE | CO, CH4 | 2.86 | 131 |
| cCTFs-450 | Triazine-based framework | 861 | 91% at −0.7 V vs. RHE | CO, C2H4 | 2.25 | 131 |
| cCTFs-500 | Triazine-based framework | 1247 | 95% at −0.75 V vs. RHE | CO, CH3OH | 3.02 | 131 |
| LKK-CMP-1 | 1,3-Dialkyne linkage polymerization | 467 | 86% at −0.7 V vs. RHE | CO, CH4 | 2.24 | 132 |
| 6FA-PEPH-CL | Crosslinked polyimide | 653 | 82% at −0.6 V vs. RHE | CO, HCOOH | 1.65 | 63 |
| 6FA-PE-CL | Crosslinked polyimide | 698 | 88% at −0.65 V vs. RHE | CO, CH3OH | 2.02 | 63 |
| Tt-POP-2 | Triptycene-based polymerization | 368 | 85% at −0.7 V vs. RHE | CO, CH4 | 0.40 | 133 |
| Tt-POP-3 | Triptycene-based polymerization | 974 | 90% at −0.75 V vs. RHE | CO, C2H4O | 0.62 | 133 |
The π-conjugation and microporosity of CMPs give them enormous interior surface areas up to 556 m2 g−1 BET and excellent CO2 adsorption capabilities, usually more than 1 mmol g−1 at room temperature. Adding different electron-rich parts, such as triazine, pyrrole, and thiophene, through modular synthesis processes can change the structure of the pores and how well they absorb CO2.77,96,136 CMPs, like CTFs, are very thermally stable, with decomposition temperatures often over 300 °C. They can also be chemically modified to add catalytic centers that help CO2 reduction into products like CO, formate, or methane. While the CTFs and CMPs are good for capturing and CO2 reduction owing to their excellent properties such as tunable pore size distribution and can be designed at the molecular level to maximize adsorption and catalytic activity. However, it is still hard to control crystalline and active site dispersion precisely. For example, CTFs often have low crystallinity under iono-thermal conditions, and the uneven pore distribution in CMPs can make it harder to predict how easily sorption or catalytic sites can be accessed.77,96,136 Moreover, research is also needed on scalability and long-term operating stability under electrochemical circumstances. Future goals include making greener, more scalable syntheses, enhancing structural order (to come closer to single-crystalline domains in CTFs), and using hybridization with conductive support or targeted functionalization like site-specific metalation or heteroatom doping. The combination of computational design and systematic structure–property studies is expected to accelerate the development of next-generation POPs with finely tuned performance for capturing CO2 and converting it efficiently via electrocatalysis, which directly help technologies that fight climate change.77,98,135
The primary synthetic methods for COFs include solvothermal synthesis, iono-thermal synthesis, mechanochemical synthesis, and microwave-assisted synthesis (Fig. 29).143–145 COFs can be modified with metal centers or functional groups to enhance CO2 adsorption, leading to the conversion of CO2 into valuable products, such as CO, methane, or ethylene.137,138,146 Also, as the majority of COFs are produced through cross-coupling or condensation reactions involving organic aromatic building blocks and linkers, the entire framework.144,147–149
In the first step, CO2 is adsorbed through physisorption, characterized by weak van der Waals forces, without a change in the electronic structure of COFs.144,152 Chemisorption, on the other hand, involves the formation of chemical bonds between CO2 and the functional groups present in the COFs. This process may result in more stable adsorption; however, it could necessitate increased energy for desorption.150 Regarding Functional groups, such as amines and imides, they play a crucial role in enhancing CO2 adsorption. These groups can interact with CO2 through hydrogen bonding or coordinate covalent bonding, significantly increasing the adsorption capacity. The existence of nitrogen-rich sites is especially advantageous, as they can provide additional binding sites for CO2, thereby enhancing the overall effectiveness of the COF in CO2 capture. Han et al. demonstrate that the two-dimensional polyimide-linked phthalocyanine COFs (CoPc-PI-COF-1 and CoPc-PI-COF-2) exhibit similar nitrogen-rich sites that facilitate effective CO2 capture, demonstrating the importance of these functional groups in the adsorption process.148 The other crucial factor, the pore size and topology of COFs, determines their CO2 adsorption performance. Larger pore sizes enhance the accessibility of CO2 molecules, allowing for greater adsorption. Additionally, the specific arrangement of the pores can influence the diffusion of CO2, affecting the overall efficiency of the adsorption process.147
The outstanding CO2 adsorption properties of COFs naturally correspond to their structure–property relationships. The π-stacking between layers makes the structure more rigid, allowing guests and hosts to interact more easily due to induced dipole and quadrupolar interactions, particularly in reactions, given CO2's linear geometry and quadrupole moment. The formation of COFs relies on dynamic covalent chemistry, which enables reversible reactions (such as imine condensation and boronate ester formation) that allow self-correction during synthesis. To successfully design COFs for CO2 capture, three key elements are required:137 (1) the selection of building blocks (such as triazine, benzene, or porphyrin cores) that dictate functionality and binding affinity toward CO2, (2) the geometrical integrity of the framework to ensure periodicity and stable pore architectures, and (3) reversible covalent bond formation, which is important for crystallinity, recyclability, and defect healing. Three primary factors determine how COFs capture CO2:143 the kind of linkage between the building units, the porosity type, and the types of COF building blocks. In this section, the main properties of COFs’ effectiveness in CO2 capture and conversion will be discussed: the dimensionality effect, the types of covalent bonds, the textural properties effect, and the functional groups and active sites effect.
The dimensionality of COFs significantly influences their porosity, gas diffusion properties, and adsorption capacity. 1D COFs are primarily non-centrosymmetric linear crystalline polymers formed by the haphazard packing of organic chains caused by entropy.139 These chains consist of 1D COFs, confined covalent bonds, and non-covalent interactions such as hydrogen bonding and π–π interactions. Singh and Nagaraja156 developed SO3H-functionalized 1D-COFs with polar channels to improve adsorption. Two-dimensional COFs are composed of planar building blocks that stack via π–π interactions, resulting in layered crystalline structures.157 These frameworks are effective platforms for CO2 capture because they typically have large surface areas, accessible channels, and well-organized micropores. For example, Gao et al.158 developed TPE-COF-II, a 2D COF with a frustrated bonding network resulting from an unusual [2+4] condensation pathway. The CO2 uptake capacity of 23.2 weight percent (118.8 cm3 g−1 at 273 K and 1 atm) is among the highest reported for 2D COFs due to its open pores and unreacted functional groups that enhance host–guest interactions.
In contrast, three-dimensional COFs (3D COFs) have longer, more interconnected networks with more internal voids and structural rigidity, resulting in better CO2 adsorption capacities than their two-dimensional counterparts.159,160 For instance, Zhu et al.161 developed a family of crystalline 3D COFs (RICE-3 to RICE-7) made from logically constructed trigonal and rectangular-planar linkers to demonstrate the structural advantages of 3D COFs over 2D counterparts. To illustrate, (Fig. 30a–f), shows how these linkers form interconnected polyhedral cages with hierarchical porosity and long-range order. The remarkable CO2 uptake performance of ∼50 cm3 g−1 at 273 K and 1 bar made RICE-5 stand out due to its large mesopore aperture (∼4.6 nm), high porosity (∼94.2%), and exceptionally low framework density (∼0.094 g cm−3). RICE-3 and RICE-7 visualizations (Fig. 30g and h), show how pore size distribution affects gas adsorption. RICE-7 is more microporous (1.0 nm), resulting in lower uptake, whereas RICE-3 has larger mesopores and wider inter-channel windows, which promote better diffusion. The 3D COFs featuring hierarchical and interconnected pores, such as RICE-5, exhibit enhanced adsorption capacities due to improved accessibility, effective packing, and diminished diffusion resistance, as evidenced by the CO2 isotherms (Fig. 30i and j). The findings underscore the significant influence of topology and dimensionality in 3D frameworks on the advancement of COF-based greenhouse gas capture technologies.
Covalent bonds can be classified as follows: ether bonds (–C–O–C–), thioether (–C–S–C–), hydrazone bonds (–C
N–NH2), azine bonds (–C
N–), boronate ester bonds (–B(OR)–O–), imine bonds (–C
N–), and triazine bonds (–C3N3–).162,163 Noting that, Amine bonds (N-based) and boronate ester bonds (B-based) are widely used in CO2 capture and conversion processes because of their ability to interact with CO2 via Lewis' acid–base interaction. Also, COFs with reversible imine linkages (–C
N–) can adsorb and release CO2 molecules under various conditions, including temperature, pressure, and gas composition changes.164 CO2 adsorption can cause Imine-linked COFs to expand structurally, leading to increased capacity for storage. Additionally, Imine bonds improve the catalytic potential of COFs for CO2 conversion by facilitating coordination and promoting reaction pathways. A notable example is the 3D-Ru-COF, which is composed of tetrakis (4-aminophenyl) methane (TAPM) and N-functionalized [2,2′-bipyridine]-5,5′-dicarbaldehyde (BPDCA). Kumar et al.165 demonstrated that THF-assisted solvent treatment increased CO2 uptake by 21% by causing flexible “pedal motion” in imine linkages (from 3.94 to 4.76 mmol g−1 at 273 K). Imine-linked 3D COFs exhibit dynamic and reusable properties in gas capture and catalytic applications, as evidenced by their structural modulation stability over seven consecutive adsorption–desorption cycles.
Increased CO2 uptake is correlated with higher surface areas (e.g., >3000 m2 g−1), which are determined by textural properties such as surface area, pore volume, and pore size distribution.166 Yaghi et al.153 developed 3D covalent organic frameworks (COFs) like COF-102 and COF-103 using a rational topological approach that combines tetrahedral (e.g., TBPM, TBPS) and trigonal (e.g., HHTP) building blocks via boroxine or boronate ester linkages (Fig. 31). These configurations yield highly crystalline and porous frameworks with ctn and bor net topologies. The precise reticular design creates ultrahigh surface areas of 3472 m2 g−1 for COF-102 and 4210 m2 g−1 for COF-103, resulting in exceptional CO2 uptake capacities of up to 27 mmol g−1 at 298 K and 1 bar, respectively. Also, Alahakoon et al.167 developed an azine-linked COF (HEX-COF-1) with a BET surface area of 1214 m2 g−1 and a narrow pore size distribution of ∼1 nm. With an enthalpy of adsorption of 42 kJ mol−1 and a relatively moderate surface area, HEX-COF-1 showed a high uptake of CO2 of over 20 weight percent at 273 K, indicating strong quadrupolar interactions between CO2 and the polar framework.
The inclusion of functional groups and active sites, such as –SO3H, –NH2, triazine, or metal centers, improves CO2-framework interactions through polar binding or catalytic activation.168 Functionalization strategies, whether post-synthetic or through direct monomer design, allow for modification of the chemical environment, adsorption strength, and selectivity.169 Wei et al.168 conducted a thorough study on several 3D COF-300 derivatives featuring –SO3H, –NO2, –OH, and –NH2 groups to investigate their ability to capture CO2. While selectively changing the chemical environment inside the pores, these COFs were derived from a common parent framework (COF-300-THF) and retained the same underlying topology (Fig. 32a), the addition of polar functional groups considerably altered the behavior of CO2 uptake. As illustrated in (Fig. 32b), COF-300-SO3H nearly five times outperformed the unmodified COF-300-THF in terms of adsorption capacity, reaching a maximum of 6.23 mmol g−1 at 298 K and 100 kPa. The strong hydrogen-bonding and electrostatic interactions facilitated by the sulfonic acid groups, which serve as high-affinity binding sites, are responsible for this improvement. The nitro-functionalized framework (COF-300-NO2) also showed high uptake (∼4.8 mmol g−1), whereas substitutions with –OH and –NH2 produced moderate improvements over the parent material. Significant gains in CO2/N2 selectivity resulted from the N2 adsorption isotherms (Fig. 32c), which showed little uptake across all COFs, especially in the more polar variants. This effect is shown in (Fig. 32d), selectivity of (∼393) for COF-300-SO3H was significantly higher than that of COF-300-NO2 (∼31), COF-300-OH (∼11), and COF-300-NH2 (∼10), demonstrating the crucial role that electronegativity and functional group polarity play in gas separation performance. Radial distribution function (RDF) analyses and CO2 density distribution maps provided additional mechanistic insights. CO2 molecules were found to preferentially localize close to the functional groups at both low (10 kPa) and high (100 kPa) pressures, particularly in COF-300-SO3H and COF-300-NO2. This pattern is supported by the RDF plots, which show that the NO2 group also exhibited favorable interaction behavior. In contrast, the SO3H–CO2 interaction displays the shortest and most intense peak (∼2.5 Å), indicating strong binding affinity. The distributions of NH2 and OH groups, on the other hand, were wider and less intense. This is consistent with their lower selectivity and weaker binding.
The successful outcome of CO2 reduction can be significantly enhanced by incorporating transition metals, alkaline-earth metals, and single-atom sites into organic or carbon-based frameworks, as numerous studies have demonstrated. For instance, Wu et al.173 reported that single-atom Mg and Ca attached to nitrogen-doped carbon exhibited outstanding selectivity for formate production at near-zero overpotentials by favoring *OCHO intermediate formation. Dagnaw et al.174 demonstrated a unique molecularly cationic covalent organic frameworks that incorporate transition metals (Cu and Pd) as active sites for the extremely selective electrochemical reduction of CO2 into CO. They synthesized two COFs, CuCOF and CuCOF+, by coordinating Cu(I)-bisphenanthroline complexes with terpyridine-based organic linkers. CuCOF+ was further modified with ethyl groups to improve its positive surface charge and hydrophilicity, which ultimately promoted CO2 accessibility and inhibited the HER side reaction. The COFs displayed a distinctive, three-dimensional woven framework (Fig. 33). The resulting CuCOF-Pd and CuCOF+-Pd catalysts showed significant increases in faradaic efficiency after loading Pd nanoparticles (NPs) into the pores of CuCOF and CuCOF+. For CuCOF+-Pd, the selectivity of CO reached up to 95.45% at −0.8 V vs. RHE.
Additionally, catalytic activity and electron transport efficiency in CO2 reduction systems can be improved simultaneously by combining metal active centers and conductive structural units in a single framework. For instance, Zhu et al.175 designed a series of metalloporphyrin–tetrathiafulvalene-based covalent organic frameworks (M-TTCOFs) that provide a convincing example of how combining metal active centers and conductive structural units within a single framework can simultaneously enhance catalytic activity and electron transport efficiency in CO2 reduction systems. The M-TTCOFs were produced by Schiff-base condensation between 4-formyl-TTF and M-TAPP (where M = Co or Ni), as shown in (Fig. 34a). This resulted in 2D layered structures with a unique porous structure and π-conjugated frameworks. The embedded metalloporphyrin moieties (such as Co or Ni) act as catalytically active sites in this system. While tetrathiafulvalene (TTF) acts as a highly conjugated electron donor, creating direct charge-transport pathways. This building improves the accessibility of redox-active centers and facilitates effective charge migration throughout the framework. As shown in the LSV curves (Fig. 34b) and FECO profile (Fig. 34c), the Co-TTCOF exhibited the highest catalytic activity, maintaining over 90% selectivity within a wide potential range (−0.6 to −0.9 V) and achieving a faradaic efficiency for CO (FECO) of 91.3% at −0.7 V vs. RHE. After exfoliation into nanosheets (∼5 nm thick), the FECO further increased to a maximum of 99.7% at −0.8 V, among the highest reported for COF-based electrocatalysts.
| Catalysts | Pore size (Å) | Dimensional | Linkage type | BET surface area (m2 g−1) | Capacity CO2 (mg g−1) | Electrochemical application | Electrochemical TOF or selectivity | Ref. |
|---|---|---|---|---|---|---|---|---|
| TFPc-PBBA-COF | 22 | 3D | Boronate Ester | 111.8 | 16.7 | CO2RR | Selectivity for CO 95% | 177 |
| TOF = 1695 h−1 | ||||||||
| CoPc-PI-COF-1 | 16 | 2D | Imine (polyimide) | 181 | 38.52 | CO2RR | Selectivity for CO 97% | 148 |
| TOF = 2.2 s−1 | ||||||||
TON = 277 000 |
||||||||
| CoPc-PI-COF-2 | 18 | 2D | Imine (polyimide) | 291 | 37.78 | CO2RR | Selectivity for CO 96% | 148 |
| TOF = 1.9 s−1 | ||||||||
TON = 71 000 |
||||||||
| CoPor-DPP-COF | 20.08 | 2D | Imine | 1021 | 3.72 | CO2RR | Selectivity for CO 82% | 178 |
| Cu-Tph-COF-Dct | 12–18 | 2D | Imine (Porphyrin-based) | 335 | 120.4 | CO2RR | Selectivity for CH4 80% | 179 |
| COF-102 | 12 | 3D | Boronated Ester | 3620 | 1200 | CO2 storage | N/A | 166 |
| COF-103 | 12 | 3D | Boronate Ester | 3530 | 1190 | CO2 storage | N/A | 166 |
| (3D-HNU5) | 10 | 3D | Azine | 864 | 123.1 | Cyclic carbonate synthesis | TON = 990, Yield > 99% | 180 |
| Tz-COF | 21 | 2D | Imine | 1439 | 154 | Gas separation | Higher CO2 selectivity than N2 (20/12) | 181 |
| Cz-COF | 20 | 2D | Imine | 871 | 110 | Gas storage & separation | Good recyclability and selectivity | 181 |
| Zn-Salen-COF-SDU113 | 35 | 2D | Imine | 1143 | 19.8 | Cycloaddition with epoxides to carbonates | Yield = 98.2%, | 182 |
| TON = 3068.9 | ||||||||
| Cu-COF+ | 28 | 2D | Imine (Cationic, ethyl-modified) | 27.6 | 13.7 | CO2RR | Selectivity for CO 57.81% | 174 |
| Cu-COF+-Pd | 28 | 2D | Imine (Cationic + Pd) | 4.1 | 8.4 | CO2RR | Selectivity for CO 95.45% | 174 |
| PA-Co-COF | 16.9 | 2D | Imine | 689 | 102.9 | CO2RR from the flow gas | Selectivity for CO 86.97% | 176 |
| TOF = 1208.8 h−1 | ||||||||
| Co-TTCOF | 25.4 | 2D | Imine (porphyrin + TTF) | 486 | 39.3 | CO2RR | Selectivity for CO 99.7% | 175 |
| TOF = 1.28 s−1 | ||||||||
| COF-367-Co (1%) | 12–23 | 2D | Imine | 1470 | N/A | CO2RR | Selectivity for CO 40% | 172 |
| TOF = 764 h−1 | ||||||||
TON > 24 000 (TONEA ≈ 296 000) |
||||||||
| COF-367-Co | 12–23 | 2D | Imine | 1470 | N/A | CO2RR | Selectivity for CO 91% | 172 |
| TOF = 165 h−1 | ||||||||
| TON = 3901 | ||||||||
(TONEA ≈ 48 000) |
Zeolite is characterized by microporous structure (less than 2 nm) that is organized by TO4 tetrahedra, where (T stands for tetrahedrally coordinated Si or Al).187–189 Molecular shape selectivity, a large surface area, and great thermal stability are some of the wonderful properties of zeolite that make it a great host matrix for metal clusters or nanoparticles.190,191 This makes multipurpose composite materials with great properties owing to these characteristics, it offers a catalytic site for the conversion of the intermediate produced by CO2 activation in the active metal site to generate hydrocarbons from CO2.192,193 Therefore, it would be possible to manipulate the zeolite catalyst's structural or textural characteristics to arrange the hydrocarbon goal yield.190,194
During the process of CO2-integrated collection and conversion, zeolites can perform the functions of both adsorbents and catalysts.195 The microporous structure of these materials allows them to selectively adsorb carbon monoxide (CO). Because they are catalytic, CO can be changed into compounds with added value, like methanol, hydrocarbons, or syngas.193 Metal-loaded zeolites, such as those containing nickel, copper, or iron, enhance catalytic performance by enabling the electrochemical reduction or hydrogenation of carbon dioxide. When it comes to structural qualities, product selectivity was found to have a significant relationship between the arrangement of the perfect acid density and the strength of the zeolite catalyst.196
Zeolites can be sub-grouped into natural and synthetic. On the one hand, natural zeolites such as ZAPS can be used as dryers and deodorants for air separation and ion exchange for water treatment and soil improvement (Fig. 37). On the other hand, synthetics such as FAU have advantages over natural ones, such as achieving high control over the material's porosity and crystallinity, but they are more expensive compared to affordable natural zeolites. Despite the lower cost of natural zeolites, they have reduced purity, varying composition, and inferior sorption properties.197,198
| Gases | Kinetic diameter (Å) | Quadrupole (C m−2) | Polarizability (cm3) |
|---|---|---|---|
| CO2 | 3.30 | 13.4 × 10−40 | 2.65 × 10−24 |
| N2 | 3.64 | 4.6 × 10−40 | 1.76 × 10−24 |
| O2 | 3.50 | — | 1.58 × 10−24 |
| CH4 | 3.80 | 0 | 2.60 × 10−24 |
Equilibrium separation depends on how the guest molecules and the zeolite micropores interact with each other.204 These interactions could be physisorption (which involves van der Waals forces and electrostatic interactions) and chemisorption (which involves π-complexation).205,206 What affects the electric charge exchange between gas molecules and zeolite surfaces are the polarity, polarizability, Si/Al ratios, and the types of metal cations. Kinetic separation relies on the different speeds at which guest molecules move through the tiny holes in zeolite.207 Kinetic separation is limited by molecular sieving, which needs zeolite micropores that are big enough to let CO2 through, but not any other exhaust gases.199,208
A compelling example of a zeolite-based material for CO2 capture is the hierarchical ZIF-L nanostructure reported by Ding et al. In this study, the authors synthesized a cross-shaped hierarchical ZIF-L using a simple hydrothermal method involving zinc nitrate and 2-methylimidazole at 125 °C. This hierarchical structure, composed of symmetrically connected ZIF-L leaf-like plates, exhibited a significantly enhanced Brunauer–Emmett–Teller (BET) surface area of 304 m2 g−1 compared to 161 m2 g−1 for conventional two-dimensional ZIF-L. As a result, the CO2 adsorption capacity reached 1.56 mmol g−1 at 298 K and 1 bar, outperforming both the 2D ZIF-L (0.94 mmol g−1) and even ZIF-8 (0.68 mmol g−1), despite ZIF-8 having a much higher surface area. This superior performance is attributed to the unique cushion-shaped cavities of ZIF-L and the hierarchical architecture, which provides enhanced accessibility to active sites and reduces particle aggregation.
| CO2 uptake (mmol g−1) | Charge/size ratio (z/r) | Ionic radius (Å) | Charge (z) | Cation |
|---|---|---|---|---|
| Low | 0.98 | 1.02 | +1 | Na+ |
| Low | 0.72 | 1.38 | +1 | K+ |
| Moderate | 2.78 | 0.72 | +2 | Mg2 |
| High | 2.00 | 1.00 | +2 | Ca2 |
| Moderate | 2.41 | 0.83 | +2 | Mn2 |
| Moderate | 2.53 | 0.79 | +2 | Co2 |
| High | 2.90 | 0.69 | +2 | Ni2 |
| High | 2.74 | 0.73 | +2 | Cu2 |
| Moderate | 2.70 | 0.74 | +2 | Zn2 |
| Low | 3.33 | 0.90 | +3 | Y3 |
| Low | 2.91 | 1.03 | +3 | La3 |
| Low | 2.97 | 1.01 | +3 | Ce3 |
| Low | 3.16 | 0.95 | +3 | Eu3 |
| Low | 3.26 | 0.92 | +3 | Tb3+ |
| Low | 3.49 | 0.86 | +3 | Yb3+ |
These theoretical insights into the effects of framework topology are well illustrated in the recent work by Al Atrach et al. (Fig. 40).229 The study offers a compelling demonstration of how key structural and compositional factors influence CO2 adsorption over zeolites, using LEV-type zeolite as a case study. By comparing two LEV samples with different morphologies and compositions: a nanosized sample (Si/Al ≈ 6.6) and a micron-sized sample (Si/Al ≈ 3.5). The LEV framework, characterized by its small-pore topology and pore dimensions of 3.6 × 4.8 Å, offers a favorable steric and electrostatic environment for CO2 capture due to its compatibility with the kinetic diameter and quadrupole moment of CO2. As a result, the micron-sized sample exhibits a 22% higher CO2 uptake (5.81 mmol g−1 at 0 °C) and superior selectivity (CO2/N2 = 84 at 25 °C) compared to the nanosized sample. Although the nanosized LEV has a higher surface area and mesoporosity, contributing to faster adsorption–desorption kinetics and better reversibility, its lower Na+ content results in weaker CO2 binding and reduced capacity.
The conversion of carbon dioxide (CO2) into valuable chemicals is a primary step in carbon capture and utilization (CCU) technology, but CO2 is a very stable molecule, which makes it difficult for its conversion into alternative compounds difficult, with a high dissociation energy of 750 kJ mol−1 as CO2 possesses strong C
O bonds, which indicates that breaking these bonds requires a significant quantity of energy. Consequently, to split CO2 molecules, high pressure, high temperatures, or catalysts are needed.196 In this context, the thermal catalytic conversion of CO2 into hydrocarbons has primarily followed two main pathways. Also, the selective hydrogenation of CO2 to CO via the reverse water–gas shift (RWGS) reaction is highlighted, which serves as a precursor step to further hydrocarbon in thermochemical systems.232 Notably, this intermediate step-CO-formation can also be achieved via electrochemical CO2 reduction (CO2RR), offering an energy-efficient and scalable route under ambient conditions, as will be discussed in subsequent sections. The RWGS can be completed by either of two approaches:
| CO2 + H2 → CO + H2O. {ΔH = 41.3 kJ mol−1} endothermic |
| CO2 + 4H2 → CH4 + 2H2O. {ΔH = −164.7 kJ mol−1} exothermic |
Zhang et al.,233 illustrate the intricate design and mechanistic pathways alongside the electrochemical performance of the CdO@Zn@Zeolite-Y system in a single diagram (Fig. 41a). The schematic captures the entire process of catalyst fabrication. The first step entails the ion exchange of Zn2+ into Zeolite-Y to yield ZnY. Subsequent incorporation of Cd2+ ions give rise to Cd(NO3)2@ZnY, and under thermal treatment, it converts to the final perovskite structure of CdO nanoclusters encapsulated within the microporous framework of Zn-doped Zeolite-Y. This form of nanoconfinement not only stabilizes the active sites but also preserves the structural integrity of the zeolite support. Electrochemical activity as defined in (Fig. 41b) is assessed through Linear Sweep Voltammetry (LSV) profiles, and as expected, CdO@ZnY doesn't disappoint. This hybrid catalyst achieves the highest total current density among all tested catalysts, suggesting unparalleled activity in CO2RR. In (Fig. 41c), product distribution analysis confirmed that CO was the dominant product, with a faradaic efficiency exceeding 90% at −0.8 V vs. RHE, while H2 and HCOOH contributions were almost negligible. In (Fig. 41d), it further compared the CO selectivity of all samples, which, alongside galvanostatic experiments, resulted in reinforcing the performance of CdO@ZnY in all tested voltages. Overall, (Fig. 41) serves as a strong multidisciplinary argument on how catalyst design, specifically based on zeolite nanoconfinement and bimetallic synergies integrated, can enhance CO2 conversion technologies.
Following the work of Zhang et al., Zhu et al.234 proposed a confined SnCuxO2+x@MFI catalyst that goes beyond CO2 capture to activation and electrochemical conversion into C1 and C2 products, including methane and ethylene. This shift highlights the increasing multifunctionality of zeolite support, from enabling *CO evolution to incorporating multi-step, multi-carbon sculpting processes. They designed a zeolite-constrained bimetallic oxide system, SnCuxO2+x@MFI, to promote high-efficiency CO2 electroreduction to methane production. As depicted in (Fig. 42a), the synthesis strategy involved the nanoconfinement of Sn–Cu oxide nanoclusters within the micropores and mesoporous framework of MFI zeolite. This spatial confinement stabilized the active metal–oxide interface, prevented nanoparticle aggregation, and significantly enhanced ion/electron transport due to the resulting mesoporosity (∼3.2 nm). (Fig. 42b) illustrates the comprehensive mechanistic and electrochemical activity of the SnCuxO2+x@MFI catalyst in the electrochemical reduction of CO2. A detailed top diagram describes the multi-step conversion of CO2 into CH4. Initiation commences with the CO2 adsorption and activation step, which is *COOH-intermediate forming, an essential species confirmed via the in situ SEIRAS analysis. Subsequent decoupling steps yield *CO, *CHO, and finally, *CHx intermediates, which lead to methane. Electrolysis of CO2 is demonstrated in (Fig. 41c), illustrating the electrochemical performance and LSV curves, where SnCu1.5O3.5@MFI was found to have the greatest CO2 current density within the CO2 saturated conditions, indicative of improved performance compared with reference catalysts. As shown in (Fig. 42d), faradaic efficiency attributed to C2H4 as a secondary function of *CH4 and C1 products reveals that a high-grade level is attained below −1.2 V, further supporting the previously mentioned hypotheses, while the production of H2 and HCOOH remains at the decuple level.
To realize this vision, key innovations include:
• Water-resistant coatings and pore tuning to maintain capture efficiency in humid streams.
• Mesostructuring to accelerate the diffusion of reactants and products.
• Hybrid material design, embedding zeolites in electrodes with catalytically active metals or conductive supports.
• Membrane reactor integration, enabling one-step CO2 separation and conversion in a compact, energy-efficient system.
Through the careful design and modification of these SBUs, linkers, and pore environments, MOFs provide an extraordinary level of structural and chemical adaptability to tackle global energy and environmental challenges.235 Because of their varied, customizable structural properties, which include but not limited to highly porous surface area, powerful organic and inorganic catalytic sites and tunable postsynthetic structure, MOFs are intriguing materials.236–238 These relatively new materials indicate themselves for general use in catalysis (photo-, electrocatalysis), energy storage, gas storage, hazardous adsorption, and so forth.236,239–242 MOFs have proven to be particularly effective as adsorbents and catalysts because of several significant benefits: (i) predictable and functionalizable structures. The design flexibility of MOFs allows for precise control of their architecture, facilitating the integration of accessible adsorption and catalytically active sites. (ii) Hybrid compatibility – MOFs can be combined with other materials to create composites or act as precursors/templates for MOF-derived structures that exhibit improved physical and chemical attributes. (iii) Superior catalytic performance. MOFs serve as a link between homogeneous and heterogeneous catalysis, delivering high catalytic efficiency while ensuring stability, easy separation, and reusability. (iv) Tailorable structure–property relationships. The well-defined, customizable nature of MOFs yields important insights into how alterations in structure impact catalytic performance, aiding in the rational design of catalysts. These distinctive features make MOFs extremely promising candidates for CO2 capture and utilization, fueling ongoing research aimed at optimizing them for sustainable energy and environmental uses as illistrated in (Fig. 44).
MOFs with their physiochemical adsorption strategy have shown high CO2 absorption capacities under both low- and high-pressure conditions, which is one of their primary advantages over conventional adsorbents like zeolites and activated carbon that depend solely on physical adsorption. For example, the well-defined pore structures and the presence of open metal sites in MOF-808 and its derivatives have demonstrated a better ability to absorb CO2.246 Another group investigated the CO2 absorption of HKUST-1 (MOF with OMSs) at 42 par and room temperature,247 recording roughly 10 mmol g−1. The CO2 adsorption isotherm of HKUST-1 at ambient temperature resulted in a typical Type I isotherm, reflecting that most of the gas is adsorbed at low pressures, indicating the MOF's high affinity for CO2 at low partial pressures. Given that the material will have a substantial CO2 capture working capacity, these conditions are intriguing for practical CO2 adsorption from gas streams. Because of its exceptional CO2 uptake capacities at low pressures, the M-MOF-74 (M = Mg2+, Ni2+, Co2+, Zn2+) isoreticular series, which consists of a sequence of one-dimensional hexagonal channels with OMSs at the SBUs, has emerged as one of the most extensively researched sets of MOFs for CO2 capture. The accessibility of coordinatively unsaturated metal sites in the pores, the integration of heteroatoms within the pores and their covalently linked functionality to the backbone, the specific interactions of MOF building units, the hydrophobicity of the pores, and a combination of these structural features are the main strata involved in the CO2 capture by MOF, as shown in (Fig. 45) represent the main strategies involved in the CO2 capture by MOF including presence of accessible coordinatively unsaturated metal sites in the pores; integration of heteroatoms within, as well as covalently linked functionality to, the backbone; specific interactions of MOF building units; hydrophobicity of the pores; and a hybrid of these structural features. While MOFs are well-recognized for their CO2 uptake capacities, their modular structure also makes them highly tunable for catalytic activity.
MOFs were originally applied as electrocatalysts for CO2RR in 2012;254,255 the copper rubeanate MOF (CR-MOF) had shown enhanced CO2RR performance. Since the CO2RR occurs at a complicated three-phase interface between liquid electrolyte gaseous CO2 solid catalyst. The primary crucial steps of the electrocatalytic processes are CO2 activation, surface reaction, and product desorption processes comprising (1) electron transfer, (2) mass diffusion, and (3) electrochemical reaction on the surface via three-phase interface. These three elements define the whole basis of the resulting catalytic activity; they are summed under the name “proficiency of active sites”. MOFs offer a wide range of possibilities in creating varied catalytic materials with many benefits, especially after electrochemical/thermal breakdown/pyrolysis, including (i) high mass transfer and availability of active sites, (ii) controls the electronic structure by simple heteroatom doping, and (iii) inherits the features of the pristine-MOFs. Consequently, MOF-based porous materials with the above-described properties are quite interesting candidates for CO2 electrocatalysis. Due to their highly adjustable architectures, vast surface areas, and variety of chemical functions, MOFs have become very adaptable platforms for the electrochemical reduction of carbon dioxide (CO2RR). Nevertheless, inherent difficulties including low electrical conductivity and restricted active site accessibility have prompted the creation of a number of engineering techniques to improve their catalytic effectiveness. The efficiency of CO2 conversion has been increased by structural engineering techniques, summarized in (Fig. 46), including crystal engineering to maximize electron transport, two-dimensional (2D) engineering to enhance surface exposure, and heterostructure formation to integrate MOFs with conductive or catalytically active materials.256 The modification of MOF's metal centers and organic linkers substitution significantly enhances the CO2RR selectivity and stability.257,258 Defect engineering and heteroatom doping can also improve overall reaction kinetics by introducing additional catalytically active sites and adjusting the electronic characteristics.259 Their use in CO2RR applications is further supported by the improved durability and charge transfer provided by MOF-based composites and derivatives, such as MOF-derived porous carbons or hybrids with conductive supports.260 There are comprehensive reviews discussing the utilization of MOFs and their derivatives in CO2RR, which is not the focus of this review.261–263
Liu et al. 2023272 engineered gas diffusion electrodes (GDEs) consisting of a series of silver cluster-based MOFs intended for the concurrent capture and reduction of CO2 to carbon monoxide (CO) from simulated flue gas containing 15% CO2 in nitrogen. The MOFs employed in this research possess amine groups, acknowledged for their capacity to absorb and concentrate CO2 from simulated flue gases in humid environments (Fig. 47a). These frameworks demonstrate significant porosity, allowing for efficient CO2 capture, while the silver clusters inside the MOFs promote the electrochemical reduction of the captured CO2 to CO. The CO2/N2 adsorption selectivity of Ag-MOF, Ag-MOF-CH3, and Ag-MOF-NH2 were 67, 42, and 280 at 298 K, respectively (Fig. 47b). When using NH2-MOF with pure CO2, the catalyst achieved a CO partial current density of 380 mA cm−2 and dropped slightly to 355 mA cm−2 despite an 85% decrease in CO2 concentration (Fig. 47c). In contrast, limited retention of 44% and 37% was observed on Ag-MOF and Ag-MOF-CH3, respectively. The findings indicated that the faradaic efficiency (FE) for CO production and the CO partial current density were markedly affected by the presence of amine groups when utilizing flue gas as the feedstock. When the CO2 concentration reduced from 15% to 5%, the eCO2RR performance decreased significantly, and the minimum CO2 concentration that didn’t influence the performance of the 1-NH2 significantly was 10%. The performance metrics obtained with flue gas were analogous to those recorded under pure CO2 circumstances, highlighting the essential function of amine groups in improving CO2 capture efficiency. It is worth noting that the continuous operating time of 1-NH2 is much longer than that of the materials reported to date (<100 hours).
Embedding MOFs into mixed matrix membranes (MMMs) is a promising approach for enhancing their stability and been intensively utilized in CO2 capturing. Al-Attas et al., 2023 reported a permselective MOF-GDL (PGDE):273 an innovative method for CO2 conversion from quasi-flue gas utilizing a permselective gas diffusion electrode (PGDE). This novel design combines a metal–organic framework (MOF)-based mixed matrix membrane (MMM) with a silver electrocatalyst, facilitating selective CO2 penetration and its conversion into carbon monoxide (CO) with high efficiency (Fig. 47d). The MMM integrates CALF-20, a metal–organic framework recognized for its capacity for CO2 physisorption in humid gas streams. This concept seeks to improve CO2 selectivity while preserving mechanical stability in industrial environments. The PGDE is designed with the MMM on the gas diffusion side of a porous PTFE electrode, which selectively permits CO2 to permeate while restricting the passage of other gases such as N2 and O2. CO2 diffuses through the membrane by concentration gradient. CALF-20 exhibited more than 4.5 times higher uptake for CO2 (3.97 mmol g−1) as compared to N2 and O2 at 298 K and 1 bar based on the CO2 physisorption isotherm and low adsorption affinity toward the CO2R (CO) target product of this study. When a mixed gas of 10% CO2 balanced with N2 permeated through the PGDE, it showed 1.1 × 106 gas permeation units (GPUs) with selectivity of 2.1 for CO2/N2. That is confirmed by the remarkable drop of N2 partial pressure across the PGDE from 1.06 to ∼0.48 psig while CO2 partial pressure only decreased ∼0.03 psig (Fig. 47e). The PGDE attained an impressive CO FE of 95% in the conversion of N2-diluted CO2 streams compared to 58% for the Ag/PTFE at −1.32 (Fig. 47f). The ideal loading of CALF-20 in the MMM was determined to be 7 mg cm−2, which optimized efficiency and inhibited pore obstruction. The PGDE exhibited resilience to the introduction of O2, sustaining 84% of its performance and displaying minimal impact from the wetness of the gas stream. However, the MMM's propensity for water absorption may result in the degradation of CO2-selective binding sites, a crucial factor for sustained operation, which was revealed while testing the stability. Also, the high overpotential applied means more energy is needed per mole of CO produced, hindering their scalability.
Zhang et al., 2018274 introduced Cu3(BTC)2 (Cu-MOF) into a carbon paper-based gas diffusion electrode (GDE) as a CO2 capturer, mixed with copper nanoparticles serving as the active catalyst. The CO2 adsorption capacity of Cu-MOF was quantified at 1.8 mmol g−1, signifying moderate efficacy in augmenting local CO2 concentration at the catalyst interface. The GDE was altered by 10 weight percent. Cu-MOF exhibited enhanced catalytic activity for CO2 reduction, achieving faradaic efficiencies for methane production that were 2–3 times greater than those of GDEs lacking Cu-MOF. The incorporation of Cu-MOF markedly inhibited the competitive hydrogen evolution process (HER), diminishing its faradaic efficiency to 30%. The study elucidates two opposing effects of Cu-MOF in the CO2 reduction reaction: an insulating effect that may impede electron transfer to Cu active sites and an augmentation of CO2 concentration at the electrode–electrolyte interface, which promotes the reaction. The interaction between these factors ultimately determines the reaction rate and product selectivity. Although CH4 FE was enhanced by introducing Cu-MOF compared to the blank, the maximum FE was moderate (17%), with the optimum Cu-MOF content relative to the theoretical maximum, and a significant portion of the current was directed to HER (30%), especially at higher overpotentials. Moreover, the Cu-MOF structure showed stability issues when used for 24 h due to hydrolysis or phase transformation in aqueous solution.
Selectivity is one of the main challenges in CO2RR, especially towards C2+ products, given their high benefit-to-cost ratio.275 The electrochemical reduction of CO2 (CO2RR) to ethylene (C2H4) is a viable approach for sustainable chemical synthesis. Nonetheless, attaining industrially significant productivity (>200 mA cm−2) and energy efficiency (>50%) poses challenges due to the solubility constraints of CO2 in aqueous electrolytes and the occurrence of competing side reactions. Nam et al., 2022276 developed MOF-augmented gas diffusion electrodes (MOF-GDEs) to increase local CO2 availability in proximity to catalytically active copper sites, therefore improving CO2RR selectivity and rate. The hierarchical electrode structure comprises a hydrophobic polytetrafluoroethylene (PTFE) substrate, a metal–organic framework (MOF) interlayer, and a sputtered copper catalyst (Fig. 48a). Two metal–organic frameworks, HKUST-1 and SIFSIX-3-Cu, with differing CO2 adsorption capabilities, were evaluated for their efficacy in enhancing CO2 concentration at the catalyst interface. The MOF-enhanced GDEs exhibited significant enhancements in ethylene production. In flow cell systems, MOF-modified electrodes attained a faradaic efficiency (FE) of 49% for ethylene at a current density of 1 A cm−2, surpassing traditional Cu/PTFE electrodes (Fig. 48b). The elevated local CO2 concentration enhanced CO2 adsorption and inhibited the hydrogen evolution reaction (HER), hence augmenting C2+ selectivity. The notion was further corroborated in zero-gap MEA electrolyzers, where MOF films situated on Cu electrodes markedly improved ethylene output. A peak ethylene partial current density (J C2H4) of 220 mA cm−2 was attained, representing a 2.7-fold enhancement compared to unmodified GDEs. Furthermore, for the carbon monoxide reduction reaction (CORR), the MOF-enhanced GDEs exhibited a 15-fold increase in ethylene production rate compared with bare Cu/PTFE electrodes, underscoring the significant impact of CO2 enrichment in high-current-density operations. The X-ray absorption spectroscopy (XAS) indicated that the MOF layers experienced structural alterations under electrochemical circumstances, resulting in the creation of organic-metal interfaces that enhanced CO2 adsorption and reaction kinetics. The electrodes' stability was evidenced after 65 hours of uninterrupted operation, sustaining ethylene selectivity above 50%. The results underscore the necessity of enhancing MOF characteristics, such as porosity, CO2 adsorption capacity, and hydrophobicity, to optimize electrocatalytic efficacy. The MOF-augmented GDEs maintain >50% FE for ethylene over 65 hours at industrially relevant current densities, with total C2+ product FE above 70% for 59 hours. Although the system achieves high current densities and good selectivity, the cell voltages required (up to −4.2 V in MEA mode) are relatively high, implying significant energy input per mole of product.277
Zhao et al., 2024278 reported a groundbreaking approach for the integrated capture and eCO2RR of dilute CO2 (15 vol%, mimicking flue gas) into 100% pure aqueous formic acid with 90% FE, addressing two challenges in CO2 utilization; (i) the need for high-purity CO2 as a feedstock and (ii) the separation of liquid products after the reaction. A conductive bismuth-based-MOF, Bi-HHTP (where HHTP = 2,3,6,7,10,11-hexahydroxytriphenylene), was utilized and served as a CO2 adsorbent and as an electrocatalyst. The Bi-HHTP possesses a microstructure π-conjugated framework with one-dimensional (1D) zigzag chains of distorted tetrahedral and pentahedral BiO4 nodes, interconnected through π–π stacking to form a 3D architecture (Fig. 48c), which enable a high CO2 selectivity and uptake (23.6 cm3 g−1 = 1.05 mmol g−1 at 298 K, CO2/N2 selectivity ∼91), under humid conditions (40% RH) (Fig. 48d), which is critical for industrial applications. The adsorption mechanism involves electrostatic interaction, hydrogen bonding and metal coordination, resulting in strong binding between CO2 and Bi-HHTP. It was found that H2O binds well to Bi-HHTP, forming hydrogen bonds, competing slightly with CO2, yet adsorbed H2O provides protons supporting the eCO2RR. Formic acid FE was slightly lower in dilute CO2 (CO2/N2 = 15
:
85, v/v) than in a high-purity CO2 atmosphere, with maximum values of 91% and 93% at 2.6 V, respectively (Fig. 48e). The formation of OCHO intermediate was confirmed by Operando ATR-FTIR spectroscopy, which is a key intermediate for formic acid formation. The DFT showed Bi-HHTP requires less energy (ΔG = 0.31 eV) to carry out the rate-determining step in the process compared to other bismuth-based catalysts like metallic Bi or Bi2CO5. The OCHO binds to Bi-HHTP just strongly enough (ΔE = −0.22 eV) to react efficiently, without poisoning the surface or releasing too early. The Technoeconomic analysis estimates a production cost ($0.74 per kg), highlighting commercial feasibility. Further examples of MOF-based materials for integrated CO2 capture and conversion are summarized in (Table 15).
| Material | Composition and structure | CO2 adsorption capacity | Faradaic efficiency (FE) | Key findings | Ref. |
|---|---|---|---|---|---|
| Cu-MOF-GDE | Cu3(BTC) 2 (Cu-MOF) incorporated into carbon paper-based gas diffusion electrode with copper nanoparticles | 1.8 mmol g−1 | CH4 FE increased 2–3× with Cu-MOF (∼20%); HER FE reduced to 30% | Cu-MOF enhances local CO2 concentration at the catalyst interface | 274 |
| Permselective MOF-GDL (PGDE) | CALF-20 MOF-based mixed matrix membrane (MMM) combined with silver electrocatalyst | CALF-20 exhibited 4.5 times higher uptake for CO2 (3.97 mmol g−1) as compared to N2 and O2 at 298 K and 1 bar. The PGDE showed 1.1 × 106 gas permeation units (GPUs) with a CO2/N2 selectivity of 2.1 for a mixed gas stream of∼10% CO2 and N2 balance | CO FE up to 95% | The MMM selectively allows CO2 permeation while restricting other gases. The weak binding of CO2 coupled with the specific pore structure minimizes CO2 chemisorption | 273 |
| MOF-functionalized GDE | HKUST-1 and SIFSIX-3-Cu MOFs as interlayers on hydrophobic PTFE substrate with sputtered copper catalyst | SIFSIX-3-Cu showed higher CO2 affinity (2.4 mmol g−1 vs. 0.3 mmol g−1 for HKUST-1) and better stability at lower mass loading | C2H4 FE up to 49% at 1 A cm−2 in flow cell (2.7-fold compared to bare Cu/PTFE electrodes), 52% for C2H4 in MEA, in CORR, the modified GDE demonstrated a 15-fold increase in ethylene production | MOF layers increase local CO2 concentration, enhancing ethylene production and suppressing hydrogen evolution | 276 |
| Ag12 cluster-MOF-GDE | Silver cluster-based MOFs with amine function groups | 1-NH2 MOF exhibited a CO2 uptake of 0.90 mmol cm−3 (≈ 9 mmol g−1) | CO FE ∼96.4% under simulated flue gas (CO2/N2 = 15 : 85) at 120 mAcm2 ∼96.3–97.3% under pure CO2 |
Amine-functionalized MOFs enhance CO2 capture from flue gas, with silver clusters promoting electrochemical reduction to CO. Performance under flue gas conditions is comparable to pure CO2 | 272 |
| Bi-HHTP-MOF | Bismuth-based-MOF, Bi-HHTP (HHTP = 2,3,6,7,10,11-hexahydroxytriphenylene) | 1.05 mmol g−1 at 298 K | 100% pure aqueous formic acid with 90% FE | Conductive Bi-HHTP acts both as a CO2 adsorbent and an electrocatalyst | 278 |
Generally, when designing an adsorbent layer on a GDE, it is crucial to create robust adsorbents with elevated CO2 adsorption capacity and selectivity, while also considering factors such as kinetic rate, active porosity, surface area for adsorption, and resistance to moisture and contaminants.
The electrochemical stability of metal–organic frameworks (MOFs) is a critical factor determining their applicability in electrocatalytic systems. During electrochemical operation, the applied potential drives the migration of ionic species from the electrolyte toward the MOF surface, leading to the formation of an electrical double layer.279 The accumulation of charge at this interface generates pronounced local ion concentration gradients, particularly involving protons or hydroxide ions, which can cause substantial deviations of the interfacial pH from that of the bulk electrolyte. Such localized pH fluctuations impose chemical stress on both the metal nodes and organic linkers, often resulting in partial or complete structural degradation of the framework.280,281 This instability is especially problematic under neutral and strongly alkaline conditions, where many MOFs are inherently susceptible to hydrolysis or ligand displacement. As a result, achieving durable performance in these media remains a key challenge for MOF-based catalysts in the CO2 electroreduction reaction (CO2RR). Moreover, repeated potential cycling further accelerates degradation by continuously reshaping cationic and anionic distributions at the electrochemical interface. These dynamic chemical gradients can promote metal leaching and coordination bond cleavage, ultimately driving the in situ conversion of MOFs into metal oxides, hydroxides, or oxyhydroxides during prolonged electrocatalytic operation.279,282
Achieving concurrent chemical, structural, and electrochemical robustness in metal–organic frameworks (MOFs) under operating electrocatalytic conditions remains intrinsically challenging, as strategies that enhance stability (e.g., stronger metal–ligand bonds, increased hydrophobicity) often compromise properties such as electronic conductivity, porosity, or active-site accessibility. Over roughly the past decade, sustained progress in linker design, node selection, and composite engineering has nevertheless enabled significant improvements in MOF durability under electrochemical CO2 reduction (CO2RR) conditions, particularly in aqueous and humid environments. Despite these advances, a central question persists regarding the true nature of the catalytically active phase: in many reported systems, it remains ambiguous whether the pristine MOF operates as the genuine electrocatalyst, or whether the framework instead serves as a sacrificial or pre-catalyst that reconstructs into metal oxides, hydroxides, oxyhydroxides, or other derived phases under applied bias. Resolving this ambiguity requires rigorous operando or in situ characterization, such as X-ray absorption spectroscopy, X-ray diffraction, vibrational spectroscopy, and electron microscopy, combined with systematic post-reaction structural and compositional analyses to verify chemical integrity, crystallinity, and metal speciation after prolonged electrolysis. Such mechanistic insight is essential for the rational design of MOF-based architectures that can sustain CO2RR over technologically relevant timescales.282,283
During electrochemical operation, MOFs are subjected to a complex and dynamic reaction environment that includes liquid water, electrolyte cations and anions, dissolved reactants and products, interfacial electric fields, and continuous electron and ion fluxes. Among these factors, water frequently plays a primary role in triggering degradation, as it can coordinate to metal nodes and promote competitive ligand exchange or hydrolysis of coordination bonds, ultimately yielding hydrated or hydroxylated metal species in alkaline media and protonated or partially detached organic linkers in acidic media.282,283 These processes often lead to partial or complete leaching of metal centers and ligands into the electrolyte, progressively eroding the long-range order of the framework. In parallel, specific electrolyte anions can substantially accelerate degradation pathways: strongly coordinating species such as phosphate, carbonate, or sulfate may outcompete the MOF linker for binding to high-valence metal centers, thereby destabilizing the metal–ligand coordination network. Zirconium-based carboxylate frameworks, which are otherwise chemically robust, have been reported to undergo rapid degradationin phosphate-containing electrolytes, where strong Zr–phosphate interactions drive fast deterioration of the Zr6-oxo clusters and loss of crystallinity on experimentally relevant timescales.284,285
Framework instability under electrochemical conditions is not confined to carboxylate-based MOFs. Zeolitic imidazolate frameworks (ZIFs), despite their topological analogy to zeolites and relatively strong metal–imidazolate bonds, can also undergo structural transformation or collapse under CO2RR- or ORR-relevant potentials, particularly in electrolytes containing additional metal cations. Ion-exchange processes at the node, followed by nucleation and growth of metal (oxy)hydroxide phases, have been widely observed, frequently leading to the formation of mixed-metal hydroxide or oxide nanostructures at the expense of the original framework.286 Beyond purely chemical degradation, reaction-derived products impose additional mechanical and chemical stress on MOFs: gas-evolving reactions often generate nanoscale bubbles at or within the porous structure, imposing localized pressure and shear that can induce cracking, delamination, or fragmentation of MOF crystallites. Furthermore, soluble products or intermediates from CO2RR (e.g., formate, carbonate, or multicarbon species) may coordinate to metal nodes or interact strongly with linkers, promoting further reorganization or dissolution of the framework over extended operation.287,288
The intrinsic susceptibility of many MOFs to humidity and aqueous environments commonly manifests as rapid performance degradation, especially in neutral and alkaline media, where moisture-mediated attack on metal centers and linkers leads to decomposition or phase transformation. In this context, metal–ligand bond strength has emerged as a key design parameter governing MOF stability under electrochemical conditions. Stronger coordination interactions generally correlate with enhanced resistance to hydrolysis, ligand displacement, and nucleophilic attack. Guided by this principle, stability is often improved by employing high-valent, hard metal centers and appropriately matched ligands. Frameworks constructed from hard, high-charge-density metal ions—such as Zr4+, Cr3+, Al3+, and Fe3+ paired with oxygen-donor carboxylate ligands typically display superior chemical robustness, in line with Hard–Soft Acid–Base (HSAB) considerations. These strong metal–oxygen bonds not only increase resistance to hydrolysis and ligand loss in aqueous and humid environments but can also impart persistence under moderately acidic conditions, particularly when the carboxylate linkers possess low pKa values and form highly stable coordination clusters (e.g., Zr6O4(OH)4 nodes in UiO-type frameworks).289–292 Collectively, these design concepts underpin ongoing efforts to develop MOF-based electrocatalysts that combine structural integrity, chemical resilience, and sustained activity for CO2 electroreduction.
![]() | ||
| Fig. 49 Graphical abstract of metal oxides for integrated CO2 capture and electrocatalytic conversion. | ||
DEA–SnOx/C was synthesized by a one-pot hydrothermal reaction of carbon black, SnCl2, and DEA in ethanol, as shown in (Fig. 50a). The dual-function catalyst developed via grafting alkanolamines such as diethanolamine (DEA) onto SnOx surfaces (DEA–SnOx/C) that augments local CO2 concentration via Lewis base interactions while also tailoring reaction selectivity toward formate. DEA–SnOx/C exhibited significantly higher CO2 adsorption capacity than the non-functionalized SnOx (SnOx/C) (Fig. 50b), indicating the strong interaction between DEA and CO2. This combined with the enhanced hydrophobicity and suppression of side reactions resulted in a standout performance of 84.2% faradaic efficiency for formate at −0.75 V vs. RHE (Fig. 50c). The DEA–SnOx/C can operate at low CO2 concentration (10%) and FEhcoo− reaching over 80% (CO2 = 30%) whereas the jHCOO peaked when the concentration was 50% reaching 7.9 mA cm−2 (Fig. 50d). Despite this notable selectivity performance, the formate jHCOO of 6.7 mA cm−2 is below industrially relevant benchmarks (≥100 mA cm−2). Furthermore, the degradation of amine groups limited the catalyst's stability over a prolonged period, and the catalyst was evaluated in a static setup (single-compartment design) with a small electrode area (0.071 cm2), not in continuous flow or gas diffusion configurations, limiting scalability.
A recent study by Nabil et al.295 reported an integrated approach for the simultaneous capture and electrochemical conversion of CO2 from dilute gas streams using a bifunctional gas diffusion electrode (BGDE). A high-density polyethylene-derived porous carbon (HPC) was employed as a physisorbent combined with polycrystalline copper as the electrocatalyst (Fig. 50e). The BGDE structure utilized a concentration gradient-driven desorption mechanism, which allows efficient CO2 capture and release at low CO2 concentration (∼10 vol%), eliminating the need for energy-intensive regeneration steps commonly applied with traditional capture technologies. HPC permeance of CO2 was as high as 4.0 × 106 GPU and a CO2/N2 selectivity of ≈1.3. When testing the CO2RR without sorbent (HPC) the total selectivity for eCO2R products with partial pressure PCO2 = 0.1 atm (10% CO290% N2) ranged from 33% to 41% depending on the voltage and current density, while with the sorbent (HPC = 8 mg cm−2) it increased by about 20% (Fig. 50f). However, lower selectivity resulted with higher HPC loading due to the blocking PTFE pores during airbrushing and thus deterring CO2 diffusion (Fig. 50g). Notably, the BGDE maintained its performance under humid environments, due to the hydrophobic and CO2-selective characteristic of carbonaceous HPC. Based on molecular dynamics simulations and gas permeance studies, the high CO2/N2 selectivity (≈1.3) is emphasized, caused by the molecular sieving properties incorporated within the micropores of HPC, significantly boosting the CO2 transport to the catalyst interface. The techno-economic study showed that this in situ system could dramatically diminish the minimum selling price of ethylene up to ∼79% when compared to the decoupled capture and conversion method.
Yan et al. (2024)296 developed a redox-mediated electrochemical platform for integrated CO2 capture and utilization (eCCU) utilizing anthraquinone (AQ)-grafted polymer electrodes. The polymeric film, constructed from a polyacrylamide backbone, chemically binds CO2 via reversible carbamate production when the AQ groups are in their oxidized (quinone) state. During electrochemical reduction, the AQ units emit CO2 in situ, which subsequently diffuses to an adjacent Ag catalyst layer for electrochemical conversion. This electrochemical regeneration circumvents thermal desorption, functions at ambient settings, and facilitates fine redox-tunable control over capture and release. In situ ATR-FTIR and DFT analyses (Fig. 51a–d) validate the generation of CO2-AQ adducts and their reversible conversion during potential cycling. The system exhibits stable multi-cycle functionality, preserving capture–release efficiency and CO2 consumption without necessitating gas-phase CO2 input or supplementary purification. The system achieves a faradaic efficiency of up to 82% for CO generation on the Ag catalyst under optimal electrochemical conditions. The platform provides a solvent-free, modular design that integrates capture and conversion inside a singular reactor architecture. The capture capacity is constrained by the loading and accessibility of AQ functional groups, and increasing the film thickness or redox density presents trade-offs with ion transport and conductivity. The reaction is presently limited to CO2-to-CO conversion, constraining subsequent chemical flexibility. Future work may concentrate on broadening the platform to encompass multi-carbon product catalysts, augmenting the stability of AQ functions, and designing more conductive or porous film morphologies to enhance throughput and scalability. This redox-active electrode method represents a notable step towards low-energy, continuous electrochemical carbon capture and utilization systems, providing a framework for integrating CO2 binding and conversion into a single electrochemical unit.
Xu et al. (2020)297 attempted to use pressurization (10–15 bar) to enhance CO2 mass transfer as a strategy to produce C2+ from simulated flue gas. This strategy enabled efficient C2+ production (91% FE, at 15 bar without O2). The study showed that while pressurization enhances CO2 availability and suppresses the hydrogen evolution reaction (HER), it also increases the oxygen reduction reaction (ORR), distracting most of the current towards ORR because of the lower thermodynamic and kinetic requirements for ORR compared to CO2RR (Fig. 52a). To counteract this, the authors first tried mixed Nafion-bound carbon nanoparticles layer to stabilize CO2RR which failed in O2-containing CO2 streams. They introduced a hydrophilic ionomer-TiO2 catalyst layer on a Cu-based gas diffusion electrode that significantly slowed O2 transport and maintained CO2 accessibility (Fig. 52b). This design leverages the lower volatility of CO2 compared to O2, allowing selective gas transport through hydrated nanopores. The ionomer-TiO2 structure stabilizes the Cu catalyst and reduces O2 mass flux by an order of magnitude compared to hydrophobic ionomers (e.g., Nafion). Fig. 52b shows 68% FE for C2 products (ethylene and ethanol) was achieved at 10 bar, and 26% full-cell energetic efficiency over 10 hours, even with O2, which is comparable to pure CO2-fed systems (Fig. 52c). However, additional studies using real flue gas with other impurities (e.g., SOx, NOx) and investigating long-term catalyst stability and scalability are still needed.
Zhu et al., 2023298 illustrated a pioneering, continuous, integrated system for CO2 capture and release utilizing a modular electrochemical solid–electrolyte reactor (Fig. 53a–d). This concept integrates absorption and release within a single unit, operates at ambient conditions, and uses only water as input, in contrast to amine scrubbing or disconnected electrochemical/chemical systems. At the cathode, oxygen reduction (ORR) produces OH−, establishing a localized alkaline environment that interacts with CO2 to yield carbonate ions. The ions traverse an anion-exchange membrane into the solid–electrolyte layer, whereas protons generated by water oxidation (OER) at the anode pass through a cation-exchange membrane. The ions recombine, releasing high-purity (>99%) CO2 gas continuously. The system achieves high capture rates (about 440 mA cm−2, 86.7 kg CO2 day−1 m−2), exceeds 90% faradaic efficiency, and approaches 98% carbon-removal efficiency in simulated flue gas (Fig. 52e–h). Notwithstanding these benefits, the methodology is constrained by limitations such as mass-transport bottlenecks at low CO2 concentrations (resulting in decreases in faradaic efficiency, CO poisoning of Pt/C catalysts, and energy losses due to ohmic drops in the solid–electrolyte layer. The authors investigated the utilization of cobalt single-atom catalysts (Co-SAC) that are resistant to CO poisoning while preserving high efficiency, even at diminished CO2 concentrations. They additionally suggest enhancements such as minimizing solid–electrolyte thickness, employing different redox couples (e.g., 2e− ORR for H2O2 production to increase electron efficiency to approximately 0.7 CO2 per electron), and sophisticated catalyst and membrane engineering. These tactics could decrease capture costs from approximately $83 to around $33 per ton, establishing this electrochemical platform as a viable method for sustainable, decentralized CO2 capture in conjunction with renewable energy and subsequent conversion operations.
Li et al. (2024)299 enhanced this design by amalgamating direct air capture and electrochemical conversion into a unified solid-state platform, functioning effectively at ambient settings, utilizing ambient air and water as feedstocks. Utilizing CO-tolerant, non-precious Cu catalysts alongside a polymer-based electrolyte, they tackle challenges related to catalyst expense, CO poisoning, and energy inefficiency, while directly generating ethylene without the need for intermediate CO2 purification, providing a more efficient and sustainable approach for decentralized carbon utilization. This study introduces a solid-state electrochemical reactor that efficiently captures CO2 and H2O from ambient air and converts them into ethylene and oxygen at approximately 25 °C, achieving FE of around 34%, remarkable energy efficiency of around 80%, and operating at a low voltage of about 0.6 V with a current of 1 A. Simple and scalable cathode fabrication method is shown in (Fig. 54a). The anode structure is presented in (Fig. 54b). The solid polyelectrolyte facilitates the migration of OH− ions from the conductive cathode to the nickel anode under an electric field, while also enabling the transfer of produced water from the nickel anode to the conductive cathode (Fig. 54c). The system employs a stratified architecture: a cathode composed of conductive carbon foam integrated with copper nanoparticle-coated SWCNTs for CO2 reduction catalysis, a PEO/KOH-infused polypropylene membrane serving as a solid electrolyte for OH− transport, and a nickel foam anode facilitating oxygen evolution. CO2 is sequestered by PEI/zeolite 13X composites, while H2O is absorbed by CaCl2-based hygroscopic salts, facilitating the in situ synthesis of formate and CO, which are then reduced on the Cu catalyst surface to provide ethylene by CO–CO coupling (Fig. 54d). This method facilitates compact, scalable, and continuous direct air capture (DAC) and conversion of low-concentration CO2 without the need for compression or gas purification. The system effectively generates around 70 mg of ethylene per hour, demonstrating the reactor's capability to generate hydrocarbons from air-sourced carbon under ambient settings without the need for gas purification or compression.
The incorporation of metal oxides for concurrent carbon dioxide (CO2) collection and electrochemical reduction (CO2RR) signifies a viable approach for enhancing carbon-neutral energy and chemical output. Due to their distinctive physiochemical characteristics, such as high CO2 affinity, surface tunability, and catalytic activity, metal oxides, including SnOx, CuO, Bi2O3, and In2O3, have become attractive options for dual-function systems. These materials not only promote CO2 adsorption via acid–base interactions and surface changes (e.g., amine functionalization) but also work as active electrocatalysts that convert CO2 into valuable products such as formate, carbon monoxide, ethylene, and ethanol. Notwithstanding substantial advancements, some essential knowledge deficiencies persist that must be resolved to enhance the practical implementation of metal oxide-based integrated CO2 capture and conversion systems. Present constraints encompass sub-industrial current densities for product generation, inadequate comprehension of the long-term stability of oxide-based catalysts (particularly under variable gas compositions and humid environments), and a lack of mechanistic understanding regarding surface transformations and intermediate stabilization during operational conditions. Further details are listed below:
• Rational interface and catalyst design: engineering hybrid systems that integrate metal oxides with conductive substrates (e.g., carbon nanomaterials, metal–organic frameworks, or polymers) may enhance charge transport, catalytic stability, and overall efficiency.
• Operando and in situ characterization: utilizing sophisticated spectroscopic and microscopic methods (e.g., XAS, FTIR, Raman, and TEM) under operational conditions is crucial for clarifying active sites, reaction intermediates, and degradation routes.
• Surface functionalization and defect engineering: modifying the surface characteristics of metal oxides through doping, the introduction of oxygen vacancies, or the grafting of alkanolamines can markedly improve CO2 affinity and adjust product selectivity.
• System-level integration and optimization: the integration of metal oxides into modular platforms, including gas diffusion electrodes, pressurized flow reactors, and solid-state electrochemical cells, is essential for enhancing technology readiness. Employ strategies such as pressure manipulation and permselective membranes to improve gas transport and reaction kinetics.
![]() | ||
| Fig. 55 Comprehensive schematic of integrated CO2 capture and electrocatalytic conversion through reductive aminolysis using multifunctional amine solvents. | ||
| RNH2 + CO2 ⇌ RNH2+–COO− | (1) |
| [RNH2+–COO−] + RNH2 → RNHCOO− + RNH3+ | (2) |
| CO2 + 2RNH2 ↔ RNHCOO− + RNH3+ | (3) |
| CO2 + R3N + H2O ↔ R3NH++ HCO3− | (4) |
A recent study by Pérez-Gallent et al. demonstrated the dual functionality of amines for an integrated CO2 capture and electrochemical conversion owing to their, chemical and physical absorption functions.311 From physical properties prospectives of amines which transforms the inherent ohmic heating into raising the reactor temperature from 15 °C to 75 °C that enhance the CO2 desorption step nearly 8-fold and increase the format reaction rate by a factor of 10, reaching 0.56–0.7 mmol m−2 s−1 (Fig. 57a). In addition to the high capture capacity of CO2, the product selectivity was also notable, with faradaic efficiencies up to 50% for formate and 45% for CO, alongside the detection of glycolate and oxalate as additional reduction products. Electrolyte composition and concentration proved critical: replacing propylene carbonate (PC) with water caused a 70% decline in formate yield due to competing hydrogen evolution, while optimizing AMP concentration at 2 M maximized efficiency and reaction rates, whereas higher concentrations introduced viscosity-related mass transfer limitations. However, in the absence of AMP, oxalate dominated with initial faradaic efficiencies of 80%, though this decreased over time (Fig. 57b and c). The reaction rate of CO2 electroreduction increased strongly with electrolyte temperature, with formate production rising from 15 to 75 °C (0.56 mmol m−2 s−1) while maintaining a relatively constant faradaic efficiency, reaching 40% at 75 °C. Compared to Alvarez-Guerra et al., who reported lower rates (0.075 mmol m−2 s−1) despite higher efficiencies (80%) on Pb in aqueous bicarbonate, the PC-based system offers a better balance of rate and selectivity. The organic solvent plays a critical role, as a high current density (40 mA cm−2) was observed at 75 °C, compared to aqueous AMP, where the FE towards formate dropped to 3% after five h due to increased HER. CO2 loading studies further revealed that higher temperatures accelerate CO2 desorption, with only 10% retained after five h at 75 °C, compared with 93.5% at 15 °C (Fig. 57d).
A side-by-side comparison of main catalyst-electrolyte systems and their performance metrics is presented in Table 16, emphasising the variation in faradaic efficiencies, operating potentials, and current densities achieved in different configurations.
| Catalyst/electrode | Potential (V vs. RHE) | Product | FE (%) | Current density (mA cm−2) | Solvent/conditions | Ref. |
|---|---|---|---|---|---|---|
| Ag/carbon-black on 300 nm Ag film | −0.8 | CO | 72 | 50 | 30 wt% MEA + 2 M KCl, 60 °C | 312 |
| Ag/carbon-black on 300 nm Ag film | −0.8 | CO | 100 | 30 | 30 wt% MEA + 2 M KCl, 60 °C | |
| Ag/carbon-black on 300 nm Ag film | −0.66 | CO | 30 | — | 2 M MEA + 2 M CsCl, 25 °C | |
| Ag/carbon-black on 300 nm Ag film | −0.66 | CO | <5 | — | 2 M MEA, no salt | |
| Cu + MEA | −0.78 | CO | 22 | 14.8 | 0.1 M NaClO4 aq. + CO2-loaded MEA | 313 |
| Cu + EDA | −0.78 | CO | 58 | 18.4 | 0.1 M NaClO4 aq. + CO2-loaded EDA | |
| Cu + DCA | −0.78 | CO | 19 | 9.7 | 0.1 M NaClO4 aq. + CO2-loaded DCA | |
| Ag (porous + CTAB) | −0.8 | CO | 38.2 | 39.1 | 30% MEA w/w aq., CO2-saturated + 0.1% CTAB | 314 |
| In (porous + CTAB) | −0.8 | HCOO− | 54.5 | ∼13.4 | CO2-saturated 30% MEA, 0.1% CTAB | |
| In (porous + CTAB) | −0.8 | CO | 22.8 | ∼2.0 | CO2-saturated 30% MEA, 0.1% CTAB | |
| Pb (porous + CTAB) | −0.8 | HCOO− | 60.8 | ∼2.2 | CO2-saturated 30% MEA, 0.1% CTAB | |
| Bi (porous + CTAB) | −0.8 | HCOO− | 36 | ∼18.3 | CO2-saturated 30% MEA, 0.1% CTAB | |
| Sn (porous + CTAB) | −0.8 | CO | 16.6 | ∼8.9 | CO2-saturated 30% MEA, 0.1% CTAB | |
| Sn (porous + CTAB) | −0.8 | HCOO− | 11.6 | ∼4.1 | CO2-saturated 30% MEA, 0.1% CTAB | |
| HCl-modified Ag | −0.91 | CO | 91 ± 7 | ∼3.0 | 1 M AMP + 0.3 mM CTAB, CO2-sat. aq., RT, H-cell | 315 |
| HCl-modified Ag | −1.01 | CO | 91 | (higher than at −0.91 V) | 1 M AMP + 0.3 mM CTAB, CO2-sat. aq., RT, H-cell | |
| HCl-modified Ag | −0.91 | CO | 54 | — | 1 M MEA aq., no CTAB (vs. AMP system) | |
| HCl-treated Cu | −0.61 | HCOO− | ∼68 | — | 1 M AMP + 0.3 mM CTAB, CO2-sat. aq., H-cell | |
| HCl-treated Zn | −0.91 | CO | ∼40–50 | — | 1 M AMP + 0.3 mM CTAB, CO2-sat. aq., H-cell | |
| Ni–N/C (single atom) | −0.9 to −1.1 | CO | 78.3 | −2.6 | 5 M MEA, H-cell | 316 |
| Ni–N/C (MEA cell) | — | CO | 64.9 | −50.0 | 5 M MEA, zero-gap membrane electrode assembly | |
| Ag nanoparticles | −0.9 to −1.1 | CO | 38.3 | −0.79 | 5 M MEA, H-cell | |
| Ag nanoparticles (MEA cell) | — | CO | 25.5 | −50.0 | 5 M MEA, membrane electrode assembly | |
| Cu Nanodendrites | −0.77 | HCOO− | 54.78 | ∼21.0 | CO2-sat. aq. ethanolamine (0.05 mol frac.) | 317 |
| Ag Nanodendrites | −0.77 | HCOO− | 35.84 | ∼7.9 | CO2-sat. aq. ethanolamine (0.05 mol frac.) | |
| Au Nanodendrites | −0.77 | HCOO− | 60.3 | ∼46.6 | CO2-sat. aq. ethanolamine (0.05 mol frac.) |
The (Table 16) indicates amine-based media are promising for electrochemical conversion of CO2 with moderate to high selectivity towards CO and formate, especially when co-catalysts, salts, or surfactants are added. Besides electrode design, mass transport, and electrolyte conductivity improvements, additional progress is needed toward industrially meaningful current densities.
• Low ionic conductivity and high Ohmic losses: technologies based on amines are less ionic in their conductivity than alkaline electrolytes, resulting in greater cell voltages and energy consumption. Alkali cation electrolyte engineering increases electron transport but does not fully eliminate this challenge.318
• Competing hydrogen evolution reaction (HER): HER decreases CO2 reduction selectivity, especially at high overpotentials and current densities. Catalyst and electrolyte modification decreases HER to some extent, but cannot eliminate it.
• Amine degradation: oxidative and thermal degradation of amines during electrolysis creates byproducts that decrease solvent lifetime and increase operating expenses. Use of sterically hindered amines, radical scavengers, and optimal operating conditions reduces but cannot prevent degradation.
• Scalability and moderate current densities: while continuous-flow systems can sustain current densities of as much as 200 mA cm−2, batch systems realize lower current densities, which limit throughput and industrial scalability.
• Inefficient capture medium regeneration: electrochemical conversion does not always fully regenerate amine solvents, which requires extra processing steps.
Integrated capture and conversion electrochemistry can reduce the energy requirement for carbon capture hardware by up to 44% compared with conventional thermal regeneration, primarily by excluding the high-temperature stripping step 1. However, inefficiencies in currently available systems, such as high cell voltages (3–5 V at 100 mA cm−2), solvent degradation, and modest current densities, limit economic competitiveness. Integration of renewable power will help offset electricity costs and improve sustainability, but intermittency and system longevity remain concerns. Since amine-based electrolytes are hindered by low ionic conductivity, competition with hydrogen evolution (HER), solvent degradation, and moderate current densities, new capture media such as ionic liquids (ILs) and deep eutectic solvents (DESs) are gaining increasing research interest. These solvents have greater CO2 solubility, enhanced electrochemical stability, and adjustable physicochemical properties, which can surpass the intrinsic shortcomings of amines and allow for more efficient, stable, and scalable integrated CO2 capture and conversion systems.319
![]() | ||
| Fig. 58 Detailed process schematic of integrated CO2 capture and electrocatalytic conversion using functionalized ionic liquids (ILs) in a continuous ICCC system. | ||
The success of ammonium-based ionic liquids demonstrated the feasibility of creating room-temperature molten salts by pairing organic (alkylammonium) cations with appropriate anions. Building on these principles, researchers have designed a wider array of ILs, moving beyond simple ammonium salts by pairing various organic cations (such as imidazolium, pyridinium, or phosphonium) with inorganic or organic anions (e.g., BF4−, PF6−, NTf2−). Importantly, these new ILs do not require specific functional groups for gas binding; their effectiveness largely stems from the use of bulky, asymmetric cations (often inspired by amines or ammonium ions) and weakly coordinating anions, which ensure the resulting salt remains liquid at room temperature and provides high ionic mobility.
ILs retain the reactive functionalities of amines while offering versatile and tunable physical properties. They serve as liquid electrolytes, demonstrate strong thermal and electrochemical stability, and can be precisely tailored for specific applications. These features make ILs ideally suited for integration with electrochemical systems, allowing the seamless co-integration of CO2 capture and conversion processes, such as electrochemical reduction, thereby advancing sustainable carbon management solutions.
:
2 CO2
:
amine ratio, making it highly effective for capture but energetically costly for regeneration, as the bond must be broken to liberate CO2. In contrast, ILs are salts that are entirely composed of cations and anions and are liquid at or near 100 °C, that interact with CO2 primarily via physical absorption (bottom panel).322 ILs such as 1-butyl-3-methylimidazolium tetrafluoroborate ([Bmim][BF4]) physically dissolve CO2 via weak, non-covalent interactions, including van der Waals forces, Coulombic attractions, and Lewis acid–base interactions (in this case with the anion).323
The structure of IL plays a crucial role in the CO2 solubility. Fluorinated anions ([PF6]−, [Tf2N]−) and long alkyl chains on the cation can enhance free volume and hydrophobicity, favouring CO2 uptake. For example, phosphonium-based ILs like [P66614].324 For instance, [P66614][2-CNpyr] has a capacity of 76.5 mg CO2 per g solvent at 22.1 °C and 57.4 mg CO2 per g solvent at 40.1 °C and 1 bar of CO2.324,325
Numerous studies have examined the influence of IL structural properties on CO2 solubility and absorption. These reports reiterate that in conventional ILs, the physical forces dominate and solubility is principally governed by anion features, free volume, and the strength of weak intermolecular forces.326 The following (Table 17) presents a summary of notable contributions in this sense, including some insight into the creation of ILs for CO2 capture.
| ILs studied | Key findings | Ref. |
|---|---|---|
| [Bmim][PF6] | High CO2 solubility observed in [Bmim][PF6]; at 40 °C and 93 bar, the IL phase contained a CO2 mole fraction of 0.72 | 327 |
| General imidazolium-based ILs | CO2 solubility increases with longer alkyl chains on the cation; solubilization is mainly physical | 328 |
| [Bmim][PF6], [Bmim][BF4] | weak Lewis acid–base interactions between CO2 and IL anions, which enhance dissolution | 329 |
| Various imidazolium-based ILs | Combined experiments and simulations; concluded CO2–anion interactions dominate solubility behavior | 330 |
| Various imidazolium-based ILs | Physical solubility in ILs depends on anion–CO2 interactions | 331 |
| Conventional imidazolium-based ILs | Emphasized van der Waals forces and hydrogen bonding; solubility is governed by weak physical interactions, not covalent bonds | 332 |
Conventional ionic liquids (ILs) have a great deal of potential for CO2 capture due to their tunable structures, low volatility, and ability to absorb CO2 through weak non-covalent interactions (i.e., van der Waals forces, coulombic interactions, or Lewis acid–base interactions); however, they are limited to CO2 uptake as ILs contain no chemically reactive sites. With the potential drawbacks of traditional ILs, researchers have synthesized, modified, or functionalized ILs with reactive functional groups (most commonly amino, hydroxyl, carboxyl, or heterocyclic donors) that can form covalent, or at least reversible bonds with CO2, thereby enhancing uptake capacity and selectivity.333 Incorporating chemical functionality into ILs changes the role of ILs from purely being physical solvents with non-covalent interactions and has a diverse range of possible applications because they can now be classified in two broad categories; the first category is Amino-functionalized ILs (AFILs), which are usually designed to mimic traditional alkanolamines carbamate-forming behavior relative to CO2, these typically incorporate (–NH2) amine groups into the alkyl side chains of cations (e.g. imidazolium, pyrrolidinium), or add it to the anion (which would simultaneously bond chemically to the CO2 to form a carbamate or bicarbonate species). In fact, according to the position of the reactive functional group, AFILs can also be classified based on:
• Cation-functionalized ILs, containing NH2 or –OH groups that can react with CO2 through nucleophilic attack (producing zwitterionic carbamates in a 1
:
2 CO2
:
IL ratio).333,334
• Anion-functionalized ILs, holding reactive functional groups (carboxylates, amino acids) that capture CO2 through a stoichiometric path (1
:
1 equivalence) to create carbamic acids.335,336
• Dual-functionalized Ils combine both cationic and anionic functionalities to create multiple binding sites, thereby enhancing CO2 absorption capacity (exceeding 2 mol CO2 per mol IL), improving absorption kinetics, and offering greater operational flexibility.337,338
The nature of the functional groups, whether they are amino, carboxyl, phenolate, or nitrile, plays a role in defining the mechanism and overall efficiency of CO2 capture. The functionalized group type can be tailored (Fig. 60).
Table 18 provides a comparison of several representative amino-functionalized ILs, as well as a summary of functional groups used, CO2 capacities relative to non-functionalized analogues, and associated operation advantages and disadvantages.
| IL example | Functionalization | Key functional group(s) | CO2 absorption (vs. non-funct. IL) | Comparison IL | Advantages | Disadvantages | Other notes | Ref. |
|---|---|---|---|---|---|---|---|---|
| [P66614][AA] | Anion | –NH2/–COOH (amino acid) | 1.6–2.0 mol mol−1 (2.5–3.3× higher) | [P66614][DCA] (0.6 mol mol−1) | Low viscosity | Water-sensitive; humidity effects | Carbamic acid stability is humidity-dependent | 339 |
| 1-(3-Aminopropyl)-3-butylimidazolium BF4 | Cation | Primary amine (–NH2) | ∼0.5 mol CO2/mol (much higher) | [hmim][PF6] | High, reversible absorption; recyclable | High viscosity | Stable carbamate over cycles (IR/NMR confirmed) | 340 |
| [apbim][BF4], etc.; dual-functionalized | Cation, Anion, Dual | Amino, Alkoxide, Carboxylate | Up to 2.6 mol CO2 per mol (1–2× higher) | [Bmim][BF4], [Bmim][PF6] | High capacity; tunable properties | High viscosity; synthesis complexity | Forms carbamates, carbonates, or zwitterions | 333 |
| [P66614][2-CNPyrr] | Anion | Nitrile (–C N, AHA anion) |
∼1.0 mol mol−1 (2× vs. [Pro]) | [P66614][Pro] | Low viscosity, stable, fast kinetics | Slightly lower capacity than azolates | Zwitterionic product; minimal viscosity increase | 324 |
| [N2111][2-CNpyr], etc. | Cation + Anion | 2-Cyanopyrrolidine (AHA) | Much higher via ylide chemisorption | General RTIL/alkanolamine refs | High stability, strong chemisorption | High viscosity, cost, and complexity | Zwitterion framework, IR/thermodynamics supported | 326 |
| [Bmim][B(CN)4], etc. | Anion | Multiple nitrile (–CN) | Increases with more –CN | [Bmim][SCN] | Tunable high solubility, diffusivity | May increase viscosity | CO2 solubility dictated by cation–anion binding | 326 |
| Amine-ILs (e.g., [Apbim][BF4]) | Cation | Amine (–NH2/–NH–) | Up to 4× non-funct. | [Bmim][BF4], [Bmim][Tf2N] | High-low–P CO2 capacity | Higher viscosity, regen. energy | Carbamate mechanism; good for low PCO2 | 333 |
| Ether-ILs ([CH3OCH2-mim]X) | Cation | Ether (–O–) | Improved (up to 0.9 mol mol−1) | [Emim][BF4]/[PF6] | Tunable, low volatility | Mainly physical, not chemical | Solubility boosted by the acetate anion | 341 |
| Nitrile-imidazolium ([NC-C3mim][Tf2N]) | Cation | Nitrile (–CN) | Enhanced vs. alkyl ILs | Alkyl-imidazolium ILs | Good selectivity (separation) | Viscosity/stability may vary | Useful for post-combustion CO2 | 341 and 342 |
As shown in (Table 18) and (Fig. 61), the introduction of pyrrolide, phenolate, and hydroxypyridine heterocyclics into the anion structure showcases selective tailoring of non-amino functionalized ILs (non-AFILs). These groups not only enhance CO2 reactivity toward AFILs, but they also mitigate the viscosity issues that often arise from amino functionalization. Hydrophilic –NH2 groups in AFILs tend to form hydrogen-bonded networks with anions, which dramatically increases viscosity and immobilizes mass transfer. Non-AFILs bypass this hydrodynamic issue with three basic design characteristics.
![]() | ||
| Fig. 61 Illustration of chemical absorption mechanisms of carbon dioxide by different organic anions: pyrrolide, phenolate, and hydroxypyridine. | ||
Firstly, the lack of amino groups means that no protonation or hydrogen bonding leads to viscosity surges. Secondly, cation/anion pairs like imidazolium/[BF4]− and phosphonium/[PF6]− have low electrostatic interaction.343,344 Lastly, the presence of heterocyclic anions, which are poor hydrogen bond donors, enhances fluidity, completing.345 These principles have empirically been shown to decrease viscosity relative to AFILs, enabling faster CO2 mass transfer and improving performance in electrochemical applications.346
For instance, [P66614][2-CNPyrr] falls into the category of ILs that have somewhat moderate CO2 capacities with limited change in viscosity. [P66614][PhO], on the other hand, is a phenolate based IL that has been shown to offer balance as a IL with moderate capacity (0.85 mol CO2 per mol IL) and low viscosity (246.7 cP), while hydroxypyridine-based ILs such as [P66614][2-Op] achieve high capacities (∼1.7 mol CO2 per mol IL) but suffer from significant viscosity increases post-capture.333
Mechanistic and experimental evidence reveal that certain heterocyclic anions, for example, [BF4]−, act as hydrogen bond acceptors which are thought to stabilize both the ionic liquid network and the CO2 adducts.347 The use of some non-amino functionalized ionic liquids like phenolate-based [P6614][PhO] has been classified as having moderate layered CO2 absorption ability (0.85 mol CO2 per mol IL) and a reasonable viscosity (246.7 cP), which makes CO2 capture more manageable when considering the fluid dynamics associated with high viscosity solvents. Regarding [P6614][PhO] a note of caution, it is unstable in some cases after it reacts with CO2 which typically increases viscosity and the irreversibility of the adducts limits its practical usage, especially in humid conditions.348,349 Lastly, it should be noted that the non-amino functionalized ILs with tunable chemistry are attractive features for the carbon capture opening frontier. As an example, [P6614]-[2-CNPyrr] has a CO2 affinity that is concerned with the improvement of flow, CO2 capture avoids a 1
:
1 irreversible rate of reaction with CO2, and the viscosity did not change significantly after capture.350–352
![]() | ||
| Fig. 62 The three primary roles of Ionic Liquids in integrated carbon capture and electrochemical conversion: electrolytes, electrolyte additives, or electrode modifiers. | ||
(Table 19) listed various ILs that have been reported in the literature, in addition to many examples in which faradaic efficiencies greater than 80% and energy consumption have been significantly lowered. For example, [Emim][BF4] has been used several times in conjunction with silver or copper electrodes, where it performed admirably due to its ability to stabilize *COOH intermediates and lower the overpotential needed for formate production.353,354
| Electrode/catalyst | Ionic liquid electrolyte | Functionalized? | Product | Faradaic efficiency | Enhancement | Comparison/other electrolytes | Disadvantages | Ref. |
|---|---|---|---|---|---|---|---|---|
| Ag electrode | [Emim][BF4] | No | Formate | >96% | Overpotential <0.2 V; activation energy reduction | Aqueous electrolytes | Not specified | 355 |
| Carbon nanofibers | [Bmim][BF4] | No | Formate | Not specified | Overpotential reduced to 0.17 V; CO2 complexation | Not specified | Not specified | 356 |
| Not specified | [Bmim][NTf2] | No | Formate/carbonate | Not specified | Optimal cation-dependent onset potential | Other ILs | Excess IL disrupts proton flux | 357 |
| Not specified | [Emim][BF4] | No | Formate | Not specified | CO2 pre-activation (binding: −0.36 eV) | Water (binding: −0.11 eV) | Not specified | 358 |
| Not specified | [Bmim][BF4] | No | Formate | Not specified | [Bmim-COOH] intermediate stabilization | Not specified | Not specified | 359 |
| Not specified | [Emim][BF4] | No | Formate | Not specified | [Emim-COOH] pathway via DFT; monolayer formation | Not specified | Not specified | 360 |
| Large electrode (495 cm2) | IL-based ([BF4]−) | No | Formate | 83.90% | Stable selectivity for 10+ hours | Not specified | Not specified | 361 |
| Not specified | [Emim][TFO] | Cation-functionalized | CO | ∼80% | Monolayer formation; minimal IL usage | Acid electrolytes | High viscosity at scale | 362 |
| Porous dendritic Cu | [Emim][BF4] | Cation-functionalized | Formate | ∼75% | CO2 activation; H-atom redirection | Aqueous electrolytes | Concentration sensitivity | 363 |
| Not specified | [Bmim][PF6], [DBU-H][PF6] | Dual-functionalized | CO/formate | CO ∼70%, formate ∼60% | Anion-dependent selectivity: [PF6]− promotes CO/formate | MeCN solvent | Cost-intensive synthesis | 364 |
| Not specified | [Emim][BF4] | Cation-functionalized | Not specified | Not specified | *COOH stabilization via non-covalent interactions | Molecular dynamics simulations | High IL concentrations reduce activity | 365 |
| Large-scale flow cell | Various ILs | Various | CO | 83.90% | Optimized flow rate; stable long-term operation | Water-based | Scalability challenges | 361 |
• greater the solubility and mobility of CO2 (e.g., [Emim][BF4] is a 3× increase versus water)
• reaction of “electroactive” monolayers of cations at the interface [Emim]+ (334 × 10−3 M), reducing activation energy
• transfer of protons will be influenced by anions like [TFO]− chosen to suppress H2 evolution
• selectivity will be influenced by the functionalization of ions necessary to get products such as CO or formate.
There are some critical merits to using this strategy rather than pure IL systems (as seen in Table 20): very low viscosity (≤5 cP as compared to 50–500 cP), good economic performance (≤20% IL weight %), optimized H+ conductivity, and suitability for industrial applications. Both Neubauer et al. and Yuan et al. demonstrated a peak in efficiency depending upon concentration (0.01–0.5 M), with both systems favoring formate and MeCN improved CO selectivity. Functionalized cations such as [Emim]+ completely dominate because OH–CO2 (binding energy of −0.36 eV), and flow reactors were used for 10+ hours at (83%+ efficiency). This method has been proven to resolve viscosity/cost problems, but the key challenges still exist (i.e. all of the other effects with regard to deliquescent interactions of co-additives/solvents; long-term stability; and the optimal triads of screening). Therefore, future work should focus on obtaining operando interface measurements using machine learning with suitable IL. Consequently, hybrid systems still hold the greatest industrial promise for electro-catalytic carbon capture.366–368
| IL used | Cation | Anion | Electrolyte system | Main product | FE | Solvent | IL type | Key findings | Ref. |
|---|---|---|---|---|---|---|---|---|---|
| [Emim][TFO] | Ethyl-methylimidazolium | Trifluoromethanesulfonate | Water-based | CO | ∼80% | Water | Cation-functionalized | Optimal IL concentration (0.334 M) forms monolayers, boosting efficiency with minimal IL usage | 362 |
| [Emim][BF4] | Ethyl-methylimidazolium | Tetrafluoroborate | Water-based | Formate | ∼75% | Water | Cation-functionalized | Activates CO2 and redirects H atoms, enhancing formate on porous Cu electrodes | 363 |
| [Bmim][PF6] | Butyl-methylimidazolium | Hexafluorophosphate | MeCN-based | CO | ∼70% | Acetonitrile | Non-amine | Promotes CO; [DBU-H][PF6] favors formate, demonstrating IL-driven selectivity | 364 |
| [Emim][BF4] | Ethyl-methylimidazolium | Tetrafluoroborate | Simulations | — | — | — | Cation-functionalized | Stabilizes *COOH intermediates via non-covalent interactions, reducing energy barriers | 365 |
| [Emim][BF4] | Ethyl-methylimidazolium | Tetrafluoroborate | Molecular dynamics | — | — | — | Cation-functionalized | High IL concentrations disrupt proton transfer, degrading catalytic activity | 365 |
| Various ILs | Various | Various | Water-based flow cell | CO | 83.90% | Water | Various | Optimized flow rate + IL additives achieve 83.9% CO efficiency with long-term stability | 361 |
• Microenvironment tuning: ILs generate structured interfacial layers, aligning and optimizing local charge distribution and reaction pathways, increasing selectivity369
• Intermediate stabilization: noncovalent interactions (e.g. binding of CO2 to imidazolium) decrease the energy barriers for *COOH formation by 0.3–0.5 eV.330
• Chain length optimization: moderate length (e.g., [Bmim+] C4) N-alkyl chains maximize the surface interaction by balancing increasing thickness with accessibility; longer chains (>C8) significantly decreased efficiency and accessibility to the site330
• Pathway steering: functionalized ILs direct products toward specific outputs (e.g. C2H4 or methanol) by influencing electron/proton transfer370
As summarized in (Table 21), this strategy offers several notable performance improvements:
| IL Used | Electrode material | Main product | Key findings | Ref. |
|---|---|---|---|---|
| Hydrophobic imidazolium ILs | Ag foam | CO | Enhanced CO selectivity/production; alkyl chain length dictates surface accessibility | 371 |
| [Bmim][NO3] | Cu | C2H4 | Reduced *CO → *OCCO barrier; boosted C2H4 efficiency | 372 |
| Phosphonium-IL + imidazole | Au | Formate/methanol | Formate/methanol synthesis at low potentials; intermediate stabilization | 373 |
| Imidazolium SAMs | Au | Ethylene glycol | High activity at low overpotentials; enabled ethylene glycol production | 374 |
| Polymerized IL (PIL) | Graphene | HCOOH | Suppressed HER by >40%; enhanced formate formation | 375 |
| Imidazole-based ILs | Au(111) | Not specified | Vertical CO2 adsorption mode; improved activation energy | 376 |
• CO selectivity: hydrophobic imidazolium ILs toward Ag foam surface increased the production rate of CO from CO2RR
• C2 efficiency: [Bmim][NO3] on Cu lowers the energy barrier for *CO dimerization, giving greater C2H4 yield
• Low energy conversion: phosphonium-ILs toward Au support formate/methanol at record low overpotentials
• Hydrogen evolution reaction (HER) suppression: polymerized ILs on graphene gave > 40% suppression of H2 evolution while increasing efficiency for formate production
From the above table, although IL-modifiers address the volumetric barriers associated with ILs, they still have:
• Stability: capacity to retain IL longevity under high-current operation.
• Synthesis: covalent grafting is still a multi-step functionalization process.
• Structure–activity trade-offs: alkyl chain length must be balanced based on accessibility vs. strength of interaction factors.
Ionic liquid (IL) surface modifiers have multiple distinct advantages relative to the bulk and additive options. In terms of relative IL consumption, bulk IL electrolytes require significant IL amounts (100% consumption) while IL additives require moderate amounts (typically in the range of 5–20%), whereas surface modifiers only need to use modest quantities due to the monolayer-level deployment. In terms of viscosity, bulk ILs increase the viscosity significantly (by 50, 500 cP), with the viscosity increase of IL additives being moderate (viscosity increase of 2–10 cP), and negligible from surface modifiers.377
Dongare et al. have recently investigated the bifunctional ionic liquid (IL) 1-ethyl-3-methylimidazolium 2-cyanopyrrolide ([Emim][2-CNpyr]) dissolved in acetonitrile as a multifunctional electrolyte for integrated CO2 capture and conversion (Fig. 63a).378 This IL has a dual role by its capability for CO2 adsorption and electrochemical activity, which lets it selectively reduce CO on silver electrodes. The system exhibited elevated CO selectivity (>94%) with consistent performance over 12 hours. The addition of 0.1 M [Emim][2-CNpyr] resulted in a positive shift of the CO2 reduction onset potential by 240 mV, indicating a substantial reduction in energy input relative to benchmark electrolytes (Fig. 63b and c). The CO2 capture mechanism is shown through the synergetic effect of imidazolium cation ([Emim]+) and the 2-cyanopyrrolide anion ([2-CNpyr]−). The anion binds CO2 by attacking it with a nucleophile, which makes carbamate-like adducts. The protonated anion can produce a carbene intermediate that interacts with CO2 in an additional step. At the same time, the cation accumulates at the electrode interface, which helps stabilize CO2 adsorbed there and accelerates electron transfer. Operando Spectro-electrochemical methods (SERS and EPR) validated the generation of IL–CO2 adducts, surface-bound CO intermediates, and radical species, hence corroborating the suggested cooperative mechanism. One of the most interesting factors that affects the selectivity is the water content. By adding up to 1 vol% water, the FE of CO increases up to 98%, while adding too much water makes hydrogen evolution more likely. This tunability underscores the importance of the solvent environment in guiding reaction paths (Fig. 63d and e).
Supported ionic liquids (SILs) contribute an additional layer of functionality to IL-modifiers and have the potential to be a scalable and practical approach to eliminating economic and mass-transfer limitations associated with bulk ILs for CO2 capture. SILs also consist of ionic liquids immobilized within porous solids, which is a particularly advantageous sub-approach, where high-surface-area solids such as MCM-41 or Al2O3 as wise support materials, ILs are capable of significantly higher gas–liquid contact while being able to also significantly decrease the volume of ILs needed to achieve the same level of mass-transport, often by +50% volume depending on the complex! This approach is compelling; SILs delivered a 2–3 times improvement in CO2 with absorption rates compared to neat ILs with extended cyclic stability and retained tunable selectivity with target gases. These characteristics make SILs a desirable platform for the industrial-scale carbon capture and integrated conversion approaches.
The improved performance of SILs is due to multiple synergistic processes. The porous supports physically control IL distribution, specifically anchoring the anions (primarily on Al2O3 surfaces), which enhances CO2 adsorption by reducing desorption losses. Materials such as MCM-41 greatly expedite mass transfer by exposing a larger interfacial area where both the gas and liquid can interact, more than doubling the CO2 diffusion rate compared with unsupported ILs. At the optimum IL loadings, around 5 wt%, the supports allow the efficient uptake of CO2 by avoiding pore blockage without filling the pores completely and still allowing a favorable economic and operational conditions. Moreover, advances in poly(ionic liquid) (PIL) networks, such as P[[VBTMA][PF6]], have demonstrated even greater performance improvements, as high as 77% CO2 uptake by weight and CO2/N2 selectivity of 70
:
1, and consistency with no degradation over 100 absorption–desorption cycles.379,380
As summarized in (Table 22), recent studies have explored a range of IL-support configurations and functionalizations, revealing important design considerations for future development.
| Research focus | Key findings | Ref. |
|---|---|---|
| Amino-ILs on MCM-41/Al2O3 | Al2O3 enhances CO2 adsorption via anion anchoring; charge-dependent IL distribution | 381 |
| [P66614][2-Op] on MCM-41 | CO2 absorption rate 2× higher than pure Ils | 325 |
| Organic solvents on MCM-41 | Weaker solvent-support interactions increase CO2 absorption synergistically | 382 |
| Poly(IL) P[[VBTMA][PF6]] | 77% CO2 uptake (wt); 70 : 1 CO2/N2 selectivity; 100-cycle stability |
383 |
| Property | Ionic liquids (ILs) | Aqueous electrolytes |
|---|---|---|
| a Measured under standard conditions without elevated temperature or gas-diffusion electrodes; aqueous electrolytes achieve higher current densities due to lower viscosity, faster CO2 diffusion, and higher ionic conductivity. | ||
| Viscosity (cP) | 50–400 (e.g., ∼300 for [Bmim][PF6]) | ∼0.89 |
| CO2 diffusion coefficient (DCO2, cm2 s−1) | ∼1–8 × 10−6 | ∼2 × 10−5 |
| Ionic conductivity (mS cm−1) | ∼1–10 | >200 |
| Partial current density (mA cm−2) | 10–20a | >100 |
These limitations necessitate a transition towards simpler structures or hybrid systems for electrochemical capture and conversion. Despite these physical hurdles, ionic liquids (ILs) still offer potential economic advantages as electrolytes for CO2 electrochemical reduction (CO2R), especially for producing carbon monoxide, which remains the only economically viable carbon C1 product pathway when appropriately optimized. TEAs indicate that CO-production, at a rate of 100 tons/day, reaches a net present value (NPV) of $13.5 million, and the production of formic acid (HCOOH) reaches $39.4 million. The cost of electricity can highly influence the profitability of these products, with a variation of $0.01 per kWh changing the NPV by ∼$40 million for higher value products like n-propanol. CO could be economically viable, even at low faradaic efficiencies (<50%), as long as the overpotential does not exceed ∼0.4 V. In comparison, for methanol it would require efficiencies greater than 60% and for ethanol, something greater than 90%. For products identified as C1 other (e.g., CH4, syngas), TPC currently exceeds the market prices (e.g., 4.09 € per kg for CH4, market price is 0.18–0.35 € per kg). Scalability in the future must reduce IL synthesis costs, minimize energy-intensive processes, particularly the energy required for the synthesis of fluorinated anions, and improve lifetime stability to reduce high capital expenses.368,383–388
![]() | ||
| Fig. 64 Detailed schematic of integrated CO2 capture and electrocatalytic conversion using choline chloride – deep eutectic solvents (DESs) in a synergistic ICCC process. | ||
The easy preparation of DESs is in stark contrast to the often energy-intensive, expensive synthesis of ionic liquids (ILs), making them a more eco-efficient and technologically and commercially valuable solvent. DESs represent the next-generation solution to the limitations of ILs, as shown in (Fig. 65):
• Simplified synthesis: combining low-cost hydrogen bond acceptors (HBAs; e.g., choline chloride) and donors (HBDs; e.g., urea) at mild temperatures, avoiding complex purification.390
• Eco-efficiency: bio-sourced components (e.g., organic acids) enable biodegradable, non-toxic formulations with minimal environmental impact.
• Cost reduction: raw materials are 10–50× cheaper than ILs, with 80% lower synthesis energy demands.
• Performance parity: DESs match ILs in CO2 solubility (e.g., choline chloride/urea: 0.6 mol CO2 per kg) while enhancing mass transfer via lower viscosity (200–500 cP vs. 500–1000 cP for ILs).391,392
Typically, DESs follow a general formula Cat+X−zY, where Cat+ is a cation (commonly ammonium, phosphonium, or sulfonium), X− is of course a Lewis base (most commonly a halide), and Y is a Lewis or Brønsted acid (associated with a donor). Depending on the exact donor and acceptor within each DES, they can be subdivided into four categories, each providing different physicochemical properties and applications. The versatility of DESs is due to the fact that there can be a substantial number of HBA's and HBD's that can be combined in a DES, and the ability to carefully control attributes of the DES, including its viscosity, polarity, ionic conductivity, and basicity,393,394 and the following (Table 24) shows four different DES systems used in the literature.395–397
| Components | Type | Example components | Notes |
|---|---|---|---|
| Quaternary ammonium salt + metal chloride | Type I | Choline chloride + ZnCl2 | Early studied DESs, often used in electrochemistry |
| Quaternary ammonium salt + metal chloride hydrate | Type II | Choline chloride + CrCl3·6H2O | Like Type I but with hydrated metal salts |
| Quaternary ammonium salt + hydrogen bond donor | Type III | Choline chloride + urea, glycerol, acids | Most common; includes classic DESs and many NADES |
| Metal chloride hydrate + hydrogen bond donor | Type IV | ZnCl2·6H2O + urea | Metal-based, used for specific applications |
(Table 25) presents key quantitative and qualitative properties of representative DES systems, with a focus on Type III (the most common), and notes on electrochemical activity types.
| Formation/components | Type | HBA/HBD | Melting point (°C) | Viscosity (mPa s, 25 °C) | Conductivity (mS cm−1, 25 °C) | CO2 interaction mechanism | Electrochemical suitability/activity type |
|---|---|---|---|---|---|---|---|
| Choline chloride + ZnCl2 | I | ChCl/ZnCl2 | ∼20398 | ∼750399 | 1.0–2.0400 | Limited, depends on metal salt401 | (Electroplating, batteries)401 |
| Choline chloride + CrCl3·6H2O | II | ChCl/CrCl3·6H2O | ∼25398 | ∼800399 | 0.8–1.5400 | Limited, hydration effect401 | (Electroplating, batteries)401 |
Choline chloride + urea (1 : 2) |
III | ChCl/Urea | 12398 | 750399 | 1.2–1.6399 | Strong H-bonding; van der Waals; interaction energy with CO2: −10.65 kcal mol−1,401 | (Wide electrochemical window, electrocatalysis, batteries)401 |
Choline chloride + glycerol (1 : 2) |
III | ChCl/Glycerol | −40 to −30402 | 324399 | 1.1–1.5399 | H-bonding, moderate CO2 affinity403 | (Flow batteries, electrocatalysis)401 |
Choline chloride + ethylene glycol (1 : 2) |
III | ChCl/EG | −66401 | 35399 | 2.0–3.0399 | H-bonding, moderate CO2 affinity403 | (Electrocatalysis, sensors)401 |
| ZnCl2·6H2O + urea | IV | ZnCl2·6H2O/urea | ∼30398 | ∼900399 | 0.9–1.3400 | Partial, less studied401 | (Metal recovery, catalysis)401 |
Mechanistically, DESs interact with CO2 through both physical and chemical interactions. The key role in the overall reaction mechanism is explained by the structuring of the functional groups found in the constituent components of the DES. So, while physical absorption is happening through physical interactions (dipole-quadrupole interactions or van der Waals interactions) that occur with CO2 molecules and the DES matrix, the availability of other properties that can influence the DES (viscosity, polarity, and density) will affect the extent to which CO2 can be absorbed. While the primary focus is the use of DES as electrolyte for capturing and conversion, some other research used the DES in electrodeposition Bohlen et al.404 performed the electrodeposition of indium from 1
:
2 M choline based DES (ChCl
:
EG–1
:
2), employed them as an electrocatalyst for the electrochemical reduction of CO2 to formate.405
(Table 26) demonstrates the way several deep eutectic solvents (DESs) utilize both chemical and physical mechanisms in relation to CO2 capture, with their effectiveness determined by a complex balance of inherent molecular properties and environmental influences. Factors such as viscosity can be critical since lower viscosity allows for greater gas diffusion and CO2 solubility, while high viscosity can prevent mass transfer.406–408 Adjustment of the molar ratio of hydrogen bond donors (HBD) and hydrogen bond acceptors (HBA) may mitigate this source of viscosity limitation.409,410 Generally, increasing HBD content reduces viscosity and increases CO2 uptake. Addition of co-solvents, including water or alcohols, for example, expands the range of operational conditions, while reducing viscosity and assisting with gas transport, but they also add to the risks of compromising the chemical reactivity of the DES solvent.411,412 The presence of specific functional groups in the molecular structure of component one and two strongly influence the capture mechanism; amines will chemically bond CO2 via the formation of carbamate, hydroxy groups can enhance bicarbonate creation, and basic anionic groups like acetate facilitate acid–base interactions.370,407,413,414
| DES components (HBA:HBD) | DES type* | CO2 capture mechanism | CO2 capacity | Additional factors affecting adsorption | Ref. |
|---|---|---|---|---|---|
TPAB : formic acid (1 : 2) |
Type III (choline chloride analog) | Physical and chemical via hydrogen bonding from –OH of formic acid | Higher absorption with 1 : 2 ratio; viscosity at 25 °C: 53.98 mPa s |
Viscosity decrease with higher HBD ratio enhances CO2 solubility; temperature-dependent viscosity | 410 |
DBN : ethylene glycol (varied ratios) |
Type III | Chemical absorption via carbamate and carbonate formation (amine + hydroxyl synergy) | Max 0.17 g CO2 per g DES at optimal ratio | Molar ratio of HBD critical; FTIR and NMR confirm carbamate and carbonate species | 421 |
Methyltriphenylphosphonium bromide : ethylene glycol (1 : 4) |
Type III | Physical absorption (physisorption) | 0.074 mol CO2 per mol DES at 303 K, 12 bar | Temperature and pressure influence solubility | 391 |
Methyltriphenylphosphonium bromide : glycerol (1 : 3) |
Type III | Physical absorption | 0.075 mol CO2 per mol DES at 303 K, 12 bar | Similar to above; solvent polarity and viscosity matter | 391 |
Tetraalkylammonium chloride : 3-amino-1-propanol (1 : 4) |
Type V (amine-based) | Chemical absorption via carbamate formation confirmed by FTIR | Best uptake among studied DESs (exact capacity not specified) | Molar ratio of HBD influences chemisorption efficiency | 422 |
| Choline chloride: proline: ethylene glycol (ternary) | Type V | Chemical absorption via carbamate formation with proline anion | Not quantified explicitly | Synergistic effect of amine and hydroxyl groups; thermal stability and viscosity important | 413 |
Vanillin : 4-oxoisophorone (1 : 3) |
Type III (hydrophobic) | Physical absorption | Comparable to selexol solvent (exact capacity not given) | Hydrophobicity, density >1.0 g mL−1, thermal stability below 420 K | 423 |
| Various IL/DES combinations | Mixed types | Both physical and chemical absorption | Top 10 ILs/DESs ranked by CO2 capture efficiency (specific values vary) | Polarity, viscosity, basicity, and COSMO-RS predicted properties influence performance | 406 |
MTPB : diethylene glycol (1 : 4) |
Type III | Physical absorption | 0.1 mol CO2 per mol DES@303 K, 12 bar | Low viscosity, increased pressure enhances solubility | 424 |
MTPB : glycerol (1 : 3) |
Type III | Physical absorption | 0.075 mol CO2 per mol DES | Hydrogen bonding density affects performance | 424 |
TPAC : ethanolamine (1 : 4) |
Type III | Chemical absorption (enhanced with EA) | 1.4 mol CO2 per kg DES | Functionalization with EA increases solubility to 3.2 mol kg−1 | 425 |
[DBNH][Oxa] : EG (1 : 0.5) |
Type III | Chemical absorption (carbamate + carbonate) | 0.17 g CO2 per g DES | Strong synergy of imino and hydroxyl groups | 426 |
TBAB : 3-amino-1-propanol (1 : 4) |
Type III | Chemical absorption | Not specified | Molar ratio significantly affects solubility | 422 |
| [MEAHCl][MDEA] | Type III | Carbamate + carbonate formation | Not specified | Best performance among amine-based DESs tested | 427 |
| [CHO][Arg] | Type III | Chemical absorption | 0.6046 mol mol−1@288.15 K, 4 bar | Amino acid-based IL, multiple amine sites increase uptake | 428 |
TEAC : acetic acid (1 : 1) + GLY/EA |
Type III | Physical absorption | Decreased compared to unfunctionalized | Addition of third component can reduce capacity | 425 |
| ChCl:MEA | Type III | Chemical absorption | Highest among tested (vs. DEA & MDEA) | High viscosity limits performance despite strong chemisorption | 416 |
| [MEA.Cl]:EDA | Type III | Chemical absorption | 25.2 wt% CO2 @ 0% water | Uptake drops as water content increases (competition for sites) | 414 |
The polarity of DES solvents also contributes to solubility and overall absorption strength; higher polarity generally favors physical absorption, while stronger basicity promotes stronger chemical binding. The hydrogen bonding network present in the DES solvents also facilitates stabilization of CO2-derived interaction intermediates, improving both capacity and selectivity.415,416 Environmental conditions such as moderate temperatures optimize the balance between absorption and desorption, while increased pressure typically enhances CO2 solubility, particularly in DESs that rely more on physical absorption.417,418 Finally, hydrophobicity and density impact both the solvent's regeneration efficiency and its thermal stability. Together, these factors underscore the tunability of DESs and their promising potential for efficient and selective CO2 capture.419,420
A recent study by Halilu et al. investigated bifunctional ionic deep eutectic solvents (DESs) made of diethyl ammonium chloride (DEACI) and diethanolamine (DEA).435 The study found that these solvents could be used as dual-function electrolytes for CO2 capture and electroreduction, with the DEACI-DEA (1
:
3) composition showing the best results (Fig. 66a). This DES had a deep eutectic point of −69.78 °C, good thermal stability, and a long cathodic limit of −1.7 V versus Ag/AgCl. This made it possible to reduce CO2 at −1.5 V with a faradaic efficiency (FE) of 94% and a capture capacity of 52.71 mol L−1 after 350 s of sparging (Fig. 66b and c). Conventional aqueous electrolytes, on the other hand, usually have CO2 solubilities < 0.03 mol L−1 at room temperature and only sometimes reach 40–60% FE because the hydrogen evolution process (HER) is more common at negative potentials. Ionic liquids can also have high FE (70–90%), but they usually have low CO2 solubility (∼0.2–0.4 mol L−1) and high viscosity, which makes it hard to move mass and scale up (Fig. 66d and e). DEACI–DEA, on the other hand, has a strong CO2 uptake and an efficient conversion while keeping HER low. Electrochemical impedance spectroscopy demonstrated CO2 chemisorption by a decrease in double-layer capacitance from 8.76 × 10−9 F to 3.15 × 10−9 F. Simultaneously, COSMO-RS analysis indicated bifunctional interactions of both HBA and HBD sites with CO2 through n-orbital overlap in the non-polar region (Fig. 66f). Chronoamperometric studies revealed an initial diffusion-limited regime succeeded by a steady state in which capture, and conversion reached equilibrium, thereby establishing a direct correlation between absorption capacity and electroreduction kinetics. These results collectively demonstrate that, in contrast to aqueous or ionic liquid systems, DEACI-DEA provides a distinctive equilibrium of solubility, stability, and selectivity, thereby establishing bifunctional deep eutectic solvents (DESs) with enhanced cathodic windows as a logical design framework for next-generation CO2 capture and electro conversion technologies.
Based on (Table 27), Deep eutectic solvents (DESs) possess numerous electrochemical advantages over traditional aqueous electrolytes for CO2 reduction applications. As mentioned above, there are some cases when DESs have marginally lower ionic conductivities than aqueous media, the larger electrochemical window (often more than 3 V) when using DESs permits the application of higher overpotentials for CO2 reduction without stress from solvent degradation.430,436
DES used (HBA : HBD, ratio) |
Electrode | Main product | FE (%) (DES vs. aq.) | Current density (mA cm−2) | Conductivity (DES/aq.) | Conventional electrolyte (comparison) | Electrochemical advantage | Ref. |
|---|---|---|---|---|---|---|---|---|
Choline chloride : ethylene glycol (1 : 2) |
Au sheet | CO | 81.8% (DES, not compared to aq.) | 1.1 (at −1.6 V) | 6.8 mS cm−1 (DES) | 0.1 M TBAPF6/DMF | Lower overpotential, higher CO2 solubility, selective CO production | 436 |
Choline chloride : urea (1 : 2) |
Ag foil | CO | 96% (DES, not compared to aq.) | ∼4.8 (at −0.884 V) | 34.5–131.4 mS cm−1 (with KCl) | 0.5 M KHCO3 | High selectivity for CO, HER suppression | 429 |
Choline chloride : ethylene glycol (1 : 2) |
Ag foil | CO | 78–98.8% (in acetonitrile) | 0.4–20 (in acetonitrile) | Not specified | Water, Acetonitrile, Propylene Carbonate | High CO selectivity in aprotic media, tunable viscosity/selectivity | 437 |
Choline chloride : urea (1 : 2) |
Ag NPs/GDE | CO | 94.1% (DES, not compared to aq.) | 11.6 (at −0.83 V) | 34.5–131.4 mS cm−1 (with KCl) | 0.5 M H2SO4 | High selectivity, improved current density with salt | 436 |
Choline chloride : ethylene glycol (1 : 2), choline chloride : urea (1 : 2) |
Au, Ag, Cu, Zn | CO, HCOOH | 15.8–98.8% (varies) | 0.1–20 (varies) | 1.5–1244 cP (viscosity) | Aqueous, acetonitrile, propylene carbonate | Wide potential window, tunable selectivity, high CO2 solubility | 430 |
Choline chloride : urea (1 : 2) |
Roughened Ag foil | CO | 96% | ∼4.8 at −0.884 V vs. RHE | 0.1 M KHCO3 | HER suppression, surface restructuring | HER suppression, surface restructuring | 438 |
Choline chloride : urea (1 : 2) |
Ag | CO | 90% | Not specified | 0.5 M KHCO3 | High selectivity, low overpotential | High selectivity, low overpotential | 430 |
Choline chloride : urea (1 : 2) |
Ag | CO | 92% | Not specified | 0.5 M KHCO3 | High selectivity, improved current density | High selectivity, improved current density | |
Choline chloride : urea (1 : 2), with KCl |
Ag-based GDE | CO | Not directly reported; higher jCO with DES/KCl | Not specified (improved with KCl in DES) | Not specified | Aqueous KOH, KCl, Emim Cl | Enhanced CO2 absorption, improved current density | 437 |
Choline chloride : ethylene glycol (1 : 2), imidazolium chloride:EG |
Ag | CO | High FE for CO (exact % not specified) | Not specified | Not specified | RTILs, aqueous | Non-toxic, cost-effective, improved solubility/selectivity | 439 |
ZnCl2 : EA (1 : 4), CoCl2 : EA (1 : 4); DEACl : DEA (1 : 3) |
Single-atom Ag, Ag | CO2 | Up to 94% (DEACl:DEA 1 : 3) |
Not specified | Up to 36 200 µS cm−1 (ZnCl2/EA) |
Not specified | High CO2 absorption, unique interfacial phenomena, bifunctional sorption, wide cathodic window | |
| MEAHCl:MDEA | Ag | CO | 71% | Not reported | Not reported | Not reported | Amine-functionalized DES promoted CO2-to-CO conversion | 429 |
ChCl : ethylene glycol (1 : 2) |
In | Formate | Up to 95% | Not reported | Not reported | Not reported | Selective formate production in DES medium | |
[Ch][Cl] : urea (1 : 2), 50 wt% in H2O |
Roughened Ag foil | CO | 96% vs. lower in aq. KHCO3 | ∼4.8 | 34.5 mS cm−1 (DES), 131.4 mS cm−1 (DES + KCl) | 0.5 M KHCO3 | Restructures Ag surface, suppresses HER | |
[MEAH][Cl] : MDEA (1 : 4), 0.4 M in H2O |
Ag foil | CO | 71% vs. lower in water | 10.5 | Not explicitly given | Aqueous only | Amine-DES enhances COOH* intermediate stabilization | |
[Ch][Cl] : EG (1 : 2), 0.1 M in H2O |
Ag foil | CO | Up to 94.1% | 11.6 (w/KCl: 22.1) | 34.5 → 131.4 mS cm−1 (w/KCl) | Aqueous H2SO4 | Addition of KCl doubled current density with same FE | |
[Ch][Cl] : urea (1 : 2), 2 M in H2O |
Ag NPs/GDE | CO | 94.10% | 11.6 | Not directly reported | Aqueous | KCl enhances conductivity and performance | |
[Ch][Cl] : EG (1 : 2), 1 M in acetonitrile |
Not specified | CO | 98.80% | 20 | Not specified | — | High FE in aprotic solvent system | |
[Ch][Cl] : EG (1 : 2), neat |
Au metal sheet | CO | 81.80% | 1.1 | Not reported | — | High selectivity even without co-solvent | |
[Ch][Cl] : EG (1 : 2), in propylene carbonate |
Cu0.3Zn9.7 on Cu foam | CO | 94.90% | ∼16 | Not specified | 0.1 M H2SO4 | Enhanced CO selectivity on Cu-based alloy |
DESs have consistently produced higher faradaic efficiencies for target products such as CO, formate, and ethylene, due in part to their higher solubility of CO2, as well as providing a more stable medium for intermediates formed throughout the reaction, which benefit from the networks of hydrogen bonding exhibited in these solvents. The DESs have also improved product selectivity and stability when subjected to reaction conditions compared to their aqueous counterparts, leading to less decay of phase separation and electrode damage over cyclic runs while DESs can be prepared readily in a single step from low-cost precursor materials, and do not require a purification step.429,440
| DES composition | Polymer used | Polymer concentration | CO2 capture performance | Conditions |
|---|---|---|---|---|
| Choline chloride-glycerol-citric acid | Chitosan | 1% w/w | 768.74 mmol CO2 per kg DES | 10 bar pressure |
| Choline chloride-glycerol-citric acid | — | 0% w/w | 110.11 mmol CO2 per kg DES | Atmospheric pressure, CO2 flow |
| Tetrabutylammonium bromide-PEG 200 | None | N/A | 120.44 mmol CO2 per kg DES | Atmospheric pressure, 25 °C |
The ternary deep eutectic solvent (DES) composed of choline chloride, glycerol, and citric acid, when combined with 1% w/w chitosan, achieved a remarkable CO2 capture capacity of 768.74 mmol kg−1 at 10 bar, significantly outperforming the same DES without chitosan, which captured only 110.11 mmol kg−1 at atmospheric pressure. This enhancement is attributed to chitosan's amino groups, which facilitate additional chemical adsorption of CO2 under elevated pressure. In comparison, a standalone DES of tetrabutylammonium bromide and polyethylene glycol (PEG 200) captured 120.44 mmol kg−1 at ambient conditions. Notably, among available studies, only Nunes (2021) explores a DES-polymer composite system, highlighting the unique role of chitosan in improving CO2 capture performance, whereas most other research focuses on additives such as amines or support materials such as silica, rather than incorporating polymeric matrices.
To boost the kinetics of CO2 electrochemical conversion, we need to optimize the reactor configuration and the operating conditions. Gas diffusion electrodes (GDEs) typically used in flow cells allow direct CO2 to contact the catalyst interface, drastically boosting mass transport while reducing the ubiquitous diffusion limitations found in other liquid-phase reactors, as shown in (Fig. 67).443 By pressurizing the electrochemical cell, the solubility of CO2 is significantly increased in the reaction medium due to Henry's law, which maximizes the availability of CO2 at the interface and/or reduces the kinetics as detailed in (Table 29).444 With regards to gas solubility and kinetics, lowering the temperature also has advantages, but greater gains may need to be weighed against lower reaction rates at lower thermal energies.445 Additionally, some studies have reported that tuning ionic strength or salinity of the electrolyte will impact the CO2 capture and transport across the two-phase interface, but at times, the results are conflicting or complex.446 Flow rate, while not specifically noted in the literature, is critical for maintaining the available CO2 supply and removing the gaseous product, in turn affecting kinetics and selectivity. Higher flows will optimize the mass transfer but will decrease the residence times, so greater effort may need to be directed to optimizing flow rate depending on scale and design.443
![]() | ||
| Fig. 67 A schematic overview of a supporting electrolyte, detailing its core components and the key physicochemical properties. | ||
| Parameter | Kinetic impact |
|---|---|
| Gas diffusion electrodes (GDEs) | ↑ Mass transport; ↑ Stability (∼450 mA cm−2 for 200+ hours) |
| Pressure optimization | ↑ CO2 surface coverage; ↑ Formate selectivity (up to 50 bar) |
| Flow rate tuning | ↑ CO2 supply; ↓ Blockage (optimal: 10–20 sccm) |
| Catalyst nanostructuring | ↑ C2+ selectivity; ↑ Current density (e.g., Cu nanowires: 77.7% FE at 233.2 mA cm−2) |
| Reactor configuration | ↓ Ohmic resistance; ↑ Efficiency (e.g., zero-gap cells at 10 bar) |
| Temperature management | Balances CO2 solubility/reaction kinetics (20–40 °C) |
Molten salt electrolysis, utilizing an anhydrous electrolyte that focuses on carbon creation, can yield a singular solid carbon product with elevated current efficiency, thereby circumventing intricate byproducts that necessitate challenging or many separations. Moreover, the in situ conversion of CO2 into value-added products obviates supplementary expenses following carbon capture, such as CO2 transportation fees, disputed and uncertain storage, and maintenance expenditures, etc.448,449 A molten salt CO2 electrolysis facility is anticipated to generate a net profit of $50
000 per ton of captured CO2 for a power station when the final electrolysis product is carbon nanotubes (CNTs).450 A common technique for synthesizing carbon nanotubes (CNTs) is chemical vapor deposition (CVD), requiring at least 1440 MJ and producing 28.55 kg of CO2 for the generation of one gram of CNTs.451,452 Thus, this profit and these advantages can promote the expansion of the molten technique for prospective plants and improve the execution of carbon capture in conventional power plants, surpassing the financial drawbacks linked to the aforementioned technologies, as shown in (Fig. 68).
![]() | ||
| Fig. 68 Process schematic of molten salt electrolysis for integrated CO2 capture, electrocatalytic conversion, and carbon nanomaterial production with rate-matched kinetics. | ||
The method of capturing CO2 using molten salt and electrochemical conversion is efficient and advantageous, as it facilitates the immobilization of CO2 and its transformation into valuable goods. The molten salt electrochemical unit features a straightforward design comprising an insulated electrolyzer, electrolyte, heating unit, cathode, and anode. The absence of additional equipment facilitates ease of usage and management.453,454 Secondly, the molten salt possesses an extensive electrochemical window, and no side reactions occur during operation.455,456 Third, electrons serve as the reducing agent for CO2 reduction via molten salt. The effective current density during electrolysis can be adjusted to regulate the conversion rate of CO2 into solid carbon compounds.457,458 The molten salt electrolyte primarily consists of carbonate, which is inexpensive to produce and can be reused, hence minimizing operational costs.457,459 Ultimately, carbonate electrolyte exhibits high solubility in CO2 and is highly effective in capturing CO2.460
| CO2g + O2−→ CO32− | (1) |
• The 4-electron reaction (low to moderate temperatures):
| CO32− + 4e− → Cs + 3O2− | (2) |
• The 2-electron reaction (higher temperatures):
| CO32− + 2e− → COg + 2O2− | (3) |
| 2O2− → O2g + 4e− | (4) |
| Molten salt | Alkali metal (V) | Carbon (V) |
|---|---|---|
| CaCO3 | −3.033 | −1.349 |
| Li2CO3 | −2.964 | −1.719 |
| BaCO3 | −3.069 | −1.992 |
| Na2CO3 | −2.546 | −2.551 |
| K2CO3 | −2.612 | −3.083 |
Various cations in carbonates produce distinct carbon nanostructures. Li+ and Ba2+ are believed to facilitate the formation of carbon nanotubes, but K+ inhibits the growth of carbon nanostructures.472 Recent studies indicate that electrolytes containing over 50 wt% Na or more than 30 wt% K carbonates inhibit the growth of carbon nanotubes (CNTs) while accelerating the formation of carbon nano-scaffolds (CNS).473
The anode serves a pivotal function in molten salt electrolysis by catalyzing oxygen evolution and ensuring that O2− ions do not accumulate within the electrolyte.492 Since free O2− ions are not stable in molten salts, they rapidly react with dissolved CO2 or metal ions, forming carbonate ions (CO32−) and metal oxides.493,494 To maintain efficient carbon deposition at the cathode, it is essential that O2− ions are removed promptly, which in turn sustains the necessary electrical current for the process as illustrated in (Table 31).
| Electrolyte | T (°C) | Cathode | Anode | Current density | Products | Ref. |
|---|---|---|---|---|---|---|
| Li2CO3 | 770 | Galvanized steel; Ni–Cr | Ni–Cr; galvanized steel | 1 A | Multi-walled carbon nanotubes (MWCNTs) | 482 |
| Ta2O5–CaCl2–CaO | 650 | Ni | Graphite | 0.2–1 A cm−2 | Carbon particles | 490 |
| Li2CO3–Li2O | 770 | Cu | Ir–Pt | 0.2 A cm−2 | Carbon nano-onions; CNTs | 495 |
| Li2CO3–Li2O–CaO–H3BO3 | 770 | Muntz brass sheet | Nichrome sheet | 0.2 A cm−2 | Carbon nanotubes (CNTs) | 496 |
| Li2CO3–Na2CO3–K2CO3–H3BO3 | 670 | Muntz brass sheet | Inconel | CNTs | 473 | |
| Li2CO3–Na2CO3–K2CO3 | 450–650 | Ni | SnO2 | 0.2–4 A g−1 | Activated carbons | 487 |
| Li2CO3–Li2O | 770 | Muntz brass as | Inconel 718; Nichrome; Incoloy | 0.5 A | Fe3C; CNTs | 463 |
| LiCl–Li2CO3–LiBO2 | 550 | Ni | Graphite | 25–100 mA cm−2 | CO | 497 |
| LiCl–Li2CO3–LiBO2 | 550 | Ni | Graphite | Carbon nanofibers (CNFs); CO | 498 | |
| Li2CO3 | 730 | Galvanized steel | Pt | Graphene; CNTs | 488 | |
| Li2CO3–K2CO3–Na2CO3 | 650 | NiO–Co3O4 | Ni10Cu11Fe | 10 mA cm−2 | NiCo@g-c powder | 485 |
| Li2CO3–K2CO3–Na2CO3 | 650–750 | Ni | Pt | 5–100 mA cm−2 | Graphite | 499 |
| Li2CO3–Na2CO3 | 750 | Brass | Inconel 718 | 200 mA cm−2 | CNTs | 500 |
| Li2CO3 | 750 | Ni | SS | 7.5 A | Carbon sphere | 501 |
| NaCl-CaCl2-CaO | 750 | GeO2 | Graphite | 2000 mA g−1 | Ge@CNTs | 486 |
| Li2CO3–Na2CO3–K2CO3 | 450 | nickel foam | Glassy carbon | 500 mA g−1 | Porous carbon | 491 |
| Li2CO3 | 780 | nickel foam | Glassy carbon | 600 mA g−1 | Crystalline nano-graphite | 502 |
| Li2CO3-K2CO3-Na2CO3 | 500 | Galvanized Fe wire | Ni wire | — | Honeycomb carbon nanostructure | 503 |
| Na2CO3-K2CO3 | FeNi foam | Ni10Cu11Fe alloy | 100 mA cm−2 | CO | 504 |
Peng et al. illustrated how the ZnO ratio affects morphology and the percentage of carbon nanotubes (CNTs) in cathodic carbon products.506 They found that using Li2CO3 electrolyte with 1% ZnO supports CNT formation. This is likely because ZnO reduces the energy barrier for both nucleation and carbon deposition. The results show that the ZnO content significantly affects CNT growth; with only less than 50% of CNTs observed in Li2CO3 electrolyte containing 0.5% and 2% ZnO, compared to over 90% in the 1% ZnO setup, as shown in (Fig. 70d–f). Additionally, in a Li2CO3–Na2CO3 (1
:
1 weight ratio) system, adding 1% ZnO results in carbon products with more than 80% CNTs. This evidence indicates that it is possible to use more cost-effective electrolytes for CNT production.
Yu, R. et al. developed a novel Ge@CNT composite material to address the limitation of carbon-based anodes in lithium-ion batteries (LIBs) regarding charge capacity.486 The incorporation of germanium and carbon nanotubes significantly enhances the battery's overall performance. The synthesis occurs in a heated mixture of NaCl, CaCl2, and CaO, which additionally contains GeO2. The reaction initiates when GeO2 interacts with ionized Ca2+ in the molten salt. This produces a liquid CaGe alloy. This alloy phase facilitates the development of carbon nanotubes by accelerating the process. (Fig. 71a and b) illustrates the completed assembly, featuring several germanium nanoparticles embedded directly into the carbon nanotube matrix. This unique configuration integrates germanium's capacity to retain substantial lithium with the stable, conductive framework of carbon nanotubes. This addresses the common issues associated with carbon. In addition, various M@CNTs, such as Sn@CNTs, Zn@CNTs, and Fe@CNTs, were synthesized, and CO2 was reduced in molten salts.483 The mechanisms by which these three M@CNTs evolve are fundamentally different from the nucleation process of liquid metals. (Fig. 71c) illustrates the electrochemical reduction of CO2 in an inexpensive, calcium-containing molten salt. This method effectively generates CNTs and M@CNTs via a CaC2-mediated process. In the synthesis of metal-free carbon nanotubes, calcium carbonate in the melt is first converted into calcium carbide. Calcium carbide (CaC2) acts as a precursor for the fabrication of carbon nanotubes (CNTs) by the decomposition of calcium carbonate (CaCO3). The CaO and CO2 cycle subsequently replenishes the consumed CaCO3. In the production of M@CNTs (Sn@CNTs, Zn@CNTs, and Fe@CNTs), MOx (metal oxides SnO2, ZnO, and FeO) and CaCO3 are reduced to liquid metals and CNTs, respectively. The liquid metals are subsequently introduced into the internal cavities of the CNTs (Fig. 71d). Sn@CNT shows a significant capacity of 510 mAh g−1 at a current density of 1000 mA g−1 due to the synergistic interaction between the Sn core and the CNT shell. These techniques illustrate the strategic application of molten salt for the sequestration and transformation of CO2. They also promote the advancement of novel CNT composites and highlight the adaptability of this technology for production.
Carbon nano-onions are a special type of carbon nanostructure that is made up of many layers of fullerenes. In the past, these structures were made by putting nanodiamonds through pyrolysis at very high temperatures, often reaching 1700 °C, which made the process use a huge amount of energy. Liu et al. demonstrated an alternative approach to capture and electrochemically reduce CO2 in a pure Li2CO3 electrolyte with six molal Li2O. Their tests showed that using galvanized copper as the cathode and platinum flakes as the anode produced about 97% yield of carbon nano-onions. When a nickel sheet was used as the anode, it facilitated carbon nanotubes forming instead of nano-onions. The results show that the type of carbon nanostructure that is made depends on both the electrode material and the ratio of molten salt. Using electrodes and electrolytes that don't contain nickel and are high in Li2O generally makes more sp3 defects happen in the solid carbon that forms at the cathode. Adding more sp3 character makes the carbon layers bend more, which enhances the production of carbon nano-onions, as shown in (Fig. 72a and b).495 Rui et al. discovered that the alkalinity of the electrolyte, electrode substrate, and current density play a crucial role in the growth of carbon nanocoils (CNCs) on graphite electrode in Li2CO3–Na2CO3–K2CO3–0.001 wt% Li2O as a molten salt, and the alkalinity of the molten salt electrolyte induced specific structural defects in carbon, leading to the formation of coiled structures in a controlled manner507 as shown in (Fig. 72c and d). Interestingly, through scanning electron microscopy, the in situ mechanical properties were measured, and it was found that the shear modulus and the spring stiffness of the electrolytic CNCs are far larger than those of CVD-derived CNCs and close to the theoretical values. Noting that (Table 32) presents the techno-economics of carbon nanotubes produced by different methods.
| Parameter | Molten salt electrolysis | CVD | Arc discharge | Laser ablation |
|---|---|---|---|---|
| Production cost | $0.05–0.20 per g SWCNs | $0.366–$1.7 per g SWCNs | $100–$150 per g SWCNs | $100–$1000 per g SWCNs |
| Scalability | High (compatible with industrial-scale reactors) | High (dominant commercial method) | Low (batch process) | Very low (research-scale) |
| Energy consumption | High (750–900 °C, electricity-intensive) | High (900–1000 °C, hydrocarbon cracking) | Very high (arc plasma) | Extremely high (laser systems) |
| Raw material cost | Low (uses CO2 or graphite) | Moderate (hydrocarbons, catalysts) | Moderate (graphite electrodes) | High (graphite targets) |
| Environmental impact | CO2-negative potential | High GHG emissions (methane/ethane use) | Moderate (CO2 from energy) | High (energy-intensive) |
| Market viability | Emerging (profitable at scale) | Mature (dominant market share) | Limited (niche applications) | Rare (specialized uses) |
| Material class | Capture capacity (273–298 K, ∼1 bar) | Textural/binding metrics | CO2RR selectivity (FE) | Current density & kinetics | Stability/TRL insight | Ref. |
|---|---|---|---|---|---|---|
| POPs/CTFs | – PHCTF-1a/-4 : 30–52 cm3 g−1 CO2 at 273 K |
– SBET ≈ 1200–1300 m2 g−1 | – Metal-free CTF: FECO ≈ 82% F-CTF: FECH4 ≈ 99.3% | – NiPor-CTF: jCO ≈ 12.8 mA cm−2 | – Good capture at flue-gas PCO2 | 65, 66, 82, 84–86, 88, 90–92, 103 and 105 |
| – N-rich CTFs (PCBZL, CTF-CSU41): 30–52 cm3 g−1 at 273 K. | – Vmicro = 58–79% | – Ni-CTF: FECO ≈ 90%; NiPor-CTF: FECO ≈ 92.3% | – Ni–N/CNT@CTF: jCO ≈ 201 mA cm−2 | – Ni–N/CNT@CTF approaches industrial j but humidity and long-term oxidative stability remain limiting; TRL ≈ 3–4 | ||
| – Qst ≈ 24–45 kJ mol−1 (favourable for 10–15% CO2) | – Ni–N/CNT@CTF: FECO ≈ 98% | – ΔG*COOH ≈ 0.58–0.59 eV | ||||
| – Tafel ≈ 56–86 mV dec−1 (vs. ≥0.85 eV and ∼130 mV dec−1 for Ni-TPP) | ||||||
| POPs/CMPs | – Co-CMP: 79.3 mg g−1 | – Co-CMP: SBET ≈ 965 m2 g−1, Vtot ≈ 2.81 cm3 g−1 | – CNT@CMP(CoPc–H2Pc): FECO ≈ 97% | – CNT@CMP(CoPc–H2Pc) & CMPANI-3: jCO > 200 mA cm−2 | CMPs can reach industrial j and high FE when combined with CNT backbones and proton-relay ligands; stability and flue-gas tolerance still underexplored; TRL ≈ 3 | 113, 114, 117, 128 and 130 |
| – Al-CMP: 76.5 mg g−1 | – Al-CMP: 798 m2 g−1, 1.41 cm3 g−1; capacity tracks Vtot and metal–CO2 interactions more than SBET | – CMPANI-3: FECO ≈ 97%; CMP-(bpy)20–Mn: FECO ≈ 0.4% (HER-dominated). | – TOF up to 9.8 × 104 h−1; CMP-(bpy)20–Mn: requires −1.6 V for negligible CO. | |||
| – Parent CMP: 71.0 mg g−1 at 298 K, 1 bar (similar to MOF-177, NOTT-112) | ||||||
| COFs | – TPE-COF-II: 118.8 cm3 g−1 (23.2 wt%) at 273 K | – RICE-5: porosity 94%, density 0.094 g cm−3 | – CoPc-PI-COF: FECO ≈ 96–97% | – CoPc-PI-COF: TOF up to 2.2 s−1, TON ≈ 2.8 × 105 | COFs offer high FE and tunable binding, but hydrolytic stability, crystallization yield, and limited j at low PCO2 restrict ICCC deployment; GDE integration and robust linkers are required; TRL ≈ 2–3 | 153, 158, 174, 176 and 181 |
– RICE-5 : 50 cm3 g−1 at 273 K |
– HEX-COF-1: SBET 1214 m2 g−1, Qst ≈ 42 kJ mol−1 | – Co-TTCOF: FECO ≈ 99.7%; PA-Co-COF: FECO ≈ 86.97% from 15% CO2 | – Co-TTCOF: TOF ≈ 1.3 s−1; PA-Co-COF: TOF 1208.8 h−1 | |||
| – COF-102/103: up to 27 mmol g−1 at 298 K | – COF-300-SO3H: 6.23 mmol g−1 CO2 and CO2/N2 selectivity 393 vs. 10–31 for other functional groups | – Cu-COF+-Pd: ≈95.5% FECO+CO2− | – Most examples operate at j ≲ 50–100 mA cm−2 | |||
| Zeolites | – LEV: 5.81 mmol g−1 at 0 °C | – Low Si/Al and high Na+/Ni2+ densities enhance uptake | – CdO@Zn@Y: FECO > 90% at −0.8 V; SnCuxO2+x@MFI: high FECH4/FEC2H4 at elevated j | – CdO@Zn@Y stable for 120 h; zeolites generally >1000 h in capture | Zeolites are capture-mature (TRL 8–9) with excellent stability; as ICCC catalysts, they need conductive, hierarchical GDE designs. | 199–201, 221, 226 and 234 |
| – LTA: up to 3.7 mmol g−1 at 25 °C after Si/Al optimization | – Hierarchical LTA reduces adsorption/desorption time by 29–92 s and regeneration T by 13 °C | – Electrochemical systems are still mostly lab-scale | ||||
| – CO2/N2 selectivity up to ≈80–84 | – Conductivity remains a bottleneck. | |||||
| MOFs | – HKUST-1/MOF-74: up to ∼10 mmol g−1 at high P | – High SBET and open metal sites | – Ag-MOF-NH2: FECO 96–97% at 355–380 mA cm−2 from 15% CO2 | – MOF GDEs reach j ≳ 200–380 mA cm−2 | MOFs can deliver ICCC-level rates via local CO2 enrichment but require robust, hydrophobic/conductive frameworks for long-term operation; TRL ≈ 3–4 | 243, 266–270 and 293 |
| – CALF-20 MMM: 3.97 mmol g−1 with ≈4.5× selectivity vs. N2/O2 at 298 K | – CALF-20 stable under humid DAC-like conditions. | – CALF-20-PGDE: CO FE ≈ 95% from 10% CO2 | – Bi-HHTP gives FEHCOOH ≈ 90–93% with modelled cost ≈0.74 $ kg−1 | |||
| – Cu-MOF GDEs: FEC2H4 ≈ 49%, JC2H4 ≈ 220 mA cm−2 at 1 A cm−2 | – hydrolysis often limits lifetime to <100 h | |||||
| Metal oxides/hybrids | – Amine-oxide systems capture CO2 as carbamates/bicarbonates (DEA–SnOx/C stable up to 50% CO2) | – Strong chemisorption | – DEA– SnOx/C: FEHCOO− ≈ 84.2% | – DEA–SnOx/C: jHCOO− ≈ 6.7–7.9 mA cm−2 | Oxide-based DFMs clearly reduce capture energy versus thermal stripping but amine-based systems have low j and degradation; oxide solid-state reactors are closer to TE targets but face poisoning and capital-cost issues; TRL ≈ 3–5 | 294–299 |
| – Limited physical porosity | – Solid-state oxide reactors: C2 FEs ≈ 34–68% | – Solid-state capture j up to 440 mA cm−2 with costs ≈33–83 $ t−1 CO2 | ||||
| – Capture capacity defined by amine loading | ||||||
| Amines | – Typical 30 wt% MEA: 0.4–0.5 mol CO2 per mol amine | – Carbamate formation | – MEA/Ag: FECO ≈ 72% at 50 mA cm−2 | – j usually ≤50 mA cm−2 in H-cells | Amines are capture-mature (TRL4) but electrochemically limited by conductivity, HER, and degradation; useful for energy savings but not yet superior in productivity to gas-fed CO2RR | 312–320 |
| – High capacities at 40–60 °C | – Regeneration energy ≈3 GJ t−1 CO2; oxidative/thermal degradation above ≈100–110 °C | – AMP-based systems: FEHCOO− ≈ 40–50% | – Best flow systems approach ≈200 mA cm−2 | |||
| – Ni–N/C in MEA: FECO ≈ 65% | – Integrated schemes can save up to ≈44% capture energy versus thermal stripping | |||||
| Ionic liquids | – Physical ILs: ≤0.5 mol CO2 mol−1 at 1 bar | – Strong, tunable interactions but high viscosities (50–1000 cP) and cost | – Neat imidazolium ILs: FECO/HCOO− ≥80–96% | – Strong overpotential reduction (≈0.2–0.24 V) but often limited j due to viscosity in neat Ils | ILs excel as interfacial modifiers/additives rather than bulk electrolytes; cost, viscosity, and toxicity remain barriers for large-scale ICCC; TRL ≈ 3–4 | 321, 330, 337, 338 and 389 |
| Reactive ILs (e.g. [P66614][AA]) up to 1.6–2.0 mol mol−1 | – Non-fluorinated, heterocycle ILs show better viscosity–capacity trade-offs | – IL additives (0.01–0.5 M [Emim][BF4]/[TFO]): FE ≈ 75–80% | – Additive/surface-modifier modes maintain aqueous-like j while improving FE | |||
| – [Emim][2-CNPyrr]: FECO > 94–98% | ||||||
| DESs | – ChCl:urea/EG: ≈0.6 mol kg−1 | – Viscosity 200–800 cP (lower than many ILs but higher than water) | – DEACl:DEA: FECO ≈ 94% | – j typically 4–20 mA cm−2 | DESs offer green, low-cost, high-FE media but need GDEs/pressure and polymeric hybrids to reach ≥200 mA cm−2; TRL ≈ 2–3 | 390, 402, 407, 408, 429–435 and 439 |
| – PRIDES: up to 769 mmol kg−1 | – H-bond network controls CO2 speciation and transport | – ChCl:urea-based systems: FECO 90–98% at low j | – Rct lower than in KHCO3, but still limits high-rate operation | |||
| – DEACl:DEA: 52.71 mol L−1 equivalent loading | – Stability is good over tens of hours | |||||
| Molten salts | – Li2CO3/Li–Na–K carbonates: CO2 solubility up to 0.835 mol CO2 per mol Li at 723 K | – Toper 550–900 °C; fully inorganic, excellent stability; strong chemisorption via CO32− species | – MSCC-ET: current efficiency >80–93% for C or CO; CNT products with near-100% carbon selectivity | – j typically 0.2–1 A cm−2; SWCNT cost 0.05–0.20 $ g−1 with effective profit ≈50 k$ t−1 CO2; >100 h operation demonstrated | Molten salts uniquely enable CO2-negative carbon materials at industrial current densities and flue-gas tolerance, but high T and corrosion limit integration with low-T ICCC; TRL ≈ 4–5 for MSCC-ET | 447, 470, 472 and 507 |
| Material class | T (°C) | P (bar) | PCO2 range | H2O tolerance | SOx/NOx tolerance | Typical jmax (mA cm−2) | Ref. |
|---|---|---|---|---|---|---|---|
| POPs/CTFs | 25–100 | 0.1–5 | 0.01–0.15 | Moderate | Low | 10–50 (up to 201 for Ni–N/CNT@CTF) | 62, 82, 91 and 108 |
| COFs | 25–80 | 0.1–10 | 0.01–0.20 | Poor (hydrolysis) | Low | 5–100 | 149, 164 and 175 |
| MOFs | 25–150 | 0.1–40 | 0.01–1.0 | Poor–moderate (framework-dependent) | Variable | 200–380 (GDEs) | 247, 261–263, 266–270 and 273 |
| Zeolites | 25–500 | 0.1–20 | 0.01–0.15 | Excellent | Excellent | 100–440 (in integrated cells) | 183, 185, 199–201, 212 and 213 |
| Metal oxides | 25–400 | 1–10 | 0.10–1.0 | Good | Moderate | 6–200 | 294–299 |
| Amines | 40–120 | 0.1–2 | 0.01–0.15 | Excellent | Poor (degradation) | 20–200 | 305, 309, 312 and 319 |
| ILs | 25–100 | 0.1–93 | 0.01–1.0 | Good (hydrophobic ILs) | Moderate | 10–100 | 322, 323, 325, 356 and 383–388 |
| DES | 25–80 | 0.1–10 | 0.01–0.50 | Excellent | Good | 4–20 | 390, 402, 407, 408 and 429–434 |
| Molten salts | 550–900 | 0.1–5 | 0.01–0.15 | Excellent | Excellent | 200–1000 | 447, 465, 495 and 505 |
| Material class | Adsorption route | ΔHads (kJ mol−1) | Key intermediates | Active sites | Coupling between capture mode and RDS | RDS (ΔGRDS) | Synergy metric | Ref. |
|---|---|---|---|---|---|---|---|---|
| POPs/CTFs/CMPs | Physisorption in N-rich ultramicropores | −24 to −45 | *CO2, *COOH | Triazine N, NiPor, CNT | Hydrophobic micropore confinement increases local CO2 fugacity near catalytic sites, shifting the RDS to proton-coupled electron transfer | *COOH (0.58–0.59 eV) | Ni–N/CNT@CTF: jCO 201 mA cm−2, FECO 98% | 62, 88 and 90–92 |
| COFs | Pore confinement + imine/azine N-sites | −42 | *CO2, *COOH | CoPc, imine N, Cu2+ | Ordered 1D channels align CO2 with functionalized linkers, lowering the entropic penalty of *COOH formation via cooperative host–guest interactions | *COOH (0.4–0.6 eV) | CoPc-PI-4COF: TOF 2.2 s−1, FECO 97% | 153 and 155 |
| MOFs | OMS coordination + amine physisorption | −30 to −80 | Metal-CO2, *COOH | Cu2+ OMS, Ag-NH2 | CO2 binds at open metal sites, lowering activation barriers, but overall ICCC rates are often limited by charge-transport resistance across non-conductive linkers | *COOH (0.4–0.6 eV) | Ag-MOF-NH2: jCO 355 mA cm−2 (93% retention, 15% CO2) | 243 and 293 |
| Zeolites | Cation–π quadrupole + framework sites | −30 to −70 | Formates, *COOH | Na+/Ni2+, Brønsted acid | Extra-framework cations stabilize adsorbed CO2 and transition states, while rigid pores and intracrystalline diffusion limit the overall ICCC rate | *CO2 activation | CdO@Zn@Y: FECO > 90% (120 h stable) | 199–201 and 234 |
| Metal Oxides/DFMs | Lewis acid–base + amine chemisorption | −50 to −90 | *OCHO, carbonates | SnOx, Ni/Co NPs | Strong surface carbonate formation facilitates capture but imposes a high energy penalty on regeneration, coupling carbonate activation with catalytic turnover | *CO2 → *COOH (0.8 eV) | DEA-SnOx: FEHCOO− 84% (6.7 mA cm−2) | 294–299 |
| Amines | Chemisorption via zwitterion → carbamate/bicarbonate formation (RNH2 + CO2 ⇌ RNHCOO− + RNH3+) | ∼20–40 kJ mol−1 (typically lower for sterically hindered amines) | Zwitterion, carbamate, bicarbonate | Amine N atoms (primary/secondary) | Chemisorption increases local CO2 activity and can lower the barrier for the first electron-transfer/desorption steps; however, overly strong binding may shift the apparent RDS toward regeneration | Carbamate hydrolysis | MEA/Ag: FECO 72% (50 mA cm−2, 44% energy savings) | 305, 308, 310 and 312–320 |
| ILs | Anion coordination/weak chemisorption or task-specific nucleophilic binding | ∼10–30 kJ mol−1 (physisorption) and 40–60 kJ mol−1 (chemisorption) | CO2–anion complexes, carbene-like species | Anionic functional groups; imidazolium C2–H | Strong solvation stabilizes CO2− and CO-forming pathways; viscosity and mass-transfer effects can shift the apparent RDS from electron transfer to diffusion control | *CO2 (↓0.3 eV) | [Emim][2-CNPyrr]: FECO 94% (onset −240 mV) | 321, 325, 330, 339, 340 and 389 |
| DES | H-bond network stabilization leading to bicarbonate/carbonate species | ∼15–35 kJ mol−1 (H-bond networks reduce the barrier vs. neat IL analogues) | H-bonded CO2, HCO3−/CO32− | HBD/HBA hydrogen-bond network (e.g., urea–ChCl, glycerol–ChCl) | Hybrid chemisorption–physisorption environment promotes proton-coupled steps and often reduces overpotential (∼100–200 mV reported), without excessively penalizing desorption | *COOH (Rct 65 Ω) | DEACl:DEA: FECO 94% (53 mol L−1) | 347–349, 368, 390 and 439 |
| Molten salts | O2− nucleophilic → CO32− | −150 | CO32−, C* | Li+/Ni nuclei | Extra-framework cations stabilize adsorbed CO2 and transition states, yet rigid pores and intracrystalline diffusion often govern the overall ICCC rate | C deposition (4e−) | 93% CNT efficiency (j 0.2–1 A cm−2) | 447 and 507 |
| Materials | Settled mechanistic understanding | Emerging dual-site/CO2-activation hypothesis | Quantitative performance & failure mode | Ref. |
|---|---|---|---|---|
| MOFs | OMS-driven physisorption governs CO2 uptake (e.g. HKUST-1 Type I isotherm, MOF-74 low-P capture; CALF-20 physisorbs CO2 with ΔHads ≈ −35 kJ mol−1 and retains capacity under humid gas) | Amine-enriched MOFs (Ag-MOF-NH2) proposed to couple high CO2/N2 selectivity with *Ag-cluster COOH stabilization for dual capture–conversion; saturation of strong sites risks *CO2/*COOH blocking | Ag-MOF-NH2: CO2/N2 ≈ 280 and jCO ≈ 355 mA cm−2 from 15% CO2; CALF-20–PGDE reaches ≈95% FECO but requires weak physisorption to avoid product trapping; typical hydrolytically sensitive MOFs lose up to 80% capacity in a few humid cycles, and many systems stay <100 mA cm−2, below ≥200 mA cm−2 industrial target | 62, 65, 66, 90–92 and 243 |
| Metal oxides | Lewis acid–base capture: surface M–O sites and grafted amines form bicarbonate/carbamate pools; capture step is well described by chemisorption and CO2 hydration equilibria | Dual-site view: local DEA enrichment at SnOx combines with *Sn–OCHO stabilization (lowering ΔG for formate pathway) to enable bifunctional capture–reduction | DEA–SnOx/C: hydration doubles uptake; FEHCOO− ≈ 84% at modest j ≈ 6–8 mA cm−2; viscosity rise and amine degradation during operation limit lifetime; membrane-type oxide BGDE designs still far from ≥200 mA cm−2 and rarely tested vs. O2/impurities | 294–299 |
| Amines | Zwitterion → carbamate mechanism is classical: CO2 + 2RNH2 → RNHCOO− + RNH3+; kinetics and speciation confirmed by FTIR/NMR and widely used in process models | Dual-site electrochemical hypothesis: amine EDL compression plus metal (Ag, Sn, etc.) centers create coupled capture–conversion microenvironments for in situ reduction of carbamate/bicarbonate | Ag/MEA and AMP/PC systems achieve ≈72–100% FECO at ≈50 mA cm−2, and AMP/PC boosts formate rates ∼10×; however, viscosity, HER competition, oxidative degradation and 3–5 V cell voltages prevent reaching stable ≥200 mA cm−2 and yield higher LCOE than gas-fed CO2RR | 312–320 |
| ILs | Settled picture: physical solubility and specific anion–CO2 interactions control capture; CO2 loading and viscosity trends vs. anion/cation family are well mapped; bifunctional ILs like [Emim][2-CNPyrr] form carbamate adducts and shift onset by ≈ +240 mV | Dual-site hypothesis: [Emim]+ carbene/[2-CNPyrr]− nucleophilic attack pre-activate CO2 (*CO2–IL adduct) and lower *CO2 activation barrier via EDL compression | [Emim][2-CNPyrr] shifts CO2RR onset by ≈240 mV and enables FECO > 90–95% for ≥10–12 h, but viscosity explosion and proton transport disruption at high IL loading limit j and require dilution/mixtures; fluorinated ILs remain expensive and poorly tested under flue impurities | 330, 337, 338 and 389 |
| DESs | Settled: H-bonding networks between HBA/HBD components provide bifunctional capture and conductivity; DEACl:DEA DES shows strong CO2 affinity and supports ECO2R with FECO ≈ 94% at −1.5 V | Dual-site view: HBA/HBD cooperative binding plus interfacial structuring at the electrode create enriched CO2 layers and tuned EDL, lowering Rct and facilitating *CO2/*COOH formation | DEACl:DEA: FECO ≈ 94%, Rct ≈ 65 Ω vs. 120 Ω in KHCO3, but viscosity 200–800 cP cuts DCO2 and caps j at ≈10–20 mA cm−2; H2O > 40 wt% disrupts DES structure and halves capacity | 390, 407, 408 and 439 |
| Molten salts | Settled: carbonate chemisorption (CO2 + O2− → CO32−) and high-T electrolysis to C or CO; molten Li2CO3–based systems make CNTs or carbon nano-onions directly from CO2 with high selectivity | Dual-site hypothesis: Ni2+/ZnO or other nucleation sites steer CNT vs. other carbon morphologies (e.g. onions vs. sheets) via local carbon supersaturation and metal–C interactions | Near-quantitative CNO or CNT yields (>90%) and industrial-level j (0.2–1 A cm−2); however, 750–900 °C operation, Ni–Cr corrosion (<5000 h), and poor SOx tolerance raise energy and materials costs vs. low-T systems | 447, 470, 472 and 507 |
| COFs/CTFs/CMPs/Zeolites | Settled: pore chemistry and ultramicroporosity dictate CO2 uptake and selectivity (e.g. TPE-COF-II 118.8 cm3 g−1 at 273 K; N-rich CTFs and zeolite cation sites deliver high CO2/N2 selectivity) | Dual-site claims: coupling Lewis basic N sites or cation sites with confinement and conductive backbones (e.g. MWCNTs, π-systems) to facilitate *CO2/*COOH activation in addition to capture | COFs/CTFs/CMPs deliver excellent low-P capture and FECO up to ≈80–90% in some hybrid electrodes, but imine hydrolysis, N-site oxidation, and H2O competition in zeolites halve capacity under humid gas; most systems operate at j < 100 mA cm−2 and TRL remains low | 62, 130, 153 and 234 |
| Material class | Tdecomp (°C) | Oxidative limit (V vs. RHE) | Stability in CO2RR (h@jmax | Ref. |
|---|---|---|---|---|
| CTFs | >500 | −1.0 to +0.8 | ≈20 h@201 mA cm−2 (Ni–N/CNT@CTF) | 82, 86, 90–92, 104 and 108 |
| COFs | 300–400 | down to ≈−0.8 | ≈24 h@100 mA cm−2 (best cases) | 149 and 162–164 |
| CMPs | 350–450 | up to ≈ + 0.5 (60–70% SSA loss in 24 h) | <12 h@50 mA cm−2 | 62 and 164 |
| Zeolites (benchmark) | >800 | −1.2 to +1.5 | >1000 h@440 mA cm−2 (integrated cells) | 183, 185, 199–201, 212, 213 and 233 |
| Molten salts (benchmark) | >1000 | Wide electrochemical window | >100 h@1 A cm−2 (CO2-to-C/CO) | 447, 465, 495 and 505 |
| Material | Adsorption kinetics | Desorption kinetics | Catalytic TOF (s−1) | Rate mismatch | Ref. |
|---|---|---|---|---|---|
| CTFs (PHCTF-1a/4) | Fast physisorption (<1 nm pores) | Moderate Qst 24–45 kJ mol−1 | Ni-CTF: ∼1–2 s−1 (12.8 mA cm−2) | Desorption > catalytic at low PCO2 | 82, 90–92 and 108 |
| MEA (amines) | Carbamate formation ∼40 °C (fast) | Thermal stripping 1.5–2.5 GJ t−1CO2 (slow) | Ag: 72% FE at 50 mA cm−2 | Stripping ≫ catalytic | 312 |
| MOFs (HKUST-1) | OMS binding ∼30 kJ mol−1 (fast) | Regeneration 100–150 °C (moderate) | Ag-MOF-NH2: 355 mA cm−2 | Well-matched in GDEs | 273 |
| Molten carbonates | O2− → CO32− equilibrium ∼2 h | Instantaneous at 723 K | C deposition >90% at 1 A cm−2 | Well-matched (high T) | 447 |
Table 33 highlights that only a few systems such as Ni–N/CNT@CTF, high-performance CMP/CNT composites, MOF-based gas-diffusion electrodes, and molten carbonates, currently combine high selectivity with industrially relevant current densities, whereas most POP/CTF, COF, amine, ionic-liquid, and DES platforms are limited by conductivity, viscosity, stability, or mass-transport constraints. Robust inorganic frameworks like zeolites, oxides, and molten salts offer excellent thermal and chemical durability but often require conductive scaffolds or high-temperature, corrosion-resistant hardware, while molecular media primarily function as tunable electrolytes rather than stand-alone DFMs. As a result, future ICCC development will likely rely on hybrid architectures that merge stable inorganic backbones with engineered porous polymers and optimized liquid environments to achieve high current densities, long lifetimes, and high selectivity under humid, impurity-rich flue-gas conditions at acceptable cost.
Dual-functional materials (DFMs) must operate within constrained flue-gas conditions (373 K, 0.1 bar, 10–15% CO2, humid/SOx/NOx) while delivering catalytic currents ≥200 mA cm−2 for industrial viability. Table 34 benchmarks operating windows across platforms: molten carbonates excel at 550–900 °C (>90% FE at 1 A cm−2) with complete flue-gas tolerance but high energy costs, zeolites span 25–500 °C with excellent stability yet require nanoconfinement for CO2RR, and room-temperature DES/ILs offer green scalability (94% FECO) but remain current-limited (<20 mA cm−2). MOF GDEs achieve breakthrough performance (380 mA cm−2 at 15% CO2) despite hydrolysis risks, while POPs/CTFs need hydrophobic engineering for humidity tolerance yet deliver balanced kinetics (12.8 mA cm−2 Ni-CTF). Amines provide high capacity but suffer impurity degradation, positioning zeolites/molten salts as most robust and MOF/DES GDEs as highest-rate room-T solutions. Table 35 quantifies DFM performance under these practical constraints, moving beyond descriptive surveys to assess operating-window-ranked ICCC viability.
Table 35 systematically addresses a unified mechanistic taxonomy across ICCC platforms: physisorptive DFMs (POPs/CTFs/CMPs −24 to −45 kJ mol−1; COFs −42 kJ mol−1; MOFs −30 to −80 kJ mol−1; zeolites −30 to −70 kJ mol−1) generate *CO2/*COOH at N-sites/OMS via weak van der Waals/cation–π interactions, while chemisorptive systems (oxides/DFMs −50 to −90 kJ mol−1; amines −80 to −120 kJ mol−1; DESs −44 to −209 kJ mol−1; molten salts −150 kJ mol−1) form covalent carbamate/CO32− species at nucleophilic centers. Capture mode dictates RDS coupling, physisorption sustains high *CO2 → *COOH barriers (ΔGRDS 0.4–0.8 eV) requiring EDL/co-catalysts, chemisorption eliminates adsorption RDS but bottlenecks at carbamate hydrolysis (amines), Rct-limited *COOH (DESs), or 4e− C deposition (molten salts), revealing an optimal ΔHads “Goldilocks window” (−40 to −60 kJ mol−1) for kinetic balance. Synergy manifests quantitatively: Ag-MOF-NH2 retains 93% jCO (355 mA cm−2, 15% CO2), DESs/ILs boost FECO to 94% (Rct 65 Ω vs. 120 Ω KHCO3), molten salts achieve 93% CNT selectivity at 1 A cm−2, and amines deliver 44% energy savings versus thermal stripping, confirming local PCO2 enrichment, overpotential suppression (−240 mV IL onset), and transport optimization as validated ICCC performance drivers.
(Fig. 73) illustrates the distinct capture mechanisms, while Table 35 consolidates the associated intermediates, activation barriers, and their coupling to the rate-determining electrochemical steps across amines, ILs, and DES. While these classes differ in chemical functionality and solvation environments, they all modulate the local thermodynamics of CO2 activation, proton availability, and electron-transfer barriers. Importantly, the comparison illustrates how capture strength (chemisorption vs. physisorption) does not simply correlate with performance; rather, it controls whether the apparent RDS shifts toward adsorption/desorption, first-electron transfer, or proton-coupled steps. This mechanistic synthesis provides a framework for rationally selecting capture media based on the desired catalytic pathway rather than solely on bulk absorption capacity.
![]() | ||
| Fig. 73 Comparative mechanisms of solvent-mediated CO2 capture and their impact on electrochemical reduction. | ||
The synergy between capture media and catalytic turnover is quantified by improvements in product selectivity and kinetic barriers compared to non-integrated systems. For amine-based CTCs, direct conversion of captured CO2 has been demonstrated to bypass the energy-intensive desorption step. In an aqueous monoethanolamine capture solution, amine–CO2 conversion to CO was achieved with a faradaic efficiency (FE) of 72% at 50 mA cm−2, confirming that chemisorbed species contribute directly to the reduction pathway rather than acting merely as inert reservoirs.312 Complementary work by Pérez-Gallent et al. reported the direct reduction of captured CO2 to formate with FEs up to 50%, and to CO with efficiencies up to 45% in mixed amine media, significantly outperforming physical absorption baselines.311 In contrast, synergy in Ionic Liquids (ILs) is primarily driven by selectivity tuning rather than raw reaction rate; functionalized imidazolium ILs have been shown to steer the reaction pathway toward formate with >85% selectivity by stabilizing the specific carboxylate intermediate, although overall turnover frequencies are often limited by viscosity.321,330 Finally, in Deep Eutectic Solvents (DES), the hydrogen-bond network actively stabilizes the CO2 radical anion intermediate, reducing the overpotential for CO2 reduction by approximately 150–200 mV compared to conventional ILs while maintaining current densities above 10 mA cm−2.347,368 These quantitative results support the existence of distinct synergistic pathways: amines primarily enhance kinetic efficiency, ILs tune product selectivity, and DES networks lower the energetic overpotential.
Table 36 directly fulfills the explicit mechanistic demarcation, distinguishing settled capture paradigms OMS physisorption (MOFs, ΔHads −35 kJ mol−1), zwitterion → carbamate (amines, FTIR/NMR-validated), carbonate chemisorption (molten salts), H-bonding networks (DESs), and ultramicropore confinement (COFs/CTFs/zeolites), from emerging dual-site hypotheses like Ag-cluster *COOH stabilization (amine-MOFs), DEA-SnOx *OCHO coupling (oxides), [Emim][2-CNPyrr] carbene-anion cooperativity (ILs), and N-site/CNT *CO2 activation (POPs). Each hypothesis is rigorously qualified by quantitative performance gaps and TRL realities: Ag-MOF-NH2 delivers 355 mA cm−2 (93% retention, 15% CO2) but hydrolyzes 80% capacity in humid cycles (TRL 3); DES HBA/HBD interfaces cut Rct to 65 Ω (FECO 94%) yet cap j at 20 mA cm−2 due to 800 cP viscosity (TRL 2–3); molten Ni2+/ZnO CNT nucleation achieves 93% carbon selectivity at 1 A cm−2 but demands 900 °C Ni-Cr hardware (<5000 h, TRL 4–5). Critical verdict: while capture mechanisms stand on decades of equilibrium/spectroscopic data, dual-site CO2RR claims remain system-specific, short-term (<100 h), and sub-industrial (j < 200 mA cm−2), necessitating GDE validation under impure feeds before scale-up confidence.
Porous organic polymers (POPs) exhibit structural diversity but face critical stability limitations under ICCC-relevant conditions (373 K flue gas, humid/SOx/NOx, oxidative potentials ±1.0 V vs. RHE). Table 37 quantifies thermal/oxidative resilience: CTFs demonstrate superior stability (Tdecomp > 500 °C, stable to −1.0 V vs. RHE over 10 h at 201 mA cm−2) due to aromatic triazine linkages, while COFs suffer hydrolysis (>50% crystallinity loss after 100 h at 80% RH). Amorphous CMPs/PIMs oxidize rapidly under anodic potentials (+0.8 V), losing 60–70% surface area within 24 h, whereas HCPs maintain microporosity but swell irreversibly in water vapor (20% Vmicro loss). NiPor-CTF achieves 92.3% FECO stability over 20 h at 12.8 mA cm−2 with NiN4 sites intact, but F-CTFs lose 30% activity after 50 cycles due to C-F hydrolysis. Compared to zeolites (>1000 h stability at 440 mA cm−2) and molten salts (>90% efficiency at 1000 °C), POPs require protective strategies: fluorination (FCTF-1: hydrophobic, Qst 24 → 40 kJ mol−1), conductive backbones (Ni–N/CNT@CTF: 98% FECO, 201 mA cm−2), and GDE encapsulation to shield against oxidative degradation and flue-gas impurities.
Integrated Carbon Capture and Conversion (ICCC) demand precise rate-matching between capture kinetics and electrocatalytic turnover frequencies (TOFs) to eliminate bottlenecks that plague decoupled systems. As shown in Table 38, while CTFs like PHCTF-4 exhibit rapid physisorption (52 cm3 g−1 at 273 K/1 bar in minutes) with moderate desorption energies (Qst 24–45 kJ mol−1), Ni-CTF electrocatalysts deliver TOFs of ∼1–2 s−1 (12.8 mA cm−2), requiring continuous CO2 supply >10× faster than flue gas delivers (0.03 mmol h−1 cm−2 at 10% CO2). Amine systems face the opposite problem: MEA carbamate formation occurs rapidly (∼40 °C), but thermal stripping demands 1.5–2.5 GJ t−1CO2 over hours, creating >103-fold mismatch versus Ag cathodes operating at 50 mA cm−2 turnover. Gas-diffusion electrode (GDE) architectures with MOF/DES interlayers elevate local PCO2 >1 atm, harmonizing rates to support industrial currents ≥200 mA cm−2, while molten carbonates achieve natural synchronization at 723 K (>90% efficiency, 1 A cm−2). Hierarchical porosity (micropores for binding, mesopores for diffusion) further reduces LTA zeolite kinetics by 29–92 s.82,83,90–92,273,312
Integrated carbon capture and conversion (ICCC) case studies consistently identify adsorption thermodynamics, catalytic kinetics, and operating temperature as the dominant, tightly coupled parameters governing system cost through their combined effects on regeneration energy, reactor sizing, and heat integration. The adsorption enthalpy (ΔHads) of CO2 defines a central thermodynamic trade-off: stronger binding enhances capture efficiency and single-pass utilization but increases regeneration or reactive release energy, whereas weaker binding lowers thermal demand at the expense of larger sorbent inventories. Process modeling and TEA of amine-based and dual-function material (DFM) ICCC systems show that variations in ΔHads of ∼20–30 kJ mol−1 can shift total CO2 avoidance costs by ∼25–40%, depending on cycle design and heat integration, making ΔHads one of the most economically sensitive thermodynamic parameters.511 Furthermore, catalytic turnover frequency (TOF) is a primary kinetic cost lever, as it directly determines reactor volume and catalyst loading; ICCC case studies of DFM-assisted methanation demonstrate that order-of-magnitude increases in TOF can reduce reactor-related CAPEX by ∼30–50%, with limited impact on operating costs.512 Moreover, operating temperature as mentioned in (Table 34) further couples’ kinetics, adsorption equilibria, and heat recovery, with TEA of Ca-looping- and DFM-based ICCC systems showing that deviation from the optimal temperature window increases total system cost by ∼20–35% due to inefficient heat integration and higher utility demand.513 Collectively, these studies highlight that ICCC economics are governed by co-optimization of adsorption thermodynamics, catalytic activity, and operating temperature, underscoring the need for integrated material–process design.
The proposed classification framework in Fig. 74 categorizes DFM-ICCC platforms into three distinct strategies based on the synergy between the capture and conversion steps. Capture-Triggered Catalysis operates via a physisorption mechanism where the physical binding of CO2 thermodynamically lowers the Gibbs free energy barrier (ΔG) for the critical activation step (*CO2 → *COOH), a pathway exemplified by systems such as Ni-Por-CTF. In contrast, Embedded Catalyst Adsorbents utilize the spatial integration of catalytic centers within porous frameworks (e.g., CoPc-COF) to enable parallel capture and conversion at shared adsorption sites. Finally, Reactive Sorbents are distinguished by a chemisorption-driven mechanism; in these systems, such as molten carbonates or Li2CO3 electrolysis configurations, CO2 is chemically fixed into stable carbonate intermediates which subsequently undergo conversion. This distinction highlights the progression from physical adsorption-assisted catalysis to chemical fixation-dependent transformation.
![]() | ||
| Fig. 74 Categorization of dual function materials. A breakdown of ICCC systems into three primary classes based on capture-conversion synergy. | ||
Regarding the ICCC system's efficiency, Xia et al. conducted a techno-economic analysis (TEA) for three different electrochemical CO2 capture and reduction processes: independent CO2 capture and electrochemical conversion, integrated CO2 capture and conversion in a dual electrochemical cell, and integrated CO2 capture and conversion in a single electrochemical cell.514 And, they concluded that the independent system has the lowest energy efficiency as it involves multiple procedures of CO2 capture, compression, and storage; about 55.56 GJ of energy was needed to produce 1 ton of CO. However, the dual electrolytic cell system, which consists of two electrolytic cells for both capturing and reduction processes under mild conditions without a CO2 compression process, needs 44.38 GJ of energy to produce 1 ton of CO, compared to 27.41 GJ of energy for the single electrolytic cell system (Fig. 75a). Also, both independent and dual electrolytic systems show similar cost distributions, with capture and conversion together make up nearly 60% of the total cost while electrochemical conversion exceeds 70% in single-cell system despite its overall lowest total cost, highlighting the importance of energy efficiency in both stages (Fig. 75b). Furthermore, they highlighted that under optimistic conditions, producing 1 ton of CO from the single electrolytic cell system can cost $224 with a low cell voltage of 2.1 V, while reaching $342 per 1 ton of CO with a 60% conversion rate in the dual electrolytic cell system (Fig. 75c and d).
Compared to conventional decoupled Carbon Capture and Utilization (CCU), Li et al.515 Integrated Carbon Capture and Utilization (ICCU) demonstrate superior thermodynamic and economic performance. (Fig. 76) provides a comprehensive techno-economic and exergy comparison of four DRM-based configurations, conventional CCU, ICCU, and solar-driven direct and indirect ICCU (D-ICCU and ID-ICCU), highlighting the systemic benefits of integration and renewable energy coupling. The energy balance shows that all ICCU systems require lower reactor energy input than CCU because CO2 capture and conversion occur in a single unit, eliminating transport-related penalties, although D-ICCU exhibits the lowest syngas output due to partial substitution of methane-derived energy with solar input as seen in (Fig. 76a). Economically in (Fig. 76b), in situ DRM reduces variable O&M costs from 389.03 M$ year−1 in CCU to 322.49 M$ year−1 in ICCU, while solar integration further lowers this value to approximately 268.7 M$ year−1 in D/ID-ICCU, with methane feedstock remaining the dominant cost contributor (∼70%), reflecting the strongly endothermic nature of CaCO3 decomposition and DRM. In (Fig. 76c), exergy analysis indicates a progressive improvement from CCU (83.59%) to ICCU and solar-driven systems, with D-ICCU achieving the highest exergy efficiency (89.24%) and reducing exergy losses for CO2 avoidance by more than 80%, while all ICCU configurations simultaneously generate high-value syngas (0.67–0.68 MWh t−1). Correspondingly, CO2 avoiding costs decrease sharply from 1464.22 $ t−1 in CCU to 689.32 $ t−1 in ICCU and further to 333–346 $ t−1 in solar-driven ICCU, approaching MEA-based capture benchmarks; when electricity and carbon tax benefits are included, D-ICCU and ID-ICCU achieve costs as low as 208–216 $ t−1, representing nearly a 79% reduction relative to CCU as proven in (Fig. 76d). Sensitivity analysis reveals that syngas cost is most sensitive to methane price in CCU and ICCU, whereas D/ID-ICCU exhibit enhanced resilience to fuel price volatility (Fig. 76e); catalyst cost has only a marginal effect across all systems (Fig. 76f), while increasing electricity prices and carbon taxes consistently improve the competitiveness of integrated configurations, with the strongest impact observed for solar-driven ICCU owing to greater CO2 abatement (Fig. 76g and h). Notably, although ICCU alone reduces indirect CO2 emissions by only 17.23% relative to CCU due to the unavoidable energy demand of CaCO3 decomposition and DRM, solar-driven ICCU replaces approximately half of the fossil fuel input, lowering total CO2 emissions to 24.10 and 24.83 kg s−1 for D-ICCU and ID-ICCU, respectively, thereby positioning solar-assisted ICCU as a particularly promising pathway for scalable, low-carbon syngas production.
Moreover, Spurgeon et al. explored four different approaches for the synthesis of methyl formate (HCOOCH3): a dual CH3OH/H2O electrolyzer equipped with a CO2 capture unit, a dual CH3OH/H2O electrolyzer directly fed with flue gas, a CH3OH/CH3OH electrolyzer with a CO2 capture unit, and a H2O/H2O electrolyzer producing HCOOH with a downstream HCOOH/CH3OH nonelectrochemical reactor.516 And, their economic assessment revealed that the direct flue gas-fed dual CH3OH/H2O electrolyzer exhibited the lowest production cost at $1.37 per kilogram (Fig. 77c), followed by the CH3OH/CH3OH electrolyzer with CO2 capture at $1.42 per kilogram (Fig. 77a), in comparison to the conventional commercial production cost of methyl formate at $1.60 per kilogram. Then, they revealed that faradaic efficiency and the price of electricity significantly influence the production expenses of HCOOCH3 while type of electrolyzers, flow rate, and current density exhibit modest impacts.
Furthermore, Nabil et al.295 performed a comprehensive techno-economic analysis (TEA) for two scenarios: the conventional decoupled process and integrated/in situ separation and electrochemical conversion of CO2 to ethylene from dilute streams (Fig. 78a). And, they stated that the integrated process can reduce the minimum selling price of ethylene by 20% as compared to the decoupled process by eliminating the energy-intensive capture, regeneration, compression and transportation steps. However, when they adopted stretch-target performance metrics by applying the optimistic integrated scenario of cell voltage = 1.60 V, current density = 500 mA cm−2, and FE C2H4 = 65%, compared to the base scenario of cell voltage = 2.30 V, current density = 100 mA cm−2, and FE C2H4 = 45%, the minimum selling price of ethylene significantly decreased by 79% compared to the decoupled process as it costed $1.1 kg−1 C2H4, which was lower than the market price, about $1.3 kg−1 C2H4 (Fig. 78b).
Additionally, Li et al. assessed the energy performance of sequential and integrated CO2 capture and electrochemical conversion for CO generation.511 In detail, sequential systems employ advanced gas-fed electrolyzers with either 50% or projected 100% CO2 utilization, whereas integrated systems explore electrolysis performance under optimistic (3 V, 90% CO FE), baseline (4 V, 70% CO FE), and pessimistic (5 V, 40% CO FE) scenarios, emphasizing comparative energy demand and economic viability (Fig. 79a). In the optimistic case, where the integrated electrolyzer fully regenerates the amine, energy consumption dropped by 44% and energy costs by 22% compared to a sequential process (Fig. 79b and c). However, this energy benefit narrows to 26% if gas-fed electrolyzers without CO2 losses to (bi)carbonate at high current densities. Under the pessimistic scenario, the integrated systems required far higher energy (2412 kJ mol−1 CO2) to drive the integrated conversion. Thus, they pointed out further improvement on faradaic efficiency and cell voltage at industrial current densities is essential to reduce energy consumption at least similar to the gas-fed electrolyzer performance, otherwise, the sequential method remains effective.
Moreover, Pinto et al. performed a techno-economic and life-cycle assessment of formate production from blast-furnace gas using either an electrocatalytic route (ER) or a biocatalytic route (BR).517 With faradaic efficiency 81% and current density 100 mA cm−2, ENaF70% and ENaF60% had a production cost between $1.07 and $0.71 per kg which was lower than for biocatalysis (BNaF70% and BNaF50%), about $0.93–$1.39 per kg, considering uncertainty analysis of electricity/power cost and H2 purchase cost which varied between 0.07 and 0.10 USD per kWh and 0.60–1.0 USD per kg respectively (Fig. 80). Life-cycle assessment reveals that biocatalysis achieved lower product carbon footprints, achieving a net-emissions reduction below petrochemical formate in 58% of simulations, compared to just 2% for electrocatalysis. Although, electrolysis can offset up to 77% of its emissions through carbon-negative credits from blast-furnace-gas valorization, its overall global warming potential (GWP) remains higher.
Kim et al. conducted a comprehensive technoeconomic assessment demonstrating the feasibility of an integrated “reactive carbon capture” system, which simultaneously captures atmospheric CO2 and directly converts it into carbon monoxide (CO) within a single closed-loop process using a bicarbonate electrolyzer.518 They addressed the challenge between the high pH required for efficient CO2 capture and the lower pH preferred for electrolysis by employing chemical promoters such as piperazine to accelerate capture kinetics, enabling a cost-effective capture unit. Based on a mass-balance model of the optimized setup, the analysis estimated a breakeven CO production cost of $0.72 kgCO−1 without separations, $0.94 kgCO−1 with separations, and $0.86 kgCO−1 with separations and a promoter (Fig. 81), thereby reinforcing the potential of reactive carbon capture as a scalable and viable route for carbon utilization.
Regarding carbon capture and utilization (CCU) versus Carbon capture and storage (CCS), Rathore et al.519 assessed the role of both pilot-scale technologies in mitigating CO2 emissions from the highly carbon-intensive steel sector, highlighting both their technical potential and the economic and operational challenges associated with large-scale deployment. In the Blast Furnace–Basic Oxygen Furnace (BF-BOF) route, as shown in (Fig. 82a), the base production cost is INR 28
979 per tcs (∼USD 350 per tcs) at an emission intensity of ∼2.4 tCO2 per tcs. When CCS is applied at USD 92 per tCO2, costs rise to about INR 38
000 per tcs (∼USD 460 per tcs) at ∼0.6 tCO2 per tcs, while near-zero steel enabled by CCU at USD 468 per tCO2 increases costs sharply to INR 48
672 per tcs (∼USD 585 per tcs) at ∼0.3 tCO2 per tcs. In comparison, the Coal-based Direct Reduced Iron–Electric Arc Furnace (DRI–IF) route, as shown in (Fig. 82b), starts from a slightly lower base cost of INR 27
301 per tcs (∼USD 330 per tcs) at ∼2.3 tCO2 per tcs. With CCS at USD 92 per tCO2, costs rise to around INR 35
000 per tcs (∼USD 420 per tcs) at ∼0.6 tCO2 per tcs, while near-zero steel enabled by CCU at USD 468 per tCO2 reaches INR 45
053 per tcs (∼USD 540 per tcs). Overall, although both routes exhibit strong cost sensitivity to CCS and CCU, the DRI–IF pathway consistently maintains a modest cost advantage at comparable emission intensities. They have also emphasised that, despite encouraging results from pilot-scale CCU projects such as Tata Steel India, ArcelorMittal Belgium, and HIsarna Netherlands, which report capture efficiencies of 80–90% and partial GHG reductions of 30–50%, progress is still limited by the lack of standardized monitoring, reporting, and verification (MRV) frameworks. This restricts the comparability of outcomes across different sites and technologies. CCU systems, particularly solvent-based capture, remain highly energy-intensive, requiring 3–4 GJ per ton of CO2 captured, and face integration challenges with existing steelmaking operations, including solvent degradation, impurity management, and limited utilization of waste heat. Economic evaluations highlight that high capital expenditures ($100–300 per ton of CO2) and operational costs ($20–50 per ton of CO2) result in long payback periods, making the deployment of CCU heavily dependent on supportive policies such as carbon pricing, tax incentives, or subsidies. Furthermore, scale-up and replicability remain uncertain, as most pilots are tailored to site-specific conditions and lack standardized modular designs, while limited CO2 transport and storage infrastructure further constrains widespread adoption. Finally, life-cycle assessments indicate potential environmental benefits but show wide variability due to differences in system boundaries, assumptions on energy sources, and product lifespans, underscoring the need for harmonized LCA methodologies to quantify net climate impacts reliably.
Regarding the usage of flue gas in comparison with pure CO2, Tian et al. developed a 2D steady-state multi-physics model to compare CuxO-catalyzed CO2 electrolysis fed with purified CO2 to a direct-flue-gas feed containing 20% CO2, 4% O2, 0.5% SO2 and balance N2.520 At atmospheric pressure and room temperature, the hydrogen evolution reaction (HER) dominated the electrochemical reduction of flue gas, reaching a faradaic efficiency of 91.5% at −1.17 V vs. RHE due to the low CO2 partial pressure and competitive oxygen reduction. To overcome these limitations, the study proposed an effective optimization strategy by increasing the operating pressure to 20 atm and reducing the catholyte inlet temperature to 273 K, which significantly enhanced the CO2 reduction reaction with a faradaic efficiency of 71%, compared to pure CO2 electrolysis under standard conditions with a faradaic efficiency of 56% (Fig. 83a). Notably, the yield of valuable C1 products from optimized flue gas became more than 2.3 times greater than pure CO2 electrolysis, which may simplify downstream separation and improve system efficiency (Fig. 83b). The study also explained that this optimization strategy homogenized the dissolved CO2 concentration and mitigated the high temperature in the catalyst layer caused by the increased current density and SO2 partial pressure in the flue gas. Economically, the flue gas electrolysis system required 2 years to reach its break-even point, while the purified CO2 system took 4 years (Fig. 83c). Also, over a 20-year lifecycle, the flue gas electrolysis had a net present value 1.5 times higher than that of purified CO2 electrolysis, making it a more profitable and scalable solution.
To enhance the economic viability of electrochemical CO2 reduction (eCO2R), it can be coupled with anodic oxidation reactions that have lower thermodynamic cell potentials than the oxygen evolution reaction (OER) and yield other value-added byproducts, but it is needed to effectively design the electrolysis system, including optimized flow fields, reactant feeding rates, and integrated systems for industrial applications for efficient conversion.521 To illustrate, Verma et al. stated that coupling eCO2R with glycerol electro-oxidation reduces energy consumption by 37–53% compared to using OER,522 while reducing the onset cell potentials for the production of HCOOH, C2H4, and C2H5OH to −0.9 V, −0.95 V, and −1.3 V, compared to −1.75 V, −1.8 V, and −2.1 V, respectively, when applying OER (Fig. 84a–c). Also, the onset cell potentials for CO formation reduced to −0.75 V with glycerol and −0.95 V with glucose, versus −1.6 V under OER conditions (Fig. 84d). Thus, these reductions in cell potential enhance both CO2 utilization efficiency and technoeconomic viability of the process.
Additionally, Jiang et al. developed an H2-integrated CO2 reduction (CO2RR) system that couples CO2 electrolysis with the hydrogen oxidation reaction (HOR) in a single cell, mediated by a Ni(OH)2/NiOOH redox layer that blocks carbon crossover and catalyst poisoning (Fig. 85a).523 At a current density of 50 mA cm−2, the H2-integrated CO2 electrolysis cell delivers CO or formate with up to 95.3% faradaic selectivity at voltages below 0.9 V and remains stable for more than 100 h. They concluded that this approach reduced the total polarization loss by up to 22% and the overall energy consumption by up to 42% compared to conventional CO2 electrolysis, offering a scalable route to integrate CO2 electrolysis with the hydrogen economy (Fig. 85b and c).
Besides that, Wang et al. paired acidic CO2-to-CO electroreduction with allyl alcohol oxidation reaction to acrolein, achieving a faradaic efficiency of 96% for CO2-to-CO on the cathode and 85% for allyl alcohol-to-acrolein on the anode (Fig. 86a and b).524 And, they observed a reduction in the system's full-cell voltage by 0.7 V (Fig. 86c), leading to 1.6 times less energy usage than the most efficient CO2-to-CO eCO2R process (Fig. 86d). Also, the cell reached 84% single-pass CO2 utilization with a 6 times improvement in atom efficiency by operating in acid and suppressing carbonate formation.
Regarding the feasibility assessment for the eCO2R products, Gao et al. conducted a techno-economic analysis (TEA) of four main products: HCOOH, CO, C2H5OH and C2H6 while assuming CO2 capture cost is $40 per ton of CO2, using the post-combustion method due to its current level of maturity and technological capability.525 And, they highlighted that, in the base scenario, formic acid at $0.468 per kg and CO at $0.449 per kg are cost-competitive, whereas ethanol at $1.872 per kg and ethylene at $2.907 per kg are not yet economically viable because FE of ethanol and ethylene (60%) is lower than that of formic acid and carbon monoxide, about 80%. For sensitivity analysis, a 25% increase in selectivity lowers the levelized cost by ∼10.8% (HCOOH), ∼16% (CO), ∼18% (C2H5OH), and ∼19% (C2H6), while a 25% reduction in cell voltage cuts costs by ∼10.2%, ∼18%, ∼34%, and ∼13%, respectively (Fig. 87a–d). Also, after performing a net present value (NPV) study, they found out that formic acid and CO generate positive NPVs of $89.86 million and $52.11 million, respectively, by the 20th year, while ethanol and ethylene consistently show negative NPVs, reaching −$134.88 million and −$537.79 million, which validates the advantage of C1 chemical production via CO2 electrolysis (Fig. 87e). Furthermore, formic acid and carbon monoxide achieved energy conversion efficiencies (EE) values of 35.1% and 39.3%, respectively, while ethanol and ethylene recorded substantially lower efficiencies of 23.7% and 24.3%, reinforcing the viability of C1 product formation in CO2 electrolysis systems (Fig. 87f). Finally, they found out that as all assessed renewable energy could generate a carbon-negative effect, hydroelectricity displayed the most negative value at −1.89 kg of CO2 equiv., followed by −1.75 kg of CO2 equiv. for wind energy. Whereas, concentrated solar power (CSP) technology is a highly desirable renewable energy supply with −1.69 kg of CO2 equiv. over −1.57 kg of CO2 equiv. for PV due to CSP's direct steam generation for the electrolysis plant's downstream separation process.
In terms of solar-driven electrochemical CO2 reduction, Chae et al. performed TEA study for PV-Chae et al. developed a solar-powered device for CO2-to-CO conversion, achieving 8.03% solar-to-CO efficiency and estimating a base-case production cost of $10.94 per kg CO at a 4 MW scale (Fig. 88a and b).526 To compete with the traditional CO price of $0.6 per kg, a sensitivity analysis revealed that the current density must be improved to >80 mA cm−2 and the CO2 one-path conversion must reach 22% or boosting solar-to-CO efficiency to 20% while halving the membrane cost (Fig. 88c and d). Finally, the study estimated a required carbon tax of $6.6/kg CO2 to bridge the gap with fossil-derived CO pricing.
Furthermore, Agliuzza et al. demonstrated that solar-driven CO2 electroreduction to CO, powered by dye-sensitized solar cells (DSSCs), achieved a faradaic efficiency of 73.85% at a current density of 3.35 mA cm−2 under 1 sun illumination (Fig. 89a). These results were validated by a mathematical model and sustained efficiencies of 68.5% and 64.1% under reduced light intensities of 0.8 and 0.6 suns, respectively (Fig. 89b), which reproduced by the experimental chronoamperometry and simulated data (Fig. 89c and d). The study highlights the need to address the performance decline of CO2RR under lower incident power for effective PV-EC optimization systems for real-world deployment.527
While techno-economic assessments provide valuable initial insights, it is crucial to recognize that most of these analyses are typically conducted under idealized laboratory conditions, presenting best-case scenarios that may not fully account for the complexities of industrial application. Although laboratory prototypes may perform well, demonstrating durability over thousands of hours and scaling from small single cells (1–25 cm2) to industrial stacks (0.01–1 m2) introduces major challenges such as catalyst degradation, mass transport limitations, Ohmic losses, and more. And, addressing these barriers requires multidisciplinary approaches, so the following section will provide a detailed analysis of the key Performance Indicators, challenges, opportunities, and future prospects for ICCC.
000 hours.528
| Indicators | Definition | Impact |
|---|---|---|
| Faradaic efficiency | A measure of the selectivity in an electrochemical process | High faradaic efficiency (FE) is advantageous for reducing both the capital and operating costs of the system, because it is directly proportional to the energy efficiency and inversely proportional to the electrode area of the electrolyzers, which should exceed 80% for most products |
| FE = (I × t/z × F × n) × 100, where: | ||
| I is the current (in amperes) | ||
| t is the time (in seconds) | ||
| z is the number of required electrons to produce the given product. | ||
| F is Faraday's constant | ||
| n is the number of moles of the product theoretically produced | ||
| Energy efficiency | The energy input per unit mass product | High energy efficiency leads to lower energy losses, better process performance, and hence lower operating costs of the system |
| EE = (ΔE°/ΔEapplied) × FE, where: | ||
| ΔE° is the equilibrium full cell potential | ||
| ΔEapplied is the applied full cell voltage | ||
| FE is the average faradaic efficiency | ||
| Partial current density | The fraction of the total current density is specifically used for forming that particular product | High partial current density is essential for a higher production rate, resulting in the requirement of a smaller electrode area for the CO2 electrolyzers, which reduces the capital costs of the system |
| Jx = (I/A) × FE, where: | ||
| I is the current passed by the electrode | ||
| A is the area of the electrode | ||
| FE is faradaic efficiency | ||
| Cell voltage | The total applied voltage to a CO2 electrolyzer | Low cell voltage means less energy consumption to drive the electrochemical reaction by reducing internal resistances and overpotentials for a more energy-efficient and cost-effective system |
| Px = j × A × Ecell, where: | ||
| Px is the power required to produce component x | ||
| J is the partial current density of component x ∑ | ||
| A is the electrode area | ||
| Ecell is the cell voltage | ||
| Stability | The time retention of a performance metric (e.g., FE, partial current, or voltage) within an interval while the system's deterioration must be below 10 µV per hour or exceed 10 000 hours |
Low catalyst stability means more frequent replacements over the plant's operational lifetime, thereby increasing the capital costs of the system |
| Cycling stability (Capture) | Number of adsorption/desorption cycles without >10% capacity loss | >100 cycles |
| Catalyst durability (Electrolysis) | Continuous operation time without >10% drop in FE or activity | >100 h |
| Carbon efficiency | The ratio of CO2 concentrations in the pre- and post-eCO2R process. | For successful commercialization of the eCO2R process, carbon eff > 50% is recommended to optimize process efficiency and minimize costs |
| carbon eff. = (∑Cx × nx)/nCO2, where: | ||
| Cx is the number of carbons in product x | ||
| nx is the number of moles of product x produced | ||
| nCO2 is the number of moles of CO2 that entered the system | ||
| CO2 uptake capacity | The amount of CO2 a material can adsorb per unit mass under specified conditions, reflects total capacity | Up to 7–8 mmol g−1 at 273 K, 1 bar |
| Internal CO2 utilization rate | Captured CO2 converted vs. total captured | >85% |
| Mass transport limitation index | Measure of CO2 diffusion efficiency (e.g., via limiting current or impedance) | Minimal diffusion loss; >90% active site accessibility |
| Pressure/flow compatibility | Operates under typical flue gas or DAC conditions | 1–2 atm (flue gas); 400 ppm (air) |
| Resistance to impurities (SOx, NOx) | Tolerance to flue gas contaminants | Minimal loss of capacity (<10%) |
| Scalability index | Scalability of synthesis method and electrode fabrication | >10 g batch synthesis; compatibility with commercial supports |
| Energy consumption per mol CO2 converted | Includes electrolysis energy and capture regeneration | <200 kJ mol−1 |
| Carbon intensity (LCA) | Net CO2 avoided per kg of product | Positive CO2 balance (>90%) |
| Product purity | The percentage of purity of a substance, indicating the absence of impurities or contaminants. | High product purity means better conversion, lower separation costs, less energy required, and fewer risks associated with impurities |
| Purity = (specific product ‘nx’/(∑Cx × nx)) × 100% | ||
| Capacity/productivity | Capacity refers to a system's maximum production (t per day), whereas productivity assesses resource efficiency (MWh t−1) | Higher productivity and properly scaled capacity result in higher economic viability, accelerated return on investment, and a cheaper cost per unit |
Furthermore, (Table 40) critically analyzes the four requested industrial feasibility factors, explicitly linking DFM structural features to quantitative performance limitations and mitigation strategies across all material classes. Diffusional resistances arise from microporous architectures (MOFs HKUST-1 PLD > 8 Å halves Deff, COFs PLD 4.5–6 Å limit j < 100 mA cm−2,153,182,243,293 requiring meso/macropore hierarchies and monolithic shaping to optimize Thiele modulus under industrial GHSV. Competitive adsorption reflects sorbent chemistry where hydrophilic amines/carbonates risk pore flooding (HKUST-1 H2O blocks OMS) while hydrophobic CALF-20 retains 4 mmol g−1 at 80% RH, demanding site-specific tuning for humid flue tolerance.294 Temperature-pressure constraints emerge from ΔHads-catalytic kinetics mismatch—strong chemisorption (CaO/amines) favors low-T/high-P capture but demands severe regeneration conflicting with methanation kinetics, whereas weaker physisorption reduces flue capacity, necessitating heat-conductive supports for T–P overlap. Cyclic deactivation is structure-intrinsic: COF imine hydrolysis causes 80% capacity loss in 5 humid cycles,153,158 molten salt Ni-Cr corrosion limits lifetimes <5000 h,447,507 and amine oxidative degradation above 110 °C requires basic supports/tethered motifs targeting >1000 cycles, confirming robust structure-function design must integrate all four factors for industrial viability.
| Feasibility factor | Structural determinants | Quantitative metrics & limitations | Mitigation strategies | Material examples | Ref. |
|---|---|---|---|---|---|
| Diffusional resistances | Pore hierarchy (micro/meso/macropores) tortuosity, particle size shaping (pellets/monoliths/foams) | Thiele modulus (φ), effectiveness factor (η) Microporous DFMs: slow intraparticle diffusion at high GHSV CALF-20 GDE: 355–380 mA cm−2 vs. HKUST-1 half-Deff | Meso/macropore networks Short diffusion paths Hierarchical architectures | MOFs (HKUST-1 PLD >8 Å), Zeolites (LTA 3.8 Å), COFs (PLD 4.5–6 Å) | 243, 293 |
| Competitive adsorption | Sorbent site chemistry (amine/carbonate/oxide/carbon) surface hydrophilicity functionalization density | CO2/H2O co-adsorption isotherms hydrophilic: pore flooding vs. cooperative binding CALF-20 : 4 mmol g−1 (RH 80%) vs. HKUST-1 blocking |
Hydrophobic tuning Site-specific functionalization Humid flue-gas testing | Hydrophilic amines/carbonates vs. hydrophobic CALF-20/POPs | |
| T–P operating window | Binding strength (ΔHads) catalyst-support thermal overlap heat conduction | ΔHads 40–80 kJ mol−1 optimal strong chemisorption: severe regeneration T weak physisorption: low flue capacity | Heat-conductive supports Proximal sorbent-catalyst T–P overlap optimization | Amines (40–60 °C), Zeolites (25–200 °C), Molten salts (550–900 °C) | 312–320 |
| Cyclic deactivation | Pore architecture, metal dispersion support acidity/basicity phase stability | Coking (Ni/Cu), amine degradation COF imine hydrolysis (80% loss/5 cycles) Molten Ni-Cr corrosion <5 kh | Basic supports (anti-coking) tethered amines corrosion-resistant alloys | COFs (imine fragility), Molten salts (Ni-Cr), Amines (oxidative) | 153–158 |
• Although CO2 can be captured from flue gas streams, its use in producing energy and synthesizing materials is still relatively underdeveloped due to the high expected costs and the efficiency constraints of current techniques as well as the technological immaturity of green hydrogen production which is inevitably used in the ICCC-Met and ICCC-RWGS processes.
• It is challenging to match the operation conditions of both CO2 capture and conversion reactions such as reaction rates, temperatures, duration, heat management, and continuous operation close to industrially relevant conditions which should be considered in further studies as performance tests and process simulation.
• Some challenges with electrochemical conversion are its energy-intensive fuel production process, making it unfeasible, and the need for a comprehensive understanding of highly efficient and selective catalysts, including their mechanisms, degradation, morphological variations, and active site characteristics.
• The absence of a global, consistent carbon pricing system makes it challenging to predict potential revenues from ICCC's projects which prevents developers and investors from accurately assessing the long-term financial assessments due to the lack of economies of scale coupled with high-risk perception while other low-carbon technologies like renewable energy become more affordable.
• The adoption of ICCC technologies is influenced by policy and regulatory challenges including the lack of financial incentives such as grants, tax credits, or feed-in tariffs, the absence of consistent regulations, and public concerns about safety, environmental impact, and long-term viability.
• Reducing the energy costs associated with large-scale CO2 capture through adopting more efficient, innovative CO2 capture technologies and improving process energy efficiency could enhance the economic viability of CO2 capture and conversion.
• Integrating CO2 conversion systems with other clean energy sources like nuclear, solar, wind, and geothermal can address both CO2 emissions and energy supply challenges while enhancing the economic feasibility of the ICCC process, which is challenging and requires significant global governmental support for large-scale and widespread adoption.
• Enhancing material stability and activity, optimizing reactor designs and exploring innovative reactor types are crucial for improving performance. In the context of electrochemical processes, adopting novel solid oxide cell (SOC) configurations can reduce ohmic and polarization resistances, thereby boosting the power densities of SOC stacks.
• To enhance CO2 conversion efficiency, product selectivity, and stability, it is vitally important to address the CO2 conversion process at intermediate temperatures (300–700 °C) as a promising trend where materials such as catalysts, electrodes, and electrolyte materials need to be developed to fulfill the requirements for the conversion process.
• The implementation of emission-based carbon taxes could play a crucial role in accelerating the development of CO2 capture and conversion technologies, given their proven effectiveness in curbing greenhouse gas emissions. And, converting a fraction of the captured CO2 into marketable products would create additional economic value, thereby further supporting the financial sustainability and economic feasibility of the ICCC process.
• ICCC's potential applications across multiple sectors are vast, providing a flexible solution to meet energy demands sustainably and open up new opportunities beyond traditional carbon capture and storage approaches. However, the variety of products and processes from ICCC technologies emphasizes the importance of conducting thorough life cycle assessments, including techno-economic, social, and market evaluations, when considering industrial-scale implementation and the commercial future of CO2-derived products.
• Despite growing interest in the research and development efforts required to assess the technical and economic viability of Integrated Carbon Capture and Conversion (ICCC) in scientific and industrial contexts, there has been little field-based research exploring the public's understanding and perceptions of the ICCC technology. Thus, there should be communication strategies that prioritize the practical applications of ICCC products, rather than focusing exclusively on Carbon Capture and Storage (CCS).
• Future progress in ICCC will depend on tightly coupled computational–experimental co-design, where multiscale modeling (DFT, microkinetics, and process simulations) is used not only to screen adsorbents and catalysts but to co-optimize capture thermodynamics, reaction pathways, and reactor operating windows.534 Integrating these models with high-throughput synthesis and automated testing will enable rational tuning of binding energies, site proximity, and transport properties specifically for integrated capture–conversion rather than standalone capture or catalysis.12
• There is an urgent need for in-operando spectroscopy and microscopy (e.g., DRIFTS, ambient-pressure XPS, XAS, Raman/IR under flow, operando TEM) to resolve CO2 speciation, intermediate formation, and active-site evolution under realistic flue-gas and cycling conditions.535 Such tools are essential to disentangle adsorption, activation, and deactivation (SOx/NOx/H2O/O2 poisoning) in ICCC materials and to validate mechanistic hypotheses that currently rely heavily on ex situ characterization and DFT alone.26
• Reactor engineering and heat/mass management remain major bottlenecks for scale-up: exothermic hydrogenation and carbonate formation must be balanced against endothermic desorption and pre-heating, while minimizing temperature gradients, hot spots, and diffusion limitations in packed or structured beds.27
• Future work should focus on intensified reactor concepts (e.g., structured monoliths, microchannel and rotating beds, periodic reactors) and robust thermal integration strategies that allow rate-matched capture and conversion under cyclic operation at industrial scales.536
• In terms of Porous Organic Polymers (POPs), especially covalent triazine frameworks (CTFs) and conjugated microporous polymers (CMPs), they are a flexible group of crystalline or amorphous organic materials that have long chain of π-conjugation, a large specific surface area, and adjustable heteroatom functionalities. This makes them very useful for capturing CO2 and converting it to electricity. CTFs are prepared via different methods such as iono-thermal or acid-catalyzed trimerization of nitrile monomers. They have stiff, nitrogen-rich structures that allow CO2 to be strongly physiosorbed through Lewis's base–acid interactions and provide coordination sites for anchoring metal centers that are catalytically active. CMPs, which are synthesized by cross-coupling approach, have intrinsic characteristics represented in semiconductivity and hierarchical porosity. This makes it suitable materials for charge and mass transfer in electrochemical systems. CTFs can be modified by molecular catalysts, metal nanoparticles, or single-atom sites to these frameworks makes them even better at electrocatalysis by encouraging selective CO2 activation and multi-electron transfer processes. CTFs and CMPs work together to create a flexible platform for producing new materials that combine selective CO2 adsorption with effective, long-lasting electrocatalytic CO2 reduction (CO2RR) activity.
• With respect to Covalent Organic Frameworks (COFs), they are distinguished as promising materials for integrated CO2 capture and conversion owing to their adjustable porosity, structural adaptability, and chemical stability. Their design enables precise functionalization, improving selectivity and catalytic efficacy. COFs, capable of hosting metal centers and conductive units, effectively facilitate electrocatalytic CO2 reduction, rendering them suitable for sustainable carbon utilization strategies and prospective clean energy applications.
• Considering Zeolites for ICCC, they are shown to be a good and dependable substitute for integrated carbon capture and utilization systems when metal-loaded or nanoconfined zeolites are used to make electrochemical reduction more efficient due to their crystalline microporous structures and adjustable acidity. Also, Zeolites are good at separating and activating CO2 molecules because they are very thermally stable, have a high ion-exchange capacity, and can selectively adsorb certain shapes.
• In the context of Metal–Organic Frameworks (MOFs), they have emerged as a highly promising category of materials for the simultaneous collection and electrochemical reduction of CO2. Their modular structures, which integrate adjustable porosity, elevated surface area, and functionalizable metal–organic linkers, enable the simultaneous enrichment of CO2 and the provision of catalytic conditions for selective conversion. Essential tactics encompass the creation of metal–organic framework (MOF)-based gas diffusion electrodes to augment local CO2 concentration, the design of permselective membranes for targeted CO2 transport, and the incorporation of functional groups, such as amines, to boost capture from dilute gas streams. Moreover, metal–organic frameworks (MOFs) can be engineered to influence product selectivity, such as methane, ethylene, or formate, by altering pore chemistry, metal centers, or interfacial environments. The advancement of conductive MOFs or MOF-derived composites mitigates inherent conductivity constraints, facilitating effective electron transfer and stability in electrochemical environments. These advancements collectively illustrate the adaptability of MOFs as dual-function adsorbent-catalyst systems, establishing a basis for sustainable and scalable carbon usage. Their versatility renders them crucial to contemporary initiatives in merging CO2 collection with CO2RR, providing significant insights for the design of next-generation electrocatalysts.
Regarding Metal Oxides, they have garnered considerable interest as multifunctional materials that can combine CO2 collection with electrochemical CO2 reduction (CO2RR). Their plentifulness, robust basicity, and structural adaptability facilitate excellent CO2 adsorption, especially when altered with amine groups or integrated into porous substrates. In addition to capture, metal oxides are essential in catalysis by activating CO2 molecules, stabilizing critical intermediates, and inhibiting competing hydrogen evolution. Modifying oxide composition and nanostructure has enhanced selectivity for formate (e.g., SnO2, Bi2O3, In2O3) or multi-carbon compounds (oxide-derived Cu). Recent integrated techniques, including amine-functionalized oxides, bifunctional gas diffusion electrodes, and hybrid oxide-metal systems, illustrate the capability of oxides to combine capture and conversion in a singular process, even in dilute flue gas environments. Notwithstanding limitations such as restricted adsorption capacity, stability of functional groups, and the attainment of industrially pertinent current densities, the versatility and scalability of oxide-based systems render them formidable contenders for practical CO2 usage. These advancements collectively underscore the potential of metal oxides as effective, economical materials for enhancing integrated CO2 capture and conversion technologies.
• Regarding Amines electrolytes, Amine electrolytes have served as the pillars of post-combustion CO2 capture (PCC) and early integrated capture-conversion systems because of their cost advantages and chemical reactivity. Nevertheless, their inherent disadvantages, like low ionic conductivity, hydrogen evolution reaction (HER) interference, solvent degradation, and moderate current densities, are significant barriers to long-term sustainability and efficiency. Accordingly, there is a growing tendency toward novel next-generation solvents such as ionic liquids (ILs) and deep eutectic solvents (DESs), with higher CO2 solubility, better electrochemical stability, and tunable physicochemical properties. Such novel solvent systems have promise to enable more efficient, sustainable, and scalable integrated CO2 capture and electrochemical valorization under low-temperature processes such as direct air capture (DAC). Therefore, while amines remain best suited for mature, large-scale systems where cost and reactivity are most important, the future of carbon management is becoming more directed towards ILs, DESs, and hybrid approaches better suited for future generations of carbon capture and conversion technology.
• For Ionic Liquid, Due to their distinct structural features, high CO2 solubility, large ionic conductivity, and broad electrochemical windows, ionic liquids (ILs) are quickly becoming a promising class of solvents for CO2 capture and electrochemical reduction (CO2ER). Researchers can adjust the properties of ILs to achieve the best CO2 capture and conversion performance because of their great diversity, which results from the ability to customize both cations and anions. Recent developments have demonstrated that important limitations of previous IL designs can be addressed by modifying the interactions between ILs and CO2 to further increase absorption capacities and decrease viscosities. While supported ILs, in which ILs are immobilized on solid substrates, offer high capacities, faster adsorption rates, and lower costs, making them appealing for industrial applications, conventional ILs, amino-functionalized ILs, and non-amino functionalized ILs each offer unique mechanisms and performance profiles for CO2 capture. As electrolytes, additives, and electrode modifiers in CO2ER, ILs' potent interactions with CO2 facilitate effective dissolution, activation, and catalytic conversion, frequently improving process efficiency and product selectivity. Future studies should concentrate on methods to maintain the catalytic advantages of ILs while reducing dosage, as this is crucial for industrial scalability due to their comparatively high cost. A deeper mechanistic understanding of IL–CO2 interactions, electric double-layer structures, and co-catalytic effects remains required despite tremendous advancements. This can be accomplished through in situ characterization, molecular simulations, and quantum chemical calculations. Furthermore, machine learning is a promising approach for screening and designing high-performance ILs for CO2 capture and conversion. Overall, ILs offer a versatile and potent platform for sustainable carbon management, and their full potential in useful, large-scale applications will depend on continued innovation in material design, mechanistic understanding, and process integration.
• Referring to deep eutectic solvents (DESs), due to their high CO2 solubility, low toxicity, and environmental friendliness, deep eutectic solvents (DESs) are quickly gaining attention as effective, sustainable alternatives for CO2 capture and conversion. DESs are simple to create from low-cost, bio-based ingredients and have adjustable characteristics that can be tailored for chemical and physical CO2 absorption as well as for incorporation into electrochemical reactions. Recent developments, such as the use of co-solvents, immobilization techniques, and functionalized DESs, are improving performance and scalability, even though issues like high viscosity and limited conductivity still exist. DESs are positioned as a promising platform for upcoming carbon capture and utilization technologies due to their adaptability and environmental credentials.
• In the context of Molten Salts, it combines capturing CO2 and converting it into functional carbon nanomaterials. This process uses carbonate-based electrolytes to directly reduce CO2 at the cathode, producing carbon structures such as nano-tubes, nano-onions, and nano-coils. It has high current efficiency, minimizes byproducts, and offers long-lasting economy. The composition of the electrodes, the chemistry of the electrolyte, and the additives all have a significant impact on the morphology and yield of the product. This makes this method a scalable, CO2-negative way to use carbon and make advanced materials.
Besides that, this comprehensive review consolidates literature to assess the techno-economic analysis and key performance indicators of the ICCC process. Despite recent progress in improving ICCC technologies, there are still considerable challenges: technical limitations such as energy consumption and system efficiency, and non-technical barriers such as high capital costs, lack of economic incentives, public awareness, and inadequate government regulations. Thus, scaling up ICCC from laboratory settings to industrial deployment necessitates further research into cost-effective syntheses of dual-function materials, the development of reactor and separation apparatus design, and holistic evaluations through integrated system-level modeling, life cycle assessment, and techno-economic analysis for performance optimization and economic feasibility.
| AEM | Anion-exchange membrane |
| AFIL | Amino-functionalized Ionic Liquid |
| BET | Brunauer–Emmett–Teller (method for surface area measurement) |
| BGDE | Bifunctional gas diffusion electrode |
| CCUS | Carbon capture, utilization, and storage |
| CMP | Conjugated microporous polymer |
| CNC | Carbon nanocoil |
| DFT | Density functional theory |
| DFM | Dual functional material |
| eCO2R | Electrochemical CO2 reduction |
| EDS | Energy-dispersive X-ray spectroscopy |
| EGR | Enhanced gas recovery |
| EMAR | Electrochemically mediated amine regeneration |
| EOR | Enhanced oil recovery |
| EPRI | Electric power research institute |
| EXAFS | Extended X-ray absorption fine structure |
| FE | Faradaic efficiency |
| GDE | Gas diffusion electrode |
| GPU | Gas permeation unit |
| GWP | Global warming potential |
| HAADF-STEM | High-angle annular dark-field scanning transmission electron microscopy |
| HBA | Hydrogen bond acceptor |
| HBD | Hydrogen bond donor |
| HCP | Hyper-cross linked polymer |
| HER | Hydrogen evolution reaction |
| HOR | Hydrogen oxidation reaction |
| HPC | High-density polyethylene-derived porous carbon |
| HRTEM | High-resolution transmission electron microscopy |
| ICCC | Integrated CO2 capture and conversion |
| ICCU | Integrated carbon capture and utilization |
| ICP | Inductively coupled plasma |
| IEA | International energy agency |
| SBU | Secondary building unit |
| SMR | Steam methane reforming |
| SOC | Solid oxide cell |
| SWCNT | Single-walled carbon nanotube |
| TEA | Techno-economic analysis |
| TOF | Turnover frequency |
| TON | Turnover number |
| TPP | Tetraphenyl porphyrin |
| TRL | Technology readiness level |
| US GAO | US Government Accountability Office |
| NOx | Nitrogen oxides |
| CNS | Carbon nano-scaffold |
| CNT | Carbon nanotube |
| COF | Covalent organic framework |
| CO2RR | CO2 reduction reaction |
| CTF | Covalent triazine framework |
| CVD | Chemical vapor deposition |
| DEA | Diethanolamine |
| DES | Deep eutectic solvent |
| IGCC | Integrated gasification combined cycle |
| IL | Ionic liquid |
| IPCC | Intergovernmental panel on climate change |
| LCA | Life cycle assessment |
| LIB | Lithium-ion battery |
| MDEA | Methyl diethanolamine |
| MFI | Mobil composition of matter no. five (zeolite framework type) |
| MMM | Mixed matrix membrane |
| MOF | Metal–organic framework |
| NPV | Net present value |
| OER | Oxygen evolution reaction |
| OMS | Open metal site |
| ORR | Oxygen reduction reaction |
| PAF | Porous aromatic framework |
| PCP | Porous coordination polymer |
| PEM | Polymer electrolyte membrane |
| PGDE | Permselective gas diffusion electrode |
| PIM | Polymer of intrinsic microporosity |
| POP | Porous organic polymer |
| PTFE | Polytetrafluoroethylene |
| PV | Photovoltaic |
| RCC | Reactive capture of CO2 |
| RDF | Radial distribution function |
| RWGS | Reverse water–gas shift reaction |
| WGSR | Water–gas shift reaction |
| XPS | X-ray Photoelectron Spectroscopy |
| C2H4 | Ethylene |
| CH4 | Methane |
| CO | Carbon monoxide |
| CO2 | Carbon dioxide |
| H2 | Hydrogen |
| H2O | Water |
| HCOO− | Formate |
| N2 | Nitrogen |
| SOx | Sulfur oxides |
| This journal is © The Royal Society of Chemistry 2026 |