Roman M.
Mironenko
a,
Dmitry B.
Eremin
bc and
Valentine P.
Ananikov
*acd
aCenter of New Chemical Technologies BIC, Neftezavodskaya St. 54, Omsk 644040, Russia
bBridge Institute and Department of Chemistry, University of Southern California, Los Angeles, 90089-3502, USA
cN. D. Zelinsky Institute of Organic Chemistry, Leninsky Pr. 47, Moscow 119991, Russia. E-mail: val@ioc.ac.ru; Web: https://AnanikovLab.ru
dSaint Petersburg State University, 7/9 Universitetskaya Nab., St. Petersburg, 199034, Russia
First published on 20th November 2023
This review addresses the largely overlooked yet critical issue of “dead” metal in heterogeneous metal catalysts. “Dead” metal refers to the fraction of metal in a catalyst that remains inaccessible to reactants, significantly reducing the overall catalyst performance. As a representative example considered in detail here, this challenge is particularly relevant for carbon-supported metal catalysts, extensively employed in research and industrial settings. We explore key factors contributing to the formation of “dead” metal, including the morphology of the support, metal atom intercalation within the support layers, encapsulation of metal nanoparticles, interference by organic molecules during catalyst preparation, and dynamic behavior under microwave irradiation. Notably, the review outlines a series of strategic approaches to mitigate the occurrence of “dead” metal during catalyst preparation, thus boosting the catalyst efficiency. The knowledge gathered is important for enhancing the preparation of catalysts, especially those containing precious metals. Beyond the practical implications for catalyst design, this study introduces a novel perspective for understanding and optimizing the catalyst performance. The insights are expected to broadly impact different scientific disciplines, empowered with heterogeneous catalysis and driving innovation in energy, environmental science, and materials chemistry, among others. Exploring the “dead” metal phenomenon and potential mitigation strategies brings the field closer to the ultimate goal of high-efficiency, low-cost catalysis.
Supported metal catalysts generally contain metal nanoparticles (NPs) that vary in size from single units to tens of nanometers. This variance is contingent upon the nature of the support, the preparation conditions, and the catalyst's pretreatment. As the size of metal NPs expands, the proportion of surface metal atoms diminishes. It is vital to control the size of metal NPs, as only the metal atoms exposed on the NP surface and accessible to reactants constitute the active sites that govern catalytic activity. Conversely, the metal atoms hidden inside the NPs typically do not engage in the catalytic reaction. Metal atom accessibility (or metal dispersion) could be enhanced by supporting small metal clusters or single metal atoms instead of metal NPs.5 Even in these circumstances, however, a reduction in metal accessibility cannot be entirely dismissed due to spatial constraints imposed by the support surface's structural elements. These elements often present a heterogeneous characteristic, marked by various defects and structural imperfections.
The fraction of the supported metal inaccessible to reacting molecules and, consequently, not contributing to catalytic reactions could be referred to as “dead” metal. This “dead” metal phenomenon is a critical issue often encountered in the practical implementation of supported catalysts. If all the supported metal is inaccessible to the molecules, the catalyst will consequently become inactive in the catalytic reaction. The proportion of “dead” metal in supported catalysts can be ascertained through the chemisorption of probe molecules,6,7 an essential step for accurately estimating the specific catalytic activity and turnover frequency. Many studies employ transmission electron microscopy (TEM) to visualize the formation and location of “dead” metal.7–9 For example, a distinctive indicator of “dead” metal's presence is a significantly larger mean size of metal NPs as determined by the chemisorption of probe molecules (apparent size) compared to that determined by TEM measurements (actual size).
The emergence of “dead” metal in supported catalysts can be attributed to numerous factors, including the micro- and macrostructure of a support, conditions of catalyst preparation, heat treatment, and operational conditions. The possible sources of “dead” metal can be broadly divided into those that are (1) difficult or largely impossible to control and those that are (2) controllable, and in some cases, deliberately applied to render a portion of the metal surface inaccessible. This article will survey the issue of uncontrollable metal accessibility loss and the emergence of “dead” metal, specifically using carbon-supported catalysts as examples. We will omit discussion of specific methods to obtain supported catalysts with partially inaccessible (encapsulated) metal NPs.10–14 Additionally, this work will exclude considerations of catalyst deactivation processes occurring during the catalytic reaction, which lead to an increase in the proportion of “dead” metal (metal sintering and active site blockage due to coking and various types of poisoning). These issues have been thoroughly reviewed elsewhere.15–18
Addressing the issue of “dead” metal is critical from a sustainability perspective. Reduction of the quantity of metal used in catalysts is one of the primary objectives and an existing challenge. Avoiding “dead” metal could facilitate the creation of new catalyst designs with enhanced performance attributes and increased turnover number (TON) or turnover frequency (TOF) values. A further consideration is a substantial improvement in cost-efficiency, an effect most pronounced in the case of precious metal catalysis, such as Ir, Rh, Pd, Pt, etc.
The description of “dead” metal as a term has been used in metallurgy and metal processing scholar literature,19,20 dendrite formation and other processes in batteries,21–23 and soluble metal complexes.24 In heterogeneous catalysis, the term “dead” metal was introduced only recently by our study.25 This review delves into a more comprehensive discussion of the term.
Our focus is on carbon-supported metal catalysts, which are among the most prevalent and broadly utilized catalysts in laboratory practice and the chemical industry. Traditionally, activated carbon (AC) types serve as supports for such catalysts. In addition, a range of carbon nanomaterials—such as graphene, carbon nanotubes (CNTs), carbon nanofibers (CNFs), carbon nanospheres, and nanoglobular carbon (NGC)—are currently of significant interest as structurally diverse and well-defined catalyst supports.26–31 Owing to the structural and morphological characteristics of carbon materials, the effects leading to the emergence of “dead” metal are quite pronounced and varied for carbon-supported catalysts. This makes them a suitable system for studying and discussing the “dead” metal phenomenon. Due to size limitations, only some representative examples are discussed in this brief review in order to highlight the main concept.
Fig. 2 Images of the 3D model of a carbon nanoglobule and a fragment of the model. One could detect the adsorption sites strongly binding metal species on the model surface. Reproduced from ref. 30 with permission of Russ. Chem. Rev. under CC BY license, copyright 2022. |
1. Carbon materials in which micropores are absent or only slightly contribute to the total porosity (graphite, thermal kinds of NGC, Sibunit™) may be used as catalyst supports. For example, a nanostructured carbon–carbon composite material Sibunit™ produced by template synthesis has a mesoporous structure with no micropores and thus combines extensive pore space and a high specific surface area.44,45 This carbon material is successfully used, particularly in producing highly efficient palladium catalysts for the industrial processes of liquid-phase hydrogenation, rosin disproportionation, and furfural decarbonylation.
2. During catalyst preparation, large-sized metal compounds (e.g., metal complexes bearing bulky ligands) may be used as precursors because their migration into micropores is prevented by steric reasons, which facilitates metal localization on the outer surface of the carbon support. As an example, one could point to palladium polynuclear hydroxy complexes (PHCs) that are obtained by hydrolysis of H2[PdCl4] with an alkali metal carbonate in a narrow pH range of 4 to 6:
H2[PdCl4] + K2CO3 → K2[PdCl4] + H2O + CO2, |
mK2[PdCl4] + 2mH2O → {Kn[Pd(OH)2]m}n+ + (2m − n)K+ + 2mH+ + 4mCl− |
Most often, the particles of Pd PHCs are approximately 3.5 nm in size, and therefore, they could not penetrate the micropores of the carbon support. After the deposition of these complexes on the carbon support and subsequent reduction, the resulting Pd/C catalysts contain accessible Pd NPs and show increased activity in hydrogenation reactions.33,46,47
3. To prepare the M/C catalysts, choosing a method that excludes metal migration into micropores is expedient. For example, the deposition–reduction method31,48 ensures the localization of metal NPs on the outer surface of the support since the rate of formation of metal NPs in the solution bulk during the reduction of the metal precursor is much higher than the rate of diffusion of reactants into the micropores of the support.
Nanoglobular carbon (NGC) exemplifies this, where carbon nanoglobule accretion areas and aggregate contact points can be hard to reach (Fig. 1b). In a liquid-phase catalytic reaction, NGC-supported metal catalysts form suspensions, the smallest particle size of which is determined by the carbon nanoglobule aggregate size. Varieties of NGC differ significantly in such aggregate and nanoglobule sizes.30,49 For instance, furnace NGCs consist of tens to hundreds of small nanoglobules (10–80 nm) arranged in branched aggregates, possessing a somewhat developed interglobular space teeming with “dead zones”. Supported metal NPs could be obscured from larger adsorbate or reactant molecules.
The low accessibility of metal localized in the carbon support's “dead zones” can also be circumvented using a single catalyst particle. In recent work, individual 1% Pd/C catalyst particles were separated and isolated from one catalyst batch using a nanomanipulator needle (Fig. 3a).52 For instance, in the 1% Pd/NGC catalyst, such a particle was rounded and contained several thousand Pd NPs. Each isolated catalyst particle was characterized by scanning electron microscopy (SEM), and the analyzed data using a neural network helped determine the number and size of all supported Pd NPs within individual catalyst particles.
Fig. 3 Schematic representation of the characterization and properties of one Pd/C catalyst particle: (a) use of a nanomanipulator to select one catalyst particle; (b) estimation of TONs and loadings for exemplified palladium catalysts in heterogeneous catalytic systems; (c) relationship between TON and the number of Pd atoms in the catalyst particle, according to data of ref. 52, (a) and (b) are reproduced from ref. 52 with permission of American Chemical Society, copyright 2022. The authors prepared (c); no permission was needed. |
Contrary to those in the initial catalyst's entire mass with an increased fraction of palladium localized in the “dead zones”, these Pd NPs were fully exposed. In the Suzuki–Miyaura reaction, single-defined 1% Pd/NGC catalyst particles displayed extraordinary TONs of 107–109, unprecedented in heterogeneous catalysis (Fig. 3b). While isolated 1% Pd/graphite particles were also effective (TONs of 105–107), they were less potent than the 1% Pd/NGC particles. A linear negative relationship was found between TON and the number of Pd atoms in the catalyst particle (Fig. 3c). This is most likely due to the increased size/aggregation of metal nanoparticles and the lower ratio of reactant-accessible metal centers upon enlarged overall metal content.
In the case of carbon nanofibers (CNFs), experiments and model calculations have confirmed the possibility of such penetration by nickel, palladium, and platinum atoms.53–57 This intercalation is especially pronounced with platelet-type CNFs (pCNFs), where the graphene layers are packed perpendicular to the fiber axis, exposing their edges on the fiber surface (a structure often referred to as the card deck structure, Fig. 4a). For instance, Pd/pCNF catalysts showed that palladium atoms could penetrate the bulk of pCNFs, leading to an increased interlayer distance from 3.35 to 3.75 Å at the Pd location. At a relatively low palladium content of 0.04 wt%, the catalyst was inactive in the gas-phase hydrogenation of acetylene (Fig. 4b) due to the complete loss of palladium accessibility to reacting molecules.53
Fig. 4 Carbon nanostructures with different arrangements of graphene layers (a) and performance of Pd/pCNF catalysts with different palladium contents in the gas-phase hydrogenation of acetylene in its mixture with ethylene at 90 °C (b). (a) is reproduced from ref. 28 with permission of the Royal Society of Chemistry, copyright 2015, and (b) is reproduced from ref. 53 with permission of Elsevier, copyright 2012. |
Amorphous carbon can be represented as a low-density coil of randomly connected low-nuclear carbon clusters, where carbon atoms are mainly sp2-hybridized with some contribution from sp- and sp3-hybridization (see Fig. 2).30 Because of its highly disordered structure, amorphous carbon is characterized by increased reactivity and can strongly bind active metal species. Many carbon atoms in amorphous carbon are mobile at relatively low temperatures. As a result, the structure of amorphous carbon is highly labile and can be affected by adsorbates.32 This lability of amorphous carbon can lead to the encapsulation or blocking of active metal NPs (Fig. 1d), which occurs through different mechanisms.
Fig. 5 Palladium NPs with various extents of encapsulation by carbon and bulk carbide formation. Reproduced from ref. 60 with permission of Elsevier, copyright 1998. |
The formation of carbon overlayers on the surface of metal NPs is affected by the initial conditions for forming NPs from the adsorbed precursor.63,64 If metal atoms formed at the high-temperature decomposition of the precursor strongly interact with the carbon surface, the formation of metal NPs from these atoms will be accompanied by their decoration (contamination) with carbon. In the case of rapid nucleation and growth of metal NPs, the interaction between metal and carbon is diminished, preventing such decoration of metal NPs.
It has been demonstrated in previous studies that thermal treatment of Pd/C and Pt/C catalysts at elevated temperatures stimulates the migration of carbon adatoms into the interior of metal NPs. This process results in the formation of metastable carbides that decompose during high-temperature treatment with hydrogen gas. Furthermore, at temperatures exceeding 600 °C, metal NPs promote the graphitization of amorphous carbon contaminants, preventing further sintering of NPs.58–62
The formation and structure of carbon overlayers on the surface of metal NPs in M/C catalysts are largely influenced by the presence of mobile carbon atoms on the surface of the carbon support, the chemical nature of the adsorbed metal precursor, and the conditions of the thermal treatment of the catalyst.
In cases where encapsulation of metal NPs by amorphous carbon cannot be prevented during catalyst preparation, carbon contaminants can be removed by burning them at high temperatures.58–60,63,64 For example, it was shown that the surface of Pd NPs in the 2.8% Pd/NGC catalyst can be cleaned of amorphous carbon through oxidative treatment in a flow of a mixture of 4% O2 and helium at 300 °C, followed by a reduction in hydrogen at 100 °C.58–60 This oxidation-reduction treatment of the catalyst resulted in an almost three-fold increase in TOF in gas-phase benzene hydrogenation.59 However, the heating intensity during such cleaning procedures should be carefully controlled, as there is a risk of sintering metal NPs, which can decrease the dispersion of metal and its accessibility.
During high-temperature treatment processes (such as reduction in flowing hydrogen), the supported precursor, which contains organic ligands, undergoes decomposition into organic products and metal species. Subsequent condensation (or densification) of these organic products forms disordered carbon overlayers that cover the newly formed metal NPs.
This possibility of amorphous carbon deposition on the surface of Pd NPs due to the thermal decomposition of a precursor containing organic ligands was considered in previous studies58,60 while examining 3% Pd/NGC catalysts prepared from palladium(II) acetylacetonate. Similar results were more recently obtained47,51,65 using palladium(II) acetate and tris(dibenzylideneacetone)dipalladium(0), Pd2(dba)3, as precursors to prepare Pd/NGC catalysts containing 1 or 2 wt% Pd. High-temperature reductive treatment of NGC-supported palladium acetate resulted in the formation of Pd NPs that were partially encapsulated by amorphous carbon (Fig. 6a). A more pronounced effect was observed when using the Pd2(dba)3 complex (Fig. 6b), which is expected given that this precursor is rich in carbon (containing 51 carbon atoms for every 2 palladium atoms). In this case, high-temperature treatment in flowing hydrogen led to the complete encapsulation of the formed NPs, which became inaccessible for the chemisorption of CO molecules. As a result, the Pd/NGC catalysts produced from Pd2(dba)3 showed poor activity (in terms of TOF and substrate conversion) in the liquid-phase hydrogenation of nitro compounds and vinyl derivatives. In contrast, similar catalysts obtained from inorganic palladium precursors (H2[PdCl4], Pd PHCs) contained dispersed Pd NPs and exhibited high activity in the same reactions.
Fig. 6 TEM images at different magnifications of the 1% Pd/NGC catalysts prepared by impregnation of the carbon support with solutions of Pd3(OAc)6 (a) and Pd2(dba)3 (b) in chloroform followed by treatment in flowing hydrogen at 300 °C. In both cases, the Pd NPs are encapsulated by amorphous carbon formed during the high-temperature decomposition of these palladium complexes. Reproduced from ref. 47 with permission of Elsevier, copyright 2020. |
It is important to note that although the described mechanism contributes to the encapsulation of metal NPs by amorphous carbon and the heat-induced migration and agglomeration of carbon atoms and clusters from the support surface, carbon deposits that form during the thermal decomposition of supported precursors appear to be more labile and easier to remove by high-temperature oxidative treatment compared to those whose source is the carbon support.58,60
Fig. 7 TEM image of a Pd NP encapsulated in the carbon support by the “shrinkage-following-swelling” mechanism. This NP was formed via spontaneous reduction of aqueous H2[PdCl4] by the surface of the furnace NGC at 20 °C. Reproduced from ref. 32 with permission of CRC Press and Taylor & Francis Group, copyright 2003. |
In this mechanism, newly formed metal NPs are incorporated into the carbon network due to hydrostatic overpressure (disjoining pressure) occurring in the pores and slits when the support grains interact with the impregnating solution. This way of metal encapsulation occurs when a metal precursor is spontaneously reduced by carbon during impregnation with its aqueous solution. For instance, when H2[PdCl4] comes into contact with the carbon support under certain conditions, it produces Pd NPs.30,32,46
Disjoining pressure is primarily related to the repulsion of double electric layers of the pore walls. As a result, the necks of the pores surrounded by disordered carbon fragments are enlarged due to repulsion forces. Consequently, even if the metal NPs are larger than the diameter of the “dry” pores, this enlargement allows for easy penetration of NPs into the pores. Once the solvent evaporates, the pore walls “collapse”, trapping the metal NPs inside.
Under MW irradiation in the presence of an oxidizer (such as air oxygen), metal NPs burn channels into the carbon support surface and penetrate the carbon support bulk (Fig. 1e). In a vacuum (oxidizer-free conditions), nickel and cobalt NPs can burn channels and also catalyze the growth of carbon nanotubes (CNTs), with the metal NPs remaining encapsulated inside the CNTs.
Further studies have shown that MW irradiation in air can create local hot spots on the metal, leading to significantly increased temperatures.68 For instance, this heat causes palladium NPs to melt and move along the basal carbon surface, creating complexly shaped trenches (Fig. 8a). These hot Pd NPs effectively dissolve carbon and catalyze its oxidation to CO2. The NPs also tend to agglomerate and oxidize to form oxide species during these interactions. The movement of Pd NPs along the surface is limited due to stronger binding with the edges of graphene sheets or defective regions of the carbon surface, leading to penetration into the carbon support.
Fig. 8 SEM image of the Pd/graphite catalyst after MW treatment in air for 5 min (a) and NMR monitoring of the Suzuki–Miyaura reaction of 1-bromo-4-nitrobenzene with phenylboronic acid in the presence of Pd/graphite catalysts MW-treated for different durations (b). Reproduced from ref. 68 with permission of American Chemical Society, copyright 2017. |
The dynamic behavior of carbon-supported metal NPs under MW irradiation can potentially introduce “dead” metal, meaning metal NPs that have either penetrated deep into the carbon support or have become encapsulated within the CNTs formed. These NPs are inaccessible to reacting molecules, which could dramatically affect the catalyst's performance.68 For example, even a short 5 minute exposure of a Pd/graphite catalyst to MW irradiation resulted in a nearly 8-fold decrease in the reaction rate between 1-bromo-4-nitrobenzene and phenylboronic acid (Fig. 8b).
Therefore, it is crucial to consider the dynamic behavior of carbon-supported metal NPs under MW irradiation when preparing M/C catalysts or implementing catalytic reactions over these catalysts using MW heating.
Despite these advantages, one notable challenge associated with this method is that the organic stabilizer molecules could strongly adsorb onto the metal surface and thus block the catalytically active sites, impairing their catalytic performance (Fig. 1f). Consequently, there is a need for effective strategies for removing these stabilizers from metal NP surfaces without disturbing their size and shape.31
Fig. 9 Schematic representation of the surface cleaning of shaped metal NPs, which improves their electrocatalytic performance. Reproduced from ref. 72 with permission of Elsevier, copyright 2017. |
In heterogeneous catalysts driven by leaching, the nature of metal centers (single atoms, clusters, NPs) determines the generation of active catalytic centers. Leaching is highly possible from accessible metal sites,4,71,74 but unlikely or even impossible from hindered or “dead” metal areas due to restricted access to solvent and reactants.4 The surface of a metal nanoparticle after leaching reveals a previously inaccessible metal, which could generate new catalytically active sites on the surface of a catalyst.
However, it is essential to note that even trace levels of metal can exhibit high catalytic activity, such as in reactions where the catalyst is used in ppm or ppb quantities.75–78 Palladium contamination, sometimes referred to as “homeopathic” levels of Pd, can also catalyze cross-coupling reactions.76,77,79 It is often present in reagents or labware, and can significantly affect the outcome of the reaction.80
Even though these issues highlight that low metal levels can still lead to successful reactions, it is important to scrutinize the estimations of “dead” metal. Detailed mechanistic investigations, particularly kinetic measurements, can help identify and quantify only the catalytically active species.
In heterogeneous catalyst precursors, determining the speciation, types of active centers, and metal atoms that maintain the active catalytic form is essential.81,82 The diversity and distribution of metal-containing species offer multiple opportunities for analytical measurements. Ex situ techniques offer invaluable insights; however, there is always vulnerability to compromise the environment of a catalyst by means of sample preparation or by the measurement itself. Prioritizing operando studies can help understand the amount of “dead” metal and how to avoid it to prepare a catalyst with maximized metal involvement.
Identifying the causes of metal inactivity is a challenging but necessary task. Therefore, further research is needed to accurately quantify the amount of “dead” metal and understand the reasons behind its inactivity.
Preventing or minimizing the formation of “dead” metal during catalyst preparation is feasible, except for some difficult cases, such as irreversible catalyst degradation due to microwave irradiation. This review also provides possible strategies to “revive” dead metal, which, for instance, include the careful burning out of amorphous carbon that encapsulates metal nanoparticles and the removal of stabilizing organic molecules that block the active surface of metal nanoparticles.
Detailed understanding and controlling factors contributing to the formation of “dead” metal during the preparation of metal-on-carbon catalysts, especially those containing precious metals, represent a major challenge. This knowledge could significantly boost the catalyst efficiency and offer a game-changing approach in the preparation of catalysts.
Particularly notable is the demonstrated advantages of nanoglobular carbon as a support for palladium catalysts. The NGC-supported catalysts exhibit high performance in various hydrogenations30,47,50,51,66 and cross-coupling reactions52,66 with a low palladium content, a significant innovation in the field of catalysis.
Indeed, despite having higher palladium loading, some palladium catalysts supported on activated carbon were less efficient due to the blockage of a portion of the palladium nanoparticles in micropores, rendering them inaccessible to reacting molecules. This issue brings to the forefront the need for optimizing catalyst preparation procedures to reduce the catalyst's palladium content by minimizing or preventing the appearance of “dead” palladium.
This review reflects the necessity for a paradigm shift in our understanding of heterogeneous catalysts. It extends beyond just metal-on-carbon catalysts, and the strategies discussed here to prevent the formation of “dead” metal are broadly applicable to other metal catalysts supported on different materials.
The analysis provided here could be a gateway towards creating highly efficient metal catalysts with a maximized amount of “alive” metal involved in the catalytic process. The novelty and impact of this research are undeniable, and it lays the groundwork for a new generation of catalysts composed exclusively of “alive” metal. The concept presented here offers a path towards more efficient, cost-effective, and sustainable catalysis, which will have profound implications for numerous industrial processes.
While our research underscores the paramount significance of optimizing metal efficiency and decreasing inaccessible metal fractions, we urge researchers to apply rigorous considerations. The precise methods and general strategies for catalyst preparation, tailored for specific metal size/dispersion, remain deeply interconnected with the individual catalytic processes in focus. The efficiency characteristics of a catalyst are intricately linked with the specific reaction and its operating conditions. It is pivotal to acknowledge that the proportion of inaccessible metal can be influenced not only by pretreatment protocols but also by dynamic processes that arise during the catalytic reactions themselves. We strongly caution against an oversimplification of our discussions, applying them broadly across heterogeneous catalyst varieties and processes. Instead, we advocate for a nuanced, case-specific examination of the ideas presented herein, ensuring their relevance and adaptability to distinct catalytic systems and conditions.
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