Open Access Article
Shayan Gula,
Fatima Nasim
a,
Waheed Iqbala,
Amir Waseem
a and
Muhammad Arif Nadeem
*ab
aCatalysis and Nanomaterials Lab 27, Department of Chemistry, Quaid-i-Azam University, Islamabad 45320, Pakistan. E-mail: manadeem@qau.edu.pk
bPakistan Academy of Sciences, 3-Constitution Avenue Sector G-5/2, Islamabad, Pakistan
First published on 23rd April 2024
Efficient electrocatalytic CO2 reduction reaction (eCO2RR) to various products, such as carbon monoxide (CO), is crucial for mitigating greenhouse gas emissions and enabling renewable energy storage. In this article, we introduce Pd nanoparticles which are deposited over in-house synthesized nitrogen doped tubular carbon (NC) whose ends are blocked with cobalt oxide (CoOx). This composite material is denoted as Pd@CoOx/NC. Among the series of synthesized electrocatalysts, the optimum ratio (Pd@CoOx/NC1) within this category exhibits exceptional performance, manifesting an 81% faradaic efficiency (FE) for CO generation which was quantitatively measured using a gas chromatograph. This remarkable efficiency can be attributed to several scientific factors. Firstly, the presence of Pd nanoparticles provides active sites for CO2 reduction. Secondly, the NC offer enhanced electrical conductivity and facilitate charge transfer during the reaction. Thirdly, the CoOx capping at the ends of the NC serves to stabilize the catalyst, favoring the formation of CO. The remarkable selectivity of the catalyst is further confirmed by the qualitative CO detection method using PdCl2 strips. Pd@CoOx/NC1 exhibits a high current density of 55 mA cm−2 and a low overpotential of 251 mV, outperforming Pd decorated multiwalled carbon nanotubes (Pd@MWCNTs) which shows a higher overpotential of 481 mV. Pd@CoOx/NC1 shows long-term stability at different potentials and rapid reaction kinetics. These findings highlight Pd@CoOx/NC1 as promising CO2 reduction catalysts, with implications for sustainable energy conversion techniques.
For example, Hori et al. reported CO production by using crystalline Pd foil with FE of 28% at −0.8 VRHE.17 Similarly, Gao et al. conducted size-based investigations on palladium nanoparticles and observed a remarkably high FE of 91.2% for CO at −0.89 VRHE.10 Sheng et al. reported noteworthy FE for CO production ∼40% at −0.6VRHE for Pd/C electrocatalyst.18 These findings revealed that the eCO2RR abilities of Pd foil, Pd NPs, and Pd/C catalysts are limited due to their smaller surface areas, particle agglomeration, and carbon corrosion. Furthermore, Pd faces the challenge of CO-poisoning which decreases the CO production rate during eCO2RR.19 A proficient approach to address these challenges associated with eCO2RR involves a systematic sequence of CO2 adsorption,20–22 intermediate formation,23,24 and product removal25,26 on active sites during the electrocatalytic reaction.
The combination of Pd with other metals greatly lowers the CO binding strength by tuning the electronic properties of Pd, leading to facile desorption which in turn increases its production.27 For example, Yin et al. reported improved CO current density on the surface of CuPd NPs with FECO ∼86%.28 Similarly, AgPd NPs have been shown to alleviate the CO poisoning of Pd without scarifying the FECO.27
The pyrolysis of metal organic frameworks (MOF), an ideal precursor for the synthesis of carbon based materials, yields high surface area carbon with a metal oxide or metal nanoparticles disseminated or encapsulated within the ligand-derived matrix.29 The presence of metal within the porous carbon derived from MOF imparts stability and prevents the leaching of carbon during the electrocatalytic process.3,30 MOF derived carbon promotes fast electron transfer and provides redox active sites due to the presence of heteroatoms. These properties make MOF an attractive candidate to be used as a matrix for the uniform dispersion of metal nanoparticles.29 Xi et al. synthesized Fe–N4 sites from Fe doped MOF precursor (ZIF-8). The material exhibited electrocatalytic activity towards CO2RR with FE ∼86.9%.31 Likewise, Wang and co-workers reported nearly 100% FE at −0.9 VRHE for Fe–N–C sites.32
Doping of heteroatoms that have different electronegativities (like; B, N, and P) plays a pivotal role in eCO2RR.33,34 In the realm of heteroatom doping, nitrogen (N) stands out as the most common dopant utilized. Meyer et al. documented the synthesis of nitrogen-doped carbon nanotubes (NCNTs) to enhance the selectivity of eCO2RR towards formate production, achieving an efficiency of 59%.22 Zhou et al. reported that relative to pristine CNTs, graphitic and pyridinic N-containing CNTs enhance the eCO2RR towards CO with lower η (−0.18 V) and higher FECO (80%).35 In the context of eCO2RR, CO2 molecules are initially adsorbed onto basic N-binding sites. Subsequent reduction leads to the formation of *CO2˙− anion radicals. These stabilized *CO2˙− species play a pivotal role in enhancing both activity and selectivity.36
Keeping in view the aforementioned properties, herein we have synthesized cobalt oxide incorporated nitrogen doped tubular carbon (CoOx/NC) originated from zeolitic imidazolate framework-12 (ZIF-12). ZIF-12 contains cobalt ions coordinated with benzimidazolate ligands [Co(PhIM)2]n, exhibiting a metal atom density of 2.01 nm−3. With a diameter capacity of 14.64 Å, its largest cage comprises 48 vertices.37 The extraordinary porosity and stability of ZIF-12 make it an ideal precursor for synthesizing CoOx/NCs with tailored properties. The synthesized CoOx/NC was decorated with palladium nanoparticles by sodium borohydride (NaBH4) reduction technique. The synthesized cost-effective catalysts (Pd@CoOx/NCs) were found to be active for eCO2RR with significant FECO. The Pd nanoparticles provide active sites for CO2 reduction, whereas NCs enhance electrical conductivity, facilitating rapid charge transfer during the reaction, and the CoOx capping at the tubular carbon ends stabilizes the catalyst and may selectively influence the reaction pathway, ultimately promoting CO formation. The CoOx/NC prevents the agglomeration of Pd NPs during the reduction process, making it a highly efficient, antipoisoning, stable, and selective catalyst towards eCO2RR. The method presented here is facile and does not involve multisteps. The effect of CoOx on the Pd NPs for eCO2RR has not been observed yet to the best of our knowledge. This innovative idea solves the challenge of using Pd, a well-known catalyst for CO2 reduction, benefiting from the properties of CoOx/NC. The concentration effect of palladium on the reduction of CO2 was examined by synthesizing a novel series of electrocatalysts with varied palladium concentrations (Pd@CoOx/NCs). The optimized electrocatalyst (Pd@CoOx/NC1) delivered maximum current density (j) with high selectivity for CO.
Palladium chloride (PdCl2) strips, a unique and incredibly efficient technique, were used to qualitatively detect CO gas produced during CO2 reduction. By offering a simple and accurate way to identify and confirm the presence of CO, this novel approach represents a significant improvement in the discipline of chemistry. The method relies on the distinctive color change exhibited by the PdCl2 strips, facilitating easy visual detection of CO. Its simplicity, accuracy, and reliability make it an invaluable tool for CO detection in various chemical reactions.
m space group was exhibited by palladium metal in the synthesized materials. PXRD of all the synthesized materials has been shown in Fig. 1a. The distinguished peak observed at 2θ value of 25.81°, attributed to the (002) plane of graphitic carbon, provides strong evidence for the consistent presence and persistence of graphitic carbon across all the synthesized catalysts. The presence of graphitic carbon is further supported by the identification of two additional peaks at 2θ values of ∼44.41° and ∼51.51° (Fig. 1a), which are aligned with the distinctive pattern documented in the JCPDS card no. 00-013-0148. Due to the low cobalt content (ca. 2 wt%), as found by XPS investigations, the XRD peaks for cobalt oxide (CoOx) have not appeared. However, investigations using high-resolution transmission electron microscopy (HRTEM), XPS, and selected area electron diffraction (SAED) clearly show that CoOx nanoparticles exist.38 The formation of palladium nanoparticles was confirmed by the presence of diffraction rays at 2θ ∼39.61°, ∼44.21°, and ∼68. 11°.
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| Fig. 1 (a) PXRD of all the synthesized electrocatalysts along their JCPDS. XPS data of Pd@CoOx/NC1 (b) Co 2p (c) Pd 3d (d) N 1s. | ||
Table S1† displays the determined cell parameters (a) and the associated d-spacing values obtained for crystallographic planes of Pd ((220), (200), and (111)) by the application of Bragg's law. These calculated results demonstrate a high level of concurrence and conformity with the observations derived from HRTEM analysis. A slight increase in the lattice parameter ‘a’ and d-spacing is noticeable in the synthesized materials compared to fcc-type Pd nanoparticles (Table S1†). This deviation can be attributed to the electronic interaction between palladium and cobalt, resulting in lattice growth. The obtained values indicate metal strain and lattice distortion in the synthesized electrocatalysts, exhibiting a synergistic effect. PXRD of MWCNTs and Pd@MWCNTs has been presented in Fig. S1.†
XPS was utilized to investigate the surface elemental composition, oxidation state, and electronic properties of the optimized electrocatalyst Pd@CoOx/NC1 (Fig. 1). The Co 2p spectrum exhibits a peak for the presence of metallic cobalt at 777.8 eV. The observed peaks at 781.2 eV and 796.9 eV relate to Co 2p3/2 and Co 2p1/2, respectively indicating the cobalt oxidation within the support material (Fig. 1b).38 In Fig. 1c, the XPS spectrum of Pd nanoparticles displays two distinct peaks at 334.8 eV (Pd 3d5/2) and 340.2 eV (Pd 3d3/2). These values indicate that palladium primarily exists in the metallic state. The negative shift in palladium metal binding energy (standard value ∼335 eV) is an indication of electron transfer from cobalt species, resulting in a distinct electronic environment around palladium and a downward shift in its d-band center relative to the Fermi level. The electronegative nature of palladium (E. N ∼2.20) caused the extraction of electrons from cobalt (E. N ∼1.88), which in turn decreased the energy of palladium d-band center due to the increased valence charge on the palladium center.30,39 The observed findings were aligned with the d-band center model, as the palladium metal undergoes a downward shift of its d-band to compensate for the distortion caused by the electronic interaction with cobalt. The two distinct peaks revealed in the high-resolution profile of N 1s at 397.8 eV and 400 eV correspond to pyridinic nitrogen and graphitic nitrogen, respectively (Fig. 1d).38 The high-resolution O 1s spectrum exhibits three peaks at binding energies of 531.3 eV, 533.6 eV, and 535.9 eV, corresponding to oxygen bonded to the metal and surface-bound oxygen species, respectively (Fig. S2a†).38
The deconvolution of the C 1s core level spectrum revealed four peaks. The peaks at binding energies of 284.2 eV and 286 eV correspond to sp2 (C
C) and sp3 (C–C) hybridized carbon, respectively. The remaining peaks at 288.1 eV and 289.4 eV arise from surface-bound oxygen groups (Fig. S2b†).38,40 The XPS analysis of CoOx/NC is presented in Fig. S4.†
HRTEM analysis (Fig. 2) provided a detailed analysis of morphology and structure and showed the presence of distinct cylindrical tubes encapsulating cobalt oxide (CoOx) nanoparticles. CoOx nanoparticles, with a size of approximately 50 nm, are localized at the terminals of NC (Fig. S5†). Upon closer examination of the NC structure, the nanoparticles are observed to be encapsulated within layers of tubular carbon. The tubes exhibit distinct curved growth lines, uniformly bending in the same direction to one another. Growth lines developed as curved layers emanating from the surface of the nanoparticles exhibit a non-concentric configuration (Fig. S5b†). The existence of oxygen and nitrogen heteroatoms in the precursor material promotes carbon condensation at elevated temperatures, leading to the formation of a highly interconnected matrix of tubular carbon with intertwined nodes and internodes. The interconnected nodes are supposed to serve as anchoring sites for the loaded palladium metal nanoparticles, facilitating their immobilization (Fig. S5†). Elemental mapping of Pd@CoOx/NC1 analysis provides conclusive evidence of the presence of cobalt, nitrogen, oxygen, palladium, and carbon within the sample (Fig. 2d–i). Nanoparticles of palladium, characterized by their spherical morphology, exhibit homogeneous dispersion within NC, which also contains embedded CoOx.
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| Fig. 2 (a) HRTEM analysis of Pd@CoOx/NC1 (a) 50 nm (b and c) 10 nm (d) elemental mapping of Pd@CoOx/NC1 (e) C (f) N (g) Pd (h) Co (i) O. | ||
The results obtained deliver conclusive evidence that palladium nanoparticles were successfully deposited onto the CoOx/NC framework. The HRTEM analysis undoubtedly demonstrates the presence of distinct fringes corresponding to the loaded nanoparticles (Fig. 2b and c). The fringes detected in the HRTEM analysis correspond to specific crystallographic planes of the palladium nanoparticles, with d-spacing values of 0.138 nm and 0.204 nm attributed to the (220) and (200) planes, correspondingly. HRTEM analysis findings are aligned with the XRD results presented in Table S1.† Additionally, the EDX pattern of Pd@CoOx/NC1 has been depicted in Fig S3,† which provides further supporting evidence for the deposition of palladium nanoparticles.
The electrochemical active surface area (ECSA) of the catalysts was calculated using the Pd–O reduction process by recording cycle voltammetry (CV) curves at 1.4 VRHE as a function of the higher potential limit (Fig. 3e), amongst all the electrocatalysts examined, Pd@CoOx/NC1 showed the largest ECSA (70.2 cm2) (Fig. 3f). This study highlights the outstanding electrochemical performance of Pd@CoOx/NC1 due to its greater number of active sites readily available for catalytic processes.
Measurements from electrochemical impedance spectroscopy (EIS) provide important information regarding charge transfer resistance. The Nyquist curve of Pd@CoOx/NC1 showed a substantially smaller semicircular diameter, confirming faster charge transfer conductance and lower charge transfer resistance (Fig. 4a). In comparison to other catalysts, Pd@CoOx/NC1 demonstrates higher reaction efficiency and suggests higher catalytic activity for CO2 reduction. Lower charge transfer resistance, faster electron transfer rates, and a more facile CO2 reduction pathway are all attributed to the smaller semicircular diameter. Our findings strongly support the outstanding electrocatalytic activity of Pd@CoOx/NC1 and its ability to work as an effective catalyst for eCO2RR.
The Tafel slope, which gives an idea about the kinetics of the reaction on the surface of an electrode, of all the synthesized electrocatalysts is in the following order. MWCNTs (230 mV dec−1) > CoOx/NC (168 mV dec−1) > Pd@MWCNTs (159 mV dec−1) > Pd@CoOx/NC3 (94 mV dec−1) > Pd@CoOx/NC2 (88 mV dec−1) > Pd@CoOx/NC1 (67 mV dec−1). The lower value of slope indicates better kinetics toward CO2 reduction reaction (Fig. 4b).
A series of controlled potential electrolysis experiments were conducted at various potentials (from −0.3VRHE to −0.9 VRHE) to evaluate the stability of the highly active catalyst Pd@CoOx/NC1 (Fig. 4c). Remarkably, Pd@CoOx/NC1 exhibited outstanding stability for a time duration of 3.20 h (12
000 s) for each potential test. Throughout this period, there was no discernible degradation in catalytic activity, with only a marginal decrease of approximately 2%. This underscores the catalyst's exceptional long-term performance. The high stability and activity of Pd@CoOx/NC1make it a highly suitable candidate to be employed for eCO2RR.
A novel qualitative method, the PdCl2 strips technique, was employed to detect the presence of CO gas produced during the eCO2RR. The method requires 1 N sodium hydroxide, 0.1 N hydrochloric acid, 0.5 N palladium chloride solution, and filter paper. To prepare the PdCl2 strips, a longitudinal strip of filter paper measuring 3 cm × 1 cm is immersed in a 0.5 N PdCl2 solution prepared in 0.1 N HCl and allowed to air dry. Subsequently, 1–2 drops of 1.0 N NaOH are applied to the strip. The prepared strip is then suspended in the cathodic chamber's headspace. As the reaction progresses, the CO produced changes the color of the strip from colorless to black, indicating the interaction with PdCl2. This change in color serves as confirmation of CO production (Fig. S7†).
For the quantitative determination of CO, gas chromatography (GC) analysis was employed. Under controlled potential conditions (−0.7 V vs. RHE) of 3 h, the FE of the optimized electrocatalyst i.e., Pd@CoOx/NC1, was evaluated. At hourly intervals, gaseous samples were taken and analyzed by GC. The resulting chromatogram, shown in (Fig. 4d), provides a thorough picture of how the gas composition changed throughout the reaction. These results highlight the efficiency of Pd@CoOx/NC1 as a catalyst for CO2 reduction processes by providing useful insights into its selectivity and catalytic performance. The outstanding electrocatalytic activity of Pd@CoOx/NC1 in selectively converting CO2 to CO was demonstrated by the FECO of 81%.
The contribution of other liquid electrocatalytic reduced products in faradaic efficiency was evaluated using head space gas chromatographic with flame ionization detector (HS-GCFID). The sensitivity of instrument and method verification was done using positive control. Notably, in the positive control, a peak at a retention time (Rt) of 6.8 min confirmed the presence of formic acid. However, it is noteworthy that no such peak was observed at the same Rt during the catalytic activity, thus excluding the formation of formic acid (Fig. S8†).
Moreover, the determination of other liquid products, such as methanol, ethanol, propanol, and isopropanol, was undertaken utilizing HS-GCFID. Standards for all potential products were run alongside an internal standard (IS) acetone (Fig. S9a†). Upon analysis at various time intervals, solely the peak of the IS was detected, with no evidence of any other products (Fig. S9b†). This observation underscores the selectivity of our catalyst toward CO, thus affirming its efficiency in CO selectivity.
The mass activities (mA/mgpd) of the synthesized electrocatalysts were calculated at different potentials from −0.4 VRHE to −1.0 VRHE. The mass activities of all the electrocatalysts, highlighting their respective performance in the electrocatalytic CO2 to CO conversion process, were observed in the following sequence. Pd@MWCNTs < Pd@CoOx/NC3 < Pd@CoOx/NC2 < Pd@CoOx/NC1(Fig. 4(e)).
Furthermore, turnover frequency (TOF) was calculated at different potentials from −0.4 VRHE to −1.0 VRHE in a CO2 saturated medium. The TOF of Pd@CoOx/NC1 is (1559 s−1) at −1.0 VRHE which is 4.54, 1.93 and 1.33 times higher than Pd@MWCNTs (343 s−1), Pd@CoOx/NC3 (808 s−1) and Pd@CoOx/NC2 (1176 s−1), respectively. The higher TOF value of Pd@CoOx/NC1 indicates a faster rate of catalytic reaction (Fig. 4f). The comparison of Pd-based electrocatalysts with the recent literature has been shown in Table 1.
| Catalysts | V vs. RHE | FE% | References |
|---|---|---|---|
| Pd@CoOx/NC1 | −0.70 | 81 | This work |
| Pd2.4nm | −0.89 | 91.2 | 10 |
| Pd foil | −0.80 | 28 | 17 |
| Pd/C | −0.60 | 40 | 18 |
| Pd85Cu15/C | −0.89 | 86 | 28 |
| Pd7Cu3 | −0.80 | 80 | 41 |
| Pd@Cu2O-2 | −0.77 | 58.3 | 42 |
| Pd5@Au95 | −0.5 | ∼80 | 43 |
| PdAg3 | −0.8 | 96.2 | 44 |
| Pd2 DAC | −0.85 | 98.2 | 45 |
| Pd nanosheets | −0.5 | 94 | 46 |
| Pd icosahedra/C | −0.8 | 91.1 | 47 |
| 4.3 Pd–SnO2 | −1.1 | 78.6 | 48 |
low overpotential of 251 mV, demonstrating its efficiency in promoting CO2 reduction. The catalyst exhibited great stability at various potentials, and the Nyquist plot showed a lower semicircle, indicating enhanced charge transfer kinetics. The outstanding performance, selectivity, and stability of Pd@CoOx/NC1's make it an important material that could contribute towards renewable energy technologies.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra01641f |
| This journal is © The Royal Society of Chemistry 2024 |