Marco Nazareno
Dell'Anna‡
ab,
Geet
Gupta‡
ab,
Prathamesh T.
Prabhu
ab,
Ting-Hung
Chu
ab,
Luke T.
Roling
*ab and
Jean-Philippe
Tessonnier
*ab
aDepartment of Chemical and Biological Engineering, Iowa State University, Ames, Iowa 50011, USA. E-mail: tesso@iastate.edu; roling@iastate.edu
bCenter for Biorenewable Chemicals (CBiRC), Ames, Iowa 50011, USA
First published on 20th September 2023
The decarbonization of chemical manufacturing is a multifaceted challenge that requires technologies able to selectively convert CO2-sequestering feedstocks using renewable energy. The electrochemical conversion of biomass is well-positioned to address this need. However, the electroactivity of biobased molecules that carry multiple redox centers remains challenging to predict and control. For instance, cis,cis-muconic acid, a conjugated dicarboxylic acid, is electrohydrogenated to trans-3-hexenedioic acid (t3HDA) with excellent yield and stereoselectivity while free energy calculations predict mixtures of 2- and 3-hexenedioic acids. To decipher this discrepancy, we studied the electrohydrogenation of C4 and C6 unsaturated acids, diacids, and their esters, and tied the observed product distributions to the electronic structure of the parent molecules. We show that the electrohydrogenation of the three isomers of muconic acid proceeds through a hydrogenating proton-coupled electron transfer (PCET) in the α position of the carboxylic acids and invariably yields t3HDA as the sole product. The selectivity can be explained by the electron-withdrawing effect of the carboxylic acid groups and the resulting perturbation of the local electron density that promotes the 2,5-hydrogenation over the thermodynamically-preferred 2,3-hydrogenation. This electronic perturbation is reflected in the computed Fukui indices, which can serve as local reactivity descriptors to predict product distributions not captured by calculated reaction thermochemistry. In addition to predicting the electroactivity of other unsaturated acids, this approach can provide insights into homogeneous electrochemical processes that may coexist with surface-mediated electrocatalytic transformations.
The past few years have seen breakthroughs in the electrosynthesis of various commodity chemicals from CO2, including formic acid, ethylene, and ethylene oxide.6–13 Progress in the electro-conversion of biomass has also enabled the synthesis of C3–C6 compounds—e.g., higher alkenes, furanics, phenolics, and diacids—with good yields and faradaic efficiencies.5,14–20 Electrochemical hydrogenation (ECH) plays an increasingly important role in these transformations as unsaturated functionalities, in particular carbonyl (CO) and alkenyl (CC) groups, are ubiquitous in biobased molecules whether derived from lignocellulosic biomass or produced using microbial cell factories.
Notable biobased platform molecules include unsaturated (di)carboxylic acids—fumaric, levulinic, itaconic, and muconic acids—that can be hydrogenated to produce monomers key to the manufacture of polyamides and polyesters.15,21–25 Their ECH is typically performed using the same platinum-group metal catalysts as for thermocatalytic hydrogenations (TCH).16,18 However, surface-mediated ECH presents several important advantages over TCH: (i) hydrogen is generated in situ from water instead of supplied by H2; (ii) the reaction proceeds under ambient conditions with reduced mass transfer limitations as H* is generated directly at the surface of the catalyst; and (iii) the various modes of electric current delivery—potentiostatic, galvanostatic, rapid alternating polarity, etc.—offer additional degrees of freedom to common reaction parameters such as temperature and pressure to finely control selectivity.16,20,26
In contrast to TCH, ECH can also proceed in the absence of a platinum group metal catalyst, albeit through a different reaction pathway that involves concerted or sequential proton-coupled electron transfers (PCET) in solution. This approach is particularly valuable to process feedstocks containing biogenic impurities that can irreversibly poison metal catalysts at ppm levels.27 For instance, fermentation broths present nitrogen- and sulfur-containing amino acids that deactivate common hydrogenation catalysts like Pd/C and Pt/C at concentrations as low as 50 ppm.27–30 Such deactivation is suppressed in the case of liquid-phase PCET as the reaction is not mediated by the electrode surface.
Our group has recently demonstrated that cis,cis-muconic acid (ccMA) produced from sugars or lignin monomers using metabolically-engineered microorganisms can be directly hydrogenated in its fermentation broth through PCET by reusing the broth's inorganic salts and water as electrolyte and hydrogen sources.27,31–33 This process intensification strategy minimizes chemical waste and improves process economics.32 The reaction produces the corresponding monounsaturated trans-3-hexenedioic acid (t3HDA) with excellent yield, stereoselectivity, and faradaic efficiency at an estimated cost of $1.75 kg−1, close to adipic acid's 10 years average price of $1.60 kg−1.27,34 Like adipic acid, t3HDA can be used as a monomer to manufacture polyesters and polyamides, and its double bond can be leveraged to enable the design of polymeric materials with performance advantages. For instance, t3HDA's double bond can be used to tether pendant groups and build in desired properties like hydrophobicity and flame retardancy without compromising the mechanical properties of the parent polymer.23,35
The selectivity observed for the liquid-phase PCET hydrogenation of ccMA is unexpected as TCH and surface-mediated ECH produce mixtures of the cis and trans isomers of 2- and 3-hexenedioic acids as intermediates to adipic acid (Scheme 1). This selectivity could not be explained theoretically, as the computational tools needed to quantitatively predict the chemoselectivity of electrochemical reactions are underdeveloped. Linear correlations have been established between molecules’ lowest unoccupied molecular orbital (LUMO) energies, electron affinities, and redox potentials.36–38 However, the tools available do not provide information on the reactivity of individual redox sites within a molecule.
Herein, we address this gap by studying experimentally and theoretically the liquid-phase ECH of CC in biobased chemicals with multiple redox sites. We compare the selectivity of the reaction for C4–C6 monoacids, diacids, and their esters at different pH to correlate redox activity and chemoselectivity with the substrate's molecular structure and protonation state. This work highlights how neighboring electron-donating and withdrawing functional groups alter the hydrogenation of CC and control the selectivity of the PCET process. It also highlights how thermochemistry fails to predict the observed selectivity and how, instead, the electrophilicity of the carbon atoms captured by Fukui indices explains the experimental results.
As can be seen in Fig. 1, the first H-addition to fully protonated ccMA is expected to take place on the carbon atom in the α position of the carboxylic acid. This addition has a reaction free energy of 0.00 eV at −0.48 V vs. Ag/AgCl, which is more favorable than addition at the β carbon by 0.50 eV at pH 1. The subsequent hydrogenation on the β carbon to form cis-2-hexenedioic acid (c2HDA), the 2,3-hydrogenation product, is energetically favored (ΔG = −1.35 eV) over the 2,5-hydrogenation that would yield t3HDA (ΔG = −1.21 eV). The calculations also revealed that further hydrogenation is disfavored by the energy barrier for the third proton–electron addition, such that the reaction may not readily occur at moderate potentials without a catalyst. Therefore, either c2HDA or a mixture of c2HDA and t3HDA were expected through PCET, which is inconsistent with the corresponding experiments as t3HDA was the only product detected.
The speciation diagram for ccMA revealed that diprotic, monoprotic, and deprotonated ccMA (for clarity labeled ccMAH2, ccMAH−, and ccMA2− in Fig. 2a) coexist near pH 3.5 but that diprotic muconic acid and deprotonated muconate dianions are the dominant species below pH 3 and above pH 5, respectively. This speciation and the absence of any side reactions (e.g., coupling) enabled us to identify the onset potentials of the various compounds when increasing pH from 1 to 7 and understand how reactivity changes with the protonation state of the molecule (Fig. 2b). At pH 1, protonated ccMA (ccMAH2) exhibited an onset potential at −0.57 V vs. Ag/AgCl that can be easily distinguished from the reduction of hydronium ions to H2via the acidic Volmer–Heyrovsky mechanism at −1.38 V (Fig. 2b and c).39 At around pH 2–3, mass transfer limitations depleted MA species and hydronium ions near the cathode's surface giving rise to a diffusional plateau that is also visible in the polarization curves collected for the blank electrolytes between ca. −1.5 and −2.2 V (Fig. 2c). Above pH 3, new onset potentials appeared at −1.55 V and −2.18 V (Fig. 2b), corresponding to the hydrogenation of ccMA dianions and water reduction following the alkaline Volmer–Heyrovsky mechanism, respectively. Increasing the pH further from 3 to 7 shifted the onset potential for water reduction by less than −0.10 V, in good agreement with the literature on HER.40,41
The lack of distinct onset potential for the hydrogenation of the monoprotic acid (ccMAH−) is likely due to the pKa values for ccMA being too close to distinguish the two deprotonation events. This observation is consistent with prior attempts to titrate ccMA.42 Alternatively, kinetic modeling performed for the isomerization of ccMA to ctMA provided ranges of possible pKa values for ccMA, namely, 2.8 < pKa1 < 4.4 and 4.2 < pKa2 < 5.0 at 22.5 °C.42 These values and the corresponding speciation diagram (Fig. 2a) explain the decrease in current observed for the plateau at −1.6 < Ewe < −1.0 V with increasing pH (Fig. 2b). Specifically, the current changed only slightly at pH 1–2 because ccMAH2 was the only species in solution and the reaction was not limited by [H3O+]; the reaction was solely limited by the diffusion of ccMAH2 under these conditions. At pH 3, the drop in [ccMAH2] and [H3O+] concentrations caused more substantial changes to the LSVs and their independent contributions were estimated from the polarization curves for the blank electrolyte. As Fig. 2c revealed a transition from proton reduction to water reduction for HER at pH 3, H2O was expected to also become the main source of hydrogen for ECH at this pH. Therefore, pH and [H3O+] were not expected to play any role in the change in current observed at −1.6 < Ewe < −1.0 V at pH > 3. This implies that current was controlled by the mass transport of ccMAH2 and ccMAH− for 3 < pH < 5. Above pH 5, ccMA2− became the dominant species, which suppressed the diffusional plateau at −1.6 < Ewe < −1.0 V and gave a single onset potential for ECH at −1.55 V. A new diffusional plateau also appeared at −2.2 < Ewe < −1.6 V corresponding to the mass transport of ccMA2−.
We further investigated the involved reaction mechanism(s) by analyzing the polarization curves relative to the reversible hydrogen electrode (RHE) and standard hydrogen electrode (SHE). Fig. 3a shows a perfect overlap under the RHE scale for the first onset potential in the LSVs collected at pH 1–3. This overlap reveals that the shift observed in Fig. 2b follows the Nernst equation and corresponds to a change of 59 mV per pH unit.43 It also supports a PCET process involving an equal number of protons and electrons as:
E(RHE) = E(Ag/AgCl) + 0.197 + 0.059 × (m/n) × pH | (1) |
Fig. 3 pH-Dependent current–potential polarization curves on Pb RDE for 0.5 g L−1ccMA relative to (a) RHE and (b) SHE scales. |
Overall, these experiments show that the transition from strong (COOH) to weaker (COO−) electron-withdrawing groups causes a nearly 1 V shift to stronger (more negative) reduction potentials with increasing pH. Admittedly, the deprotonation of ccMA also makes it more difficult for the substrate to approach the cathode due to the electrostatic repulsion between the negatively charged electrode and the muconate dianion. In Marcus theory, this additional work impacts the activation energy of the reaction. To address this point, we extended the dataset to other unsaturated diacids and their methyl esters.
Fig. 4 pH-Dependent current–potential polarization curves on Pb RDE for (a) maleic acid, (b) fumaric acid, (c) dimethyl maleate, and (d) dimethyl fumarate. The same colors were used for all figures for clarity and the legend is shown in Fig. 4d. |
Maleate and fumarate methyl esters were studied in order to further understand the role of pH when protonation and deprotonation of the carboxylic groups can be excluded (Fig. 4c and d). For both esters, the current–potential curves shifted by −0.25 V and −0.40 V for the maleate and fumarate methyl esters, respectively, when increasing pH from 1 to 7. The shift in overpotential was swift and occurred around pH 2–3, which is consistent with a transition from H3O+ to H2O as a hydrogen source for ECH. Surprisingly, the curves did not show the expected Nernstian shift of 0.059 mV per pH that was observed for the diacids at low pH. The most likely explanation is that the reaction is kinetically controlled by the charge transfer rather than by proton transfer for the esters. This interpretation is consistent with the higher overpotential measured at pH 1 for the maleate and fumarate esters (−0.87 V and −0.60 V, respectively) compared to the diacids (−0.58 V), and esters being weaker electron-withdrawing groups than carboxylic acids.
To this point, it can be concluded that the concentration of hydronium ions and the transition from H3O+ to H2O as a source of hydrogen play a relatively modest role on the ECH of unsaturated diacids, with a shift in overpotential on the order of −0.25 V when increasing the pH from 1 to 7. In contrast, the deprotonation of terminal carboxylic groups had a more pronounced effect evidenced by a −1.0 V shift to higher overpotentials. These experimental values are consistent with the computed change in hydrogenation energetics when increasing pH (Fig. 1). Considering the same intermediates along the energetically favored pathway from ccMA to adipic acid at pH 1, the free energies for ccMA initial hydrogenation shifted by 0.18 eV from pH 1 to 3, and by 0.92 eV from pH 1 to 7. Experimentally, the onset potentials for ECH were also found to follow the trend COOH > COOR ≫ COO−, which is in line with the electron-withdrawing capacity of these terminal groups (COOH > COOR ≫ COO−). Overall, they increased the electrophilicity of carbon atoms in α positions and thereby played a critical role in the kinetics of the ECH reaction. In the case of ccMA, these effects may also kinetically control the selectivity to t3HDA by facilitating the 2,5- over the 2,3-hydrogenation pathway.
Polarization curves were recorded at pH 7 for both ccMA and SA to avoid any contributions from [H3O+] and/or differences in the protonation state of the molecules. As can be seen in Fig. 5, a 0.35 mV shift to higher overpotentials was observed for SA compared to ccMA, which is consistent with a lower electrophilicity for the carbon atom next to the methyl group and deactivation of the γ,δ-double bond. Similar results were obtained when comparing the polarization curves of SA (trans,trans-2,4-hexadienoic acid) and of trans,trans-muconic acid (Fig. S2†).
Bulk electrolysis was carried out to investigate the role of terminal groups on ECH selectivity. As ccMA and SA present very different onset potentials, we carried out these experiments under kinetic control by applying a constant current density of 100 mA cm−2. Unsurprisingly, the bulk electrolysis of ccMA produced t3HDA with 100% selectivity (Fig. 6a). In contrast, the bulk electrolysis of SA gave two distinct isomers (Fig. 6b), 3-hexenoic acid (3HA) and 4-hexenoic acid (4HA). The selectivity of the reaction and absence of any other products such as 2-hexenoic acid (2HA) and hexanoic acid was confirmed by 1H NMR and HSQC NMR (Fig. S3 and S4†).
Both hexenoic products formed with a 3HA:4HA ratio of approximately 1:1 during most of the experiment, which indicates the coexistence of parallel PCET reaction pathways and the absence of any isomerization between 3HA and 4HA. Interestingly, the reaction proceeded through 2,5- and 2,3-addition of hydrogen to form 3HA and 4HA, respectively, but there was no sign of 4,5-addition that would yield 2-hexenoic acid (2HA). This observation suggests that the first H+|e− pair was likely added to C2 (in α of COOH) due to the electron-withdrawing effect of the carboxylic acid. In the absence of a second terminal COOH, like in ccMA, there is no preferred position for the addition of the second H+|e− pair and, therefore, 2,3- and 2,5-additions proceed simultaneously. The observed selectivity also suggests that electron-donating groups like –CH3 may completely suppress the reactivity of neighbouring CC. This contrasts with the reactivity of carbonyl-containing compounds where isolated CO were proven to react even if isolated, e.g., in glucose or levulinic acid.44
To further assess the role of the terminal –CH3 group on reactivity, we studied the hydrogenation of crotonic acid, a C4 unsaturated acid with a molecular structure similar to maleic and fumaric acids. Crotonic acid was specifically chosen because the molecule presents a single CC bond advantageously positioned between terminal –COOH and –CH3 groups. As anticipated, 1H NMR revealed no conversion even after 2 hours of bulk electrolysis at high current density (200 mA cm−2), see Fig. S5.† These results confirm the role of –CH3 in compensating the electron-withdrawing effect of COOH observed for the C4 diacids (maleic and fumaric acid), suppressing all electroactivity for this conjugated monoacid.
Our experimental results revealed that liquid-phase PCET hydrogenation reactions are primarily controlled by charge transfer in the case of unsaturated (di)acids, i.e., by a molecule's ability to accept electrons during sequential electron and proton transfers. Therefore, we expected that the onset potential for ECH should be correlated with the energy of the molecule's LUMO based on Koopman's theorem, as reported in a similar fashion for other electrochemical reactions.36–38 Building on this concept, we computed the LUMO energies for ccMA, SA, and their respective ECH reaction intermediates.
The LUMO energy of ccMA was computed to be 0.825 eV (Fig. S7†). The LUMO energies of the subsequent hydrogenation intermediates and products are all similar, ranging from 1.267 eV to 1.312 eV. Interestingly, the α-hydrogenated intermediate, through which t3HDA can form, has a slightly lower LUMO energy (1.287 eV) than the alternative β-hydrogenated radical (1.294 eV) that only yields c2HDA. The LUMO energy of t3HDA is also lower than that of c2HDA (1.267 eV vs. 1.312 eV).
The calculated LUMO energy of SA was 1.260 eV (Fig. S8†); this higher value than ccMA correlates with the more negative onset potential for the ECH of SA compared to ccMA. The singly-hydrogenated intermediates capable of forming the experimentally-observed products have again lower LUMO energies (1.264 eV and 1.278 eV) than the other intermediates (1.288 eV and 1.296 eV). Moreover, 3HA and 4HA have lower LUMO energies than the 2HA product that is not observed experimentally (1.278 eV and 1.274 eV vs. 1.309 eV, respectively).
The LUMO energies qualitatively agree with the selectivity observed for the bulk electrolysis of ccMA and SA (Fig. 6); however, this analysis has limited quantitative insight and does not provide the atomic-level detail required to understand the effects of electron-withdrawing groups (i.e., –COOH vs. –CH3) on molecular reactivity. As the hydrogenation of CC involves primarily the 2p orbitals of the corresponding carbon atoms, we also compared the LUMO 2pz eigenvalues of the reactants and various reaction intermediates (Fig. S9†). Baran and coworkers recently used these LUMO coefficients to rationalize the exceptional selectivity observed for the reduction of carbonyl groups in molecules with multiple redox centers using rapid alternating polarity (rAP).45 In this case, we do not find strong correlations between the 2pz eigenvalues and the experimentally-observed products (Fig. S9†). For ccMA, the initial elementary hydrogenation at the α position, which can lead to the formation of t3HDA, would occur at a site with a LUMO coefficient of 0.12 (in contrast to −0.11 at the β position). However, the subsequent hydrogenation would have to occur at a site with LUMO coefficient of −0.01 to yield t3HDA, instead of at a site with a coefficient of 0.15. Similar issues are observed for the LUMO coefficients in the SA reaction network: the β-carbon has the highest coefficient (0.15), though addition at that position would preclude formation of the experimentally-observed 3HA. The LUMO coefficients therefore fail to explain the product distributions obtained experimentally.
We speculate that the discrepancy with prior works (e.g., Baran) comes from the sequence of events involved in the hydrogenation of unsaturated acids. Specifically, our experiments showed a much stronger impact of pH on inductive effects (1.0 V shift to higher overpotentials when transitioning from COOH to COO−) than on hydrogen source (0.25 to 0.40 V shift when transitioning from H3O+ to H2O as a hydrogen source). This suggests that the ability of a carbon atom to accept an electron, hence its electrophilicity, and the molecule's ability to form a “stable” intermediate may be better captured using Fukui functions.
The Fukui function describes changes in the electronic charge density of a molecule due to addition or removal of an electron from the system; a higher value of the Fukui function indicates a more reactive site within the molecule. Our Fukui function analysis indicated that the hydrogenation of ccMA at one of the α carbons (Fukui index 0.16) is more favorable than at the β position (0.11), allowing formation of the intermediate leading to t3HDA due to the electron-withdrawing nature of the –COOH functionality (Fig. 7a). The Fukui index for the subsequent hydrogenation at the δ position (0.28) is more positive than that for the β position (0.25); while the two sites are linked by a resonance structure, the electron-withdrawing nature of the –COOH group near the δ position again improves the electrophilicity of that site, rationalizing the formation of t3HDA observed experimentally instead of c2HDA. The Fukui function analysis also explains the formation of 3HA and 4HA from SA (Fig. 7b). The Fukui-preferred addition at the α position (0.18, favored due to the proximity to –COOH over 0.16 at the δ position near –CH3) yields an intermediate capable of forming only 3HA or 4HA (not 2HA), the only products observed experimentally. That intermediate formed by α hydrogenation shows a slight preference for formation of 4HA based on the Fukui indices of the respective carbon atoms (0.33 vs. 0.31), once again driven by the electrophilicity of the site nearest the –COOH functionality. Overall, the atomic-scale detail offered by the Fukui function demonstrated the strongest connections to the observed experimental product distributions, providing atomic-level insights into the effects of molecular geometry and inductive effects on the reactivity of conjugated (di)acids.
The polarization curves recorded for unsaturated C4 and C6 (di)acids and esters, and the selectivity observed during bulk electrolysis revealed that the source of hydrogen (H3O+ or H2O) has a limited impact on the overpotential of the ECH reaction (∼0.25 V vs. Ag/AgCl) and no effect on its selectivity. In contrast, the deprotonation of terminal groups with increasing pH increased the overpotential by about 1.0 V due to carboxylates (COO−) being weaker electron withdrawing groups than carboxylic acids (COOH). Substituting a terminal –COOH by –CH3, an electron-donating group, in sorbic acid further shifted the onset potential and promoted the formation of both 3-hexenoic acid and 4-hexenoic acid, i.e., the 2,5- and 2,3-addition products, while only 2,5-hydrogenation was observed for ccMA. Lowering the distance between –CH3 and CC in crotonic acid completely suppressed ECH.
Computed free energies fail to predict the preferred reaction pathways and selectivity for these transformations, likely due to the inductive effects of terminal carboxylic acids on charge transfer during the addition of H+|e− pairs. To account for these effects, we computed LUMO energies and LUMO 2pz eigenvalues, but found they provided at best qualitative information on molecular reactivity. Computations ultimately demonstrated the utility of Fukui indices in describing the selectivity of ECH for both ccMA and SA, providing accurate local descriptors for predicting liquid-phase PCET transformations.
These advancements will benefit ECH beyond the molecules studied in the present work. In particular, Fukui indices provide a fast and reliable approach to predict reactivity and selectivity based on electronic structure calculations of only the reactant molecule. Moreover, the same approach can be applied to discriminate liquid-phase PCET hydrogenation and surface-mediated hydrogenation pathways that may coexist in electrocatalytic systems. Last, the local descriptors identified through this work are not unique to PCET processes; they are applicable to other electro-organic redox transformations governed by electron transfer.
Bulk electrolysis was carried out using a two-compartment Micro Flow Cell® reactor purchased from ElectroCell (Amherst, NY). The reactor was equipped with a Pb plate working electrode, platinized titania counter electrode, and the two compartments were separated by a Nafion membrane. Each electrode had an exposed surface area of 10 cm2. The reactions were performed galvanostatically at a current density of j = −100 mA cm−2 using 100 ml of solution that was looped through the reactor at 180 ml min−1 using a Fisherbrand™ GP1000 pump (ThermoFisher). These experiments were conducted at pH 7 as the solubility of organic acids is drastically reduced at low pH. Aliquots of 600 μL were withdrawn every 15 minutes for the first hour, then every 30 minutes for an additional 4 hours.
The computational hydrogen electrode (CHE) theory proposed by Nørskov and coworkers was utilized in this work to account for the effects of applied potential.56 Through this method, the reversible hydrogen electrode (RHE) was taken as a computational reference, with hydrogen gas in equilibrium with protons and electrons at a potential of 0.0 VRHE. Since the proton source at low pH (H3O+) costs no energy for the hydrogenation using CHE, the potential-dependent change in free energy for an elementary hydrogenation step (A + 0.5H2 ↔ AH) was therefore calculated as:
ΔG = GAH − GA − 0.5GH2 + |e|URHE | (2) |
The pH-dependent potential values reported in this work are provided relative to the Ag/AgCl refence electrode according to the following equation:
EAg/AgCl = ERHE − 0.197 V − 0.059 V × pH. |
Footnotes |
† Electronic supplementary information (ESI) available: Additional electrochemical results, NMR spectra of reactants and products, additional DFT energetics and analyses. See DOI: https://doi.org/10.1039/d3gc02909c |
‡ These authors contributed equally to this work. |
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