Open Access Article
Natalia D.
Loewen
,
Emily J.
Thompson
,
Michael
Kagan
,
Carolina L.
Banales
,
Thomas W.
Myers
,
James C.
Fettinger
and
Louise A.
Berben
*
Department of Chemistry, University of California Davis, CA 95616, USA. E-mail: laberben@ucdavis.edu
First published on 5th January 2016
Proton relays are known to increase reaction rates for H2 evolution and lower overpotentials in electrocatalytic reactions. In this report we describe two electrocatalysts, [Fe4N(CO)11(PPh3)]− (1−) which has no proton relay, and hydroxyl-containing [Fe4N(CO)11(Ph2P(CH2)2OH)]− (2−). Solid state structures indicate that these phosphine-substituted clusters are direct analogs of [Fe4N(CO)12]− where one CO ligand has been replaced by a phosphine. We show that the proton relay changes the selectivity of reactions: CO2 is reduced selectively to formate by 1− in the absence of a relay, and protons are reduced to H2 under a CO2 atmosphere by 2−. These results implicate a hydride intermediate in the mechanism of the reactions and demonstrate the importance of controlling proton delivery to control product selectivity. Thermochemical measurements performed using infrared spectroelectrochemistry provided pKa and hydricity values for [HFe4N(CO)11(PPh3)]−, which are 23.7, and 45.5 kcal mol−1, respectively. The pKa of the hydroxyl group in 2− was determined to fall between 29 and 41, and this suggests that the proximity of the proton relay to the active catalytic site plays a significant role in the product selectivity observed, since the acidity alone does not account for the observed results. More generally, this work emphasizes the importance of substrate delivery kinetics in determining the selectivity of CO2 reduction reactions that proceed through metal–hydride intermediates.
Accordingly, we installed a proton shuttle with weak acidity in the vicinity of the proposed location of the hydride: [Fe4N(CO)11(PPh2(CH2)2OH)]− (2−, Chart 1). We now describe that selective H2 production afforded by this structural modification must arise from proximity of the relay to the intermediate hydride. This is confirmed using the control, [Fe4N(CO)11(PPh3)]− (1−), which produces exclusively formate.
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| Chart 1 [Fe4N(CO)12]−. The “butterfly hinge” bond is Fe2–Fe3. The “butterfly wing” bonds are from Fe4 and Fe1 to Fe2 and Fe3. The “wingtip” atoms are Fe4 and Fe1. | ||
Proton relays have previously been employed to direct selectivity in the reduction of small molecules. In one example, selectivity of CO formation from CO2 reduction was improved using iron–porphyrin complexes with phenol pendants.3,4 In the absence of this outer coordination sphere effect, mixtures of CO, H2 and formate had previously been obtained. Selectivity has also been controlled by carboxylic acid proton relays in both corrole5 and porphyrin6 compounds: and there, O2 reduction to H2O is promoted over H2O2 formation.
Proton relays also enhance rates, decrease overpotentials and promote already selective reactions.7,8 For instance, molecular electrocatalysts with pendant amine bases generate hydrogen with up to 106
000 turnovers per s,9 and “Hangman” porphyrin complexes exhibit lowered proton reduction overpotentials and increased rates.10 Biologically inspired 2Fe–2S clusters incorporate various secondary sphere pendant bases to achieve fast (TOF = 58
000 s−1) H+ reduction and operate at overpotentials as low as −0.51 V.11 The reverse reaction can also be assisted by a proton relay: for example, a molecular Fe catalyst for hydrogen oxidation is catalytic when 1 (TOF = 34 s−1) or 2 (TOF = 290 s−1) proton relays are present.7
Pendant bases are also known to facilitate C–H bond-making and breaking reactions. As examples, a series of Ni(II) compounds with amine bases catalyze formate oxidation at 16 s−1,12via proton transfer from formate to a pendant amine, and in another example, an 2Fe–2S cluster with pendant amine promotes non-catalytic sp3-hybridized C–H bond activation.13
Each of the clusters, 1− and 2−, were characterized by 1H and 31P NMR, and by IR spectroscopy, and combustion analysis which confirmed compound purity. The 31P NMR spectra each show a single sharp resonance approximately 70 ppm downfield from the free phosphine ligand. The signal for 2− is at 49 ppm (Ph2P(CH2)2OH is at −23 ppm) and the signal for 1− is at 67 ppm (PPh3 is at −5 ppm). Similarly, PPN[Fe4N(CO)11(PMe2Ph)] was previously observed at 35 ppm (PMe2Ph is at −44 ppm).14a,15 IR spectroscopic measurements on phosphine-substituted clusters each showed 4 absorption bands compared with 2 bands in [Fe4N(CO)12]−. This is consistent with the expected decrease in molecular symmetry, from approximately C2v to Cs, upon ligand substitution. The IR spectra further indicate that the bands fall between 2038 and 1964 cm−1 for both 1− and 2−, and are at lower energy than in [Fe4N(CO)12]−. We ascribe this to the weaker π-accepting ability of the phosphine ligand compared with the CO ligand.
![]() | ||
| Fig. 1 Solid state structure of 2− in Et4N-2. Grey, blue, red, green, and purple ellipsoids represent C, N, O, Fe and P atoms, respectively. H atoms except OH proton omitted, ellipsoids at 50%. | ||
| ip = (2.686 × 105)n3/2D1/2AC*υ1/2 | (1) |
In eqn (1), n is the number of electrons, A the electrode area (cm2), D the diffusion coefficient for the complex (cm2 s−1), C* the concentration of complex (M), and υ the scan rate (V s−1). CPE experiments were conducted in 0.1 M Bu4NPF6 MeCN/H2O (95
:
5) under 1 atm N2 at −1.4 V. Using either catalyst 1− or 2− the Faradaic efficiency (FE) for H2 evolution was 70 ± 4 and 96 ± 6%. H2 was quantified by GC-TCD analysis of the headspace.
:
5) under 1 atm CO2 at −1.4 V (Table 1). Using 1−, FE for formate production was 61% and for H2 production was 36%. Formate was quantified by proton NMR spectroscopy. The H2 production arises from a background reaction at the GC electrode, and the charge passed for H2 production is the same as the amount of charge passed during control experiments containing no catalyst. CPE experiments with 1− conducted under CO2 in 0.1 M Bu4NPF6 MeCN solutions containing no water did not pass significant charge, and no H2, CO or formate were detected. CPE measurements performed with 2− in 0.1 M Bu4NPF6 MeCN/H2O (95
:
5) under 1 atm CO2 afforded H2, and no detectable CO2 reduction products. We attribute this to the proton relay in 2− which facilitates protonation of the hydride intermediate. As a further control experiment, CPE measurements were performed with 1− in 0.1 M Bu4NPF6 MeCN/H2O (95
:
5) containing 0.2% (1000 molar equivalents) of EtOH, under 1 atm CO2: formate production persisted with 58% FE. In all experiments some of the H2 detected arises from background production by the glassy carbon electrode, but the charge passed during experiments with catalyst is greater than in the control experiment containing no catalyst (Table 1, Fig. S3†). IR spectra collected after electrolysis showed no change to the catalysts (Fig. S3†).
:
5) under 1 atm CO2 over 50 min, with 0.1 mM catalyst. Each experiment performed three times
| Catalyst | q (C) | TON HCO2− | TON H2 | FE (%) HCO2− | FE (%) H2 |
|---|---|---|---|---|---|
| 1 − | 4 ± 2 | 5.4 ± 3 | 3.3 ± 2 | 61 ± 6 | 36 ± 3 |
| 2 − | 16 ± 4 | Na | 40 ± 5 | <3 | 97 ± 5 |
| None | 2.7 | Na | Na | Na | 28 ± 6 |
:
5) was analysed further by CV. We found that the reaction is first order in [1−] and first order in protons and CO2 (Fig. S4†). We also measured the rate of formate formation by 1− using a model described by eqn (2).19![]() | (2) |
In eqn (2), jcat/jp is the ratio of catalytic to noncatalytic current density (mA cm−2), R is the universal gas constant, T is temperature (K), F is Faraday's constant (C mol−1), n is moles of electrons, υ is the scan rate (V s−1), and kobs is the observed rate constant. The peak current density for reduction of 1− to 12− in the presence (jcat, Fig. 3, left) and absence (jp, Fig. 3, right) of CO2 was determined over a series of scans where jcat is independent of scan rate: 0.5 to 0.9 V s−1 (Fig. S5† left). Using eqn (2), kobs is 3.3 s−1.
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Fig. 3 CVs in 0.1 M Bu4NPF6 MeCN/H2O (95 : 5) recorded with varied scan rates, (left) for 1− under 1 atm CO2 and (right) for 0.1 mM 1− under N2. | ||
Taken together, these experiments illustrate that a proton relay on the [Fe4N(CO)12]− reduction electrocatalyst changes product selectivity such that H2 production occurs instead of C–H bond formation with CO2 to give formate. We have previously reported a mechanism for CO2 reduction selectively to formate by the unfunctionalized cluster, [Fe4N(CO)12]−,2 and the data acquired for this present report support an analogous mechanism for CO2 reduction by 1−: reduction of 1− to 12− is followed by protonation to afford the reduced hydride, (H-1)−. Subsequent reaction of (H-1)− with CO2 provides formate and 1. Reduction of 1 back to 1− is facile under the reaction conditions (−1.4 V) since the 10/− couple is estimated at approximately +0.4 V. An accurate value for this couple has not been obtained since the oxidation of 1− (and of [Fe4N(CO)12]−) is irreversible.
Based on the change in product selectivity in the presence of the attached ethanol relay in 2−, we conclude that the proton relay must supply a second equivalent of H+ necessary to generate H2 from (H-2)− (Scheme 1). Our results do not necessarily preclude the possibility that hydrogen bonding interactions by the hydroxyl proton are promoting the observed selectivity but they are consistent with proton relay behavior. In addition, IR-SEC experiments in MeCN on 2− generate small amounts of H2 even without added acid (vide infra): this suggests the proton relay can also protonate 22− in the first step. These observations, along with the kinetic experiments performed using CV and the results of our previously published work on [Fe4N(CO)12]−,2,17 lead to a proposed mechanism for H2 formation by 2− (Scheme 1).
![]() | ||
| Scheme 1 H = H is included in the final step of the catalytic cycle to indicate that the new proton will play the same role in a subsequent cycle. | ||
:
5). The order of reaction with respect to catalysts 1− and 2− under N2 was found to be one (Fig. S6†). With respect to protons, the reaction is second order in each case (Fig. S7†). Rate constants for proton reduction under an N2 atmosphere were also obtained for 1− and 2− using a series of experiments in the presence (Fig. 3 right and S8†) and absence (Fig. S2†) of protons, where jcat was independent of scan rate between 0.3 and 1 V s−1, and between 0.5 V s−1 and 1 V s−1 for 1− and 2− respectively (Fig. S5 right and S8 right†). Eqn (2) yielded rate constants for 1− and 2− which we calculated with the same overpotential, i.e. at −1.51 V and −1.53 V, respectively: the rates of H2 production are 2.0 ± 0.5 s−1, and 4.2 ± 0.1 s−1, respectively. These results demonstrate that the hydroxyl group enables 2− to catalyze reduction of protons to H2 two times faster than 1−.
. When a −1.45 V potential was applied to a solution of 1− the νCO absorption bands associated with 1−, at 2038, 1987, 1972, and 1966 (sh) cm−1 decreased, and new features, ascribed to 12−, appeared at 1879, 1889 (sh), 1920, and 1942 (sh) cm−1 (Fig. 4, left). The isosbestic point is at 1955 cm−1.
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| Fig. 4 Difference absorbance spectra in 0.1 MBu4NPF6 MeCN electrolyzed at −1.45 V vs. SCE, of (left) 1− and (right) 1− with 1 equivalent (0.3 mM) of butyric acid. | ||
Having generated 12−, we investigated its reaction with a weak acid to establish the pKa value for (H-1)−via the thermochemical cycle in eqn (3)–(6):
![]() | (3) |
| BuCO2H ⇌ BuCO2− + H+ pKa(BuCO2H) | (4) |
![]() | (5) |
| pKa = pKeq + pKa(BuCO2H) | (6) |
An IR-SEC experiment was performed on 1− in dry 0.1 M Bu4NPF6 MeCN solution containing 1 equivalent of butyric acid (BuCO2H, pKa = 22.7 in MeCN)22 under 1 atm of H2 (Fig. 4, right). The potential was held constant at −1.45 V vs. SCE to reduce 1− to 12−, and probe the subsequent reactivity of 12− with a weak acid. The resulting IR spectrum contained features at 1878, 1890 (sh), and 1918 (sh) cm−1. The isosbestic point was at 1926 cm−1, compared with 1955 cm−1 observed for the reduction of 1− to 12−. This suggests that no 12− is present and that conversion to (H-1)− occurred. No gas bubbles were observed, and this indicates that no H2 was evolved by protonation of (H-1)−. When a slightly stronger acid (benzoic acid; pKa = 20.7 in MeCN)23 was used, large gas bubbles formed rapidly inside the IR-SEC cell. When 10 equivalents of the weaker acid benzenesulfonamide (pKa = 24.6 in MeCN)22 were used, no H2 formed and the resulting spectra had the same isosbestic point (1955 cm−1) and features as 12− in dry MeCN (Fig. S9†). This provides the upper limit of 24.6 for the pKa of (H-1)−, and we estimate its value as 23.7 ± 1 (Table 2).
The hydricity of (H-1)− was measured by bracketing the value of Keq for eqn (7), and employing the thermochemical cycle outlined in eqn (7)–(11):
![]() | (7) |
| H+ + A− ⇌ HA 1/Kacid | (8) |
![]() | (9) |
![]() | (10) |
![]() | (11) |
Two limiting cases exist – one where the production of H2 is heavily favored (Keq > 10), and one where the hydride intermediate is formed but does not react with excess acid to form H2 (Keq < 0.1). In the IR-SEC experiment described above, under 1 atm H2, these two limiting cases were observed. Use of 1 equivalent of benzoic acid immediately afforded H2 and so the value of Keq (eqn (7)) can be estimated as Keq > 10, which gives hydricity of (H-1)−,
, as < 46 kcal mol−1. In a second experiment 1 equivalent of butyric acid afforded the hydride (H-1)− quantitatively (Fig. 4, right). If 10 equivalents of butyric acid were used, near-complete conversion to the hydride is accompanied by the slow formation of H2, as well as some peaks that correlate to 1− (Fig. S9†). This provides an estimate for Keq as < 0.5, and a limit of
> 45. The hydricity of (H-1)− is thus 45–46, or 45.5 ± 0.5 kcal mol−1 (Table 2).
The hydricity of formate in MeCN is 44 kcal mol−1.21 This means that formate production by (H-1)− is thermodynamically unfavorable by 1.5 kcal mol−1. However it has been shown that hydricity values decrease sharply in aqueous solution,2,24 and that the addition of 5% water to the CV and CPE experiments as described is sufficient to promote thermochemically favorable C–H bond formation with CO2 by (H-1)−.
values for (H-2)−: 23.7 ± 1 and 45.5 ± 0.5 kcal mol−1, respectively. DuBois and coworkers have previously demonstrated that complexes with minor structural modifications exhibit a strong correlation between reduction potential and hydricity values,25 and between reduction potential and pKa values.26 In our own work we see a correlation with reduction potential and hydricity values over the series of clusters: [Fe4N(CO)12]−,22−, and [Fe4C(CO)12]2−.27
To probe the pKa of the hydroxyl group, we first independently synthesized the deprotonated alkoxide Ph2P(CH2)2OLi, and characterized this using 1H, 31P and 13C NMR spectroscopy. We then used 1H NMR (CD3CN) to estimate two limits for the pKa of the hydroxyl proton in PPh2(CH2)2OH (Fig. S10†). In two separate experiments, a solution of PPh2(CH2)2OH in CD3CN was combined with 1 equivalent of either NaOPh (pKa for PhOH is 29.1 in MeCN)28 or NaHMDS (pKa of NaHMDS is 41 in MeCN; NaHMDS is sodium hexamethyldisilazide).29,30 Proton NMR spectroscopy indicated that deprotonation occurred with NaHMDS but not with NaOPh. Therefore, we estimated for PPh2(CH2)2OH that 29 < pKa < 41 in MeCN. Based on eqn (7)–(11), we can calculate from these measurements that ΔG° (eqn (7)) falls between 9.23 and 25.7 kcal mol−1 and predict that the reaction between (H-1)− (or (H-2)−) is unfavorable in MeCN solution. Under the conditions of the CV and CPE experiments, which are in MeCN/H2O (95
:
5) we can estimate that ΔG° (eqn (7)) is even less favorable because we know that
values for our iron clusters drop more significantly than
values for H2 when moving from MeCN into water.2
Previous work involving immobilized proton shuttles has discussed the effect where Brönsted acidic groups attached to a catalyst create a large local proton concentration near the catalyst that has an effective pKa far lower than the measured pKa of the attached acidic functional group.4 Our results obtained measuring the pKa values for PPh2(CH2)2OH and for (H-2)− and (H-1)− indicate that the measured pKa values alone cannot account for the observed reactivity where H2 is produced by 2− while formate is produced by 1−. We conclude that the proximity of the proton relay to the position of the Fe hydride must be a major factor in promoting H2 formation over reaction of (H-2)− with CO2. In addition, the apparently high pKa of PPh2(CH2)2OH could explain why H2 evolution rates we observed with 2− are only enhanced two-fold compared with rates observed for 1− under N2 atmosphere: this is significantly less rate enhancement than observed by others who have employed proton shuttles to promote H2 production.
Space group assignments were based upon systematic absences, E statistics, and successful refinement of the structures. Structures were solved by direct methods with the aid of successive difference Fourier maps and were refined against all data using the SHELXTL 5.0 software package.31d Thermal parameters for all non-hydrogen atoms were refined anisotropically. Hydrogen atoms, where added, were assigned to ideal positions and refined using a riding model with an isotropic thermal parameter 1.2 times that of the attached carbon atom (1.5 times for methyl hydrogens).
Infra-red spectra were recorded in a sealed liquid cell on a Bruker Alpha Infra-red spectrometer. IR-SEC measurements were performed under 1 atm H2 (g), using an optically transparent thin layer solution IR cell fabricated by Prof. Hartl at University of Reading at UK, as described previously.32 In each experiment, electrochemical reduction of the species of interest was monitored by IR spectroscopy for a period of 2–15 min. Diffusion and mixing of the redox products, generated at the working and auxiliary electrodes in the IR cell was reasonably suppressed within the total experimental time. Concentrations of all acids used in IR-SEC measurements were either 0.3 mM or 3.0 mM, and at these low concentrations homoconjugation is negligible (see ESI† for further details).
The working electrode was a glassy carbon plate (Tokai Carbon) with the nominal surface area immersed in solution of 8 cm2. The auxiliary electrode was a coiled Pt wire (BASi). CO2 was obtained from dry ice and transferred to experiments via cannula and tubing. Gas measurements were performed using a gas-tight syringe (Vici) to inject 50 μL to 100 μL gas samples into a Varian 3800 gas chromatogram equipped with a thermal conductivity detector. Gas samples were extracted from a sparged, septum-capped side arm on the working electrode compartment. No CO was detected. In between CPE experiments, the cell and working electrodes were sonicated in 5% v/v nitric acid for 10 min, rinsed, sonicated in methanol for 10 min, rinsed, and sonicated in water for 10 min.
Quantification of formic acid was performed using 1H NMR spectroscopy. An internal standard of a known amount of dimethylformamide, as a dilute solution in 100% C6D6, was prepared and sealed in a glass capillary tube. 500 μL of the CPE solution were injected into an NMR tube with the internal standard capillary. The integration of the 1H resonance at 7.65 ppm for DMF, was used to quantify formic acid produced (8.16 ppm).
Footnote |
| † Electronic supplementary information (ESI) available: Crystallographic data, electrochemical data. 1H-NMR data. CCDC 1418842 and 1418843. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5sc03169a |
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