L. Mauricio Murillo-Herrera* and
Ana B. Jorge Sobrido
School of Engineering and Materials Science, Queen Mary University of London, Mile End Rd, London E1 4NS, UK. E-mail: l.m.murilloherrera@qmul.ac.uk; a.sobrido@qmul.ac.uk
First published on 22nd August 2025
Deep eutectic solvents (DES) are gaining interest as promising electrolytes for vanadium flow batteries due to their tuneable solvation properties, high solubility for ionic species, and their potential green credentials, but their application has been limited to a few formulations, based on ethylene glycol and urea, which are neutral/alkaline DES. Taking into consideration the vanadium redox mechanism in aqueous media, we hypothesized that exploring acidic formulations could improve the redox performance of V(IV/V) posolytes. Here, for the first time, we investigate the effect of binary and tertiary acidic type III DES formulations on the electrochemical kinetics of the V(IV/V) redox couple. Cyclic voltammetry revealed that acidic DES moderately improved anodic performance, but significantly destabilized the cathodic process compared to a neutral hydrogen bond donors, which exhibited better cathodic reversibility. Hydroxyl groups were found to stabilize the cathodic process, likely through coordination to vanadium species, whereas carboxylic acids improved anodic kinetics, but increased cathodic irreversibility. Furthermore, the aqueous dilution of the DES strategy was not found to be universally beneficial since high water loadings were observed to destabilize the redox system. The best performing ternary mixture, consisting of choline chloride, ethylene glycol and malonic acid in 1:
2
:
2 molar ratio, exhibited a peak-to-peak separation comparable to aqueous acidic electrolytes, but lower operational currents. The improvements were attributed to the balance between pH modulation and viscosity reduction. These new findings highlight the competing effects of viscosity, solvation, speciation and pH on vanadium redox chemistry and provide useful insights on the need to balance these properties to enhance charge transfer and reversibility in the design of DES formulations for flow battery applications.
Broader contextDeep eutectic solvents (DES) have recently emerged as promising electrolytes for flow batteries, offering advantages such as high ionic species solubility, intrinsic ionic conductivity, large electrochemical windows, low toxicity, non-flammability, and task-specificity. Despite their huge molecular flexibility, the application of DES to flow batteries remains narrowed to very few archetypic formulations. Although promising, these electrolytes suffer from high charge transfer and mass transport resistance and overall poor electrochemical performance. Our study explores how modulating DES pH by incorporating carboxylic acid-based formulations, the availability of hydroxyl functional groups, and the mass fraction of the DES components impacts the electrochemical performance of the vanadium(IV/V) redox couple, which is used as the catholyte in vanadium flow batteries. We demonstrate that while organic acids enhance anodic kinetics, they destabilize the cathodic process, whereas polyol-based DES improve cathodic reversibility. Among the ternary formulations studied, certain mixtures exhibited electrochemical reversibility comparable to commercial aqueous vanadium electrolytes, though with lower operational currents, highlighting the challenges of achieving high electrochemical reversibility in DES-based systems. These findings provide valuable insights into how electrolyte composition influences vanadium redox chemistry, which is critical for advancing DES-based flow battery technologies |
In sulfuric acid solution, a coupled electrochemical/chemical mechanism (EC) has been proposed for the V(IV/V) redox process according to reactions (1)–(4). The vanadyl cation undergoes a Nernstian oxidation to VO3+ species (1), which is then quickly hydrolyzed to form the dioxovanadium(V) cation VO2+ (2). In the reverse process, VO2+ undergoes a sluggish reduction to VO2 (3), followed by reaction with hydronium ions to generate water (4). The modelling of this EC mechanism suggests that transfer coefficients for the overall forward (anodic) and reverse processes are close to 0.5.3–5
VO2+ → VO3+ + e− | (1) |
VO3+ + H2O → VO2+ + H2O + 2H+ | (2) |
VO2+ + e− → VO2 + H2O + 2H+ | (3) |
VO2 + 2H+ → VO2+ + H2O | (4) |
Deep eutectic solvents (DES) are mixtures of Brønsted–Lowry or Lewis acids, also known as hydrogen bond donors (HBD), and bases, also known as hydrogen bond acceptors (HBA). These mixtures are characterized by significantly lower melting points than their individual components. Recently, DES have gained attention in energy storage due to their potential for low toxicity, high biodegradability, high metal salt solubility, ionic conductivity, and design flexibility with over 106 possible combinations.6
One of the key constraints in conventional aqueous electrolytes is the limited solubility of vanadium species, which directly impacts energy storage capacity. DES provide a highly tuneable solvation environment, allowing for enhanced vanadium solubility beyond the limits of traditional sulfuric acid-based systems. Additionally, by carefully designing the solvent composition, it is possible to modulate pH and speciation of the electroactive molecule, to disable side reactions, and to enhance charge transfer kinetics, ultimately leading to higher energy density and improved electrochemical performance.7
Type III DES—comprising quaternary ammonium halides and hydrogen bond donors (e.g., polyols, amides, organic acids)—are being explored as electrolytes in batteries, but despite their huge structural flexibility, the application of DES in flow batteries has remained narrowed to mixtures of choline chloride (ChCl) with ethylene glycol, glycerol and urea, the three main archetypes of the DES third type (Fig. 1).8 The inorganic chemistries studied in type III DES for battery applications were all-Cu,9 hybrid all-Fe,10–12 all-V(acac),13,14 Zn/Ce,15 Zn-ion16 and V/Fe.17–19 All these batteries were demonstrated in static mode, to the best of our knowledge the only DES-based flow battery system was reported by Nayanthara et al. using the all-V chemistry type III DES diluted with sulfuric acid and dopped with carbon nanotubes.20 Type IV DES, typically composed of hydrated metal halides and hydrogen bond donors, have been applied as negolytes in Zn(II)/Zn(0)21 and Al(III)/Al(0)21–24 systems, and as posolytes in Fe(II)/Fe(III) systems.25 Although promising, these electrolytes suffer from high viscosities and low conductivities, which in consequence leads to high cell polarisation resistance, low efficiencies, high pressure drop and low operational currents.
Here we explore for the first time a potential strategy to overcome the kinetic limitations of V(IV/V) posolytes in the archetypical ethylene glycol and urea DES by formulating several acidic type III DES as supporting electrolytes. Since the proposed reaction mechanism in aqueous solution involves proton-transfer steps, we hypothesized that by modulating the pH of the HBD, we enhance the vanadium charge-transfer kinetics. Moreover, ternary mixtures consisting of the base type III DES with water or other HBDs could reduce the electrolytes viscosity and increase the electrochemical performance. Additionally, we postulate that the chloride-rich environment of the DES could stabilizes the V(V) species, which could allow the operation of the posolyte at temperatures above 40 °C, as suggested by previous research on aqueous media.26–28
The chosen acidic DES were ChCl/AA (1:
2) where ChCl is choline chloride and AA acetic acid, ChCl/MA (1
:
1) where MA stands for malonic acid and AcChCl/AA (1
:
2), where AcChCl is acetyl choline chloride. MA is nearly two orders of magnitude stronger acid than AA (pKa for the first proton-transfer reaction of malonic acid is 2.83 whereas for acetic acid is 4.76), however ChCl/MA (1
:
1) is an order of magnitude more viscous than ChCl/AA (1
:
2).6,29 Carboxylic acid-based DES can undergo side reactions even at room temperature, such as esterification between carboxylic acid and alcohol-based HBDs or with the alcohol group from the cholinium cation, while MA can undergo cracking, producing AA even under mild temperatures.30–32 This irreversible chemical step suggests that ChCl/MA (1
:
1) is not suitable as a supporting electrolyte. However, for the purposes of this investigation, ChCl/MA (1
:
1) provided higher acidity than AA, while being less viscous than other dicarboxylic acid-based DES with similar pKa, such as oxalic acid or levulinic acid. While the cracking of MA is eventually unavoidable, the esterification reaction is an equilibrium process that can be modulated and potentially leveraged by adjusting the water content in the solvent. For example, a high-throughput analysis of various DES formulations, showed that those based on acetylcholine chloride exhibited higher conductivities than their choline chloride-based counterparts, suggesting that controlled esterification is a valuable strategy to tune DES properties for high performance battery applications.33
DES | W1 | W2 | W3 |
---|---|---|---|
ChCl/EG (1![]() ![]() |
0.53 | 0.47 | — |
ChCl/AA (1![]() ![]() |
0.54 | 0.46 | — |
ChCl/MA (1![]() ![]() |
0.57 | 0.43 | — |
AcChCl/AA (1![]() ![]() |
0.60 | 0.40 | — |
ChCl/EG/H2O (1![]() ![]() ![]() ![]() |
0.51 | 0.46 | 0.03 |
ChCl/EG/H2O (1![]() ![]() ![]() ![]() |
0.50 | 0.44 | 0.06 |
ChCl/EG/H2O (1![]() ![]() ![]() ![]() |
0.47 | 0.41 | 0.12 |
ChCl/EG/H2O (1![]() ![]() ![]() ![]() |
0.42 | 0.37 | 0.21 |
ChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.52 | 0.45 | 0.03 |
ChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.50 | 0.43 | 0.07 |
ChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.47 | 0.41 | 0.12 |
ChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.42 | 0.36 | 0.22 |
ChCl/MA/H2O (1![]() ![]() ![]() ![]() |
0.55 | 0.41 | 0.04 |
ChCl/MA/H2O (1![]() ![]() ![]() ![]() |
0.53 | 0.40 | 0.07 |
ChCl/MA/H2O (1![]() ![]() ![]() ![]() |
0.50 | 0.37 | 0.13 |
ChCl/MA/H2O (1![]() ![]() ![]() ![]() |
0.44 | 0.33 | 0.23 |
AcChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.58 | 0.39 | 0.03 |
AcChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.57 | 0.38 | 0.06 |
AcChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.54 | 0.36 | 0.11 |
AcChCl/AA/H2O (1![]() ![]() ![]() ![]() |
0.49 | 0.32 | 0.19 |
ChCl/EG/AA (1![]() ![]() ![]() ![]() |
0.48 | 0.42 | 0.10 |
ChCl/EG/AA (1![]() ![]() ![]() ![]() |
0.43 | 0.38 | 0.19 |
ChCl/EG/AA (1![]() ![]() ![]() ![]() |
0.36 | 0.32 | 0.31 |
ChCl/EG/AA (1![]() ![]() ![]() ![]() |
0.28 | 0.25 | 0.48 |
ChCl/AA/EG (1![]() ![]() ![]() ![]() |
0.48 | 0.41 | 0.11 |
ChCl/AA/EG (1![]() ![]() ![]() ![]() |
0.43 | 0.37 | 0.19 |
ChCl/AA/EG (1![]() ![]() ![]() ![]() |
0.36 | 0.31 | 0.32 |
ChCl/AA/EG (1![]() ![]() ![]() ![]() |
0.27 | 0.24 | 0.49 |
ChCl/MA/EG (1![]() ![]() ![]() ![]() |
0.51 | 0.38 | 0.11 |
ChCl/MA/EG (1![]() ![]() ![]() ![]() |
0.46 | 0.34 | 0.20 |
ChCl/MA/EG (1![]() ![]() ![]() ![]() |
0.38 | 0.28 | 0.34 |
ChCl/MA/EG (1![]() ![]() ![]() ![]() |
0.28 | 0.21 | 0.50 |
ChCl/EG/MA (1![]() ![]() ![]() ![]() |
0.44 | 0.39 | 0.16 |
ChCl/EG/MA (1![]() ![]() ![]() ![]() |
0.30 | 0.26 | 0.44 |
100 mM solutions of VOSO4·xH2O (97%, Sigma Aldrich, UK) in each DES sample were prepared. TGA analysis was carried out to determine the water content in the vanadium salt, consistently around 27.5 wt%. VOSO4 did not solubilize in the DES at room temperature. Hence the mixtures were stirred at 60 °C until obtaining homogeneous solutions. The stored solutions remained homogeneous for several months, but eventually precipitation of VOSO4 was observed.
The transfer coefficients were calculated based on each peak's half-peak-width parameter (ΔEp–p/2) considering irreversible kinetics according to eqn (1), with R the ideal gas constant (J mol−1 K−1), T the temperature, a the transfer coefficient and n the number of exchanged electrons, which was assumed as 1.34 Both CV parameters are reported as the average over all scan rates. The diffusion coefficient of the V(IV/V) species were obtained via the irreversible Randles–Ševčík analysis of the ip vs. relationship, according to eqn (2), with A the electrode geometric area, C the electroactive species bulk concentration (mol cm−3), D the diffusion constant of the electroactive species (cm2 s−1) and v the scan rate (A s−1).34 All ip vs.
plots and Ep vs. log(v) plots used to calculate the peak potential shift rates are displayed in the SI. The heterogeneous rate constant (ks) was estimated using the Kinglier and Kochi model for irreversible kinetics, which only depends on the peak-to-peak separation (ΔEp), the transfer coefficient of the forward process and the diffusion coefficient of the species undergoing the forward process according to eqn (3).35,36 The reported rate constants represent the average over all scan rates.
![]() | (1) |
![]() | (2) |
![]() | (3) |
The redox properties of the V(IV/V) couple in the ternary mixtures were evaluated using CV. The comparative analysis was performed using the performance metrics obtained at a scan rate of 50 mV s−1 as well as the peak shift rates across 5 to 200 mV s−1. Each parameter was normalised between 0 and 1 by scaling to the maximum value obtained for each dilution series and the results represented in radar plots. The CVs from all ternary mixtures between 5 mV s−1 to 200 mV s−1 is displayed in the SI.
Previous spectroscopical characterization of concentrated vanadyl solutions in hydrochloric acid did not reveal significant differences due to chloride coordination to the vanadyl core.28 However, Furman and Garner reported that it was necessary to increase the concentration of chloride anions in aqueous solution to at least 20 times that of the hexaaquovanadium(III) complex or 100 times the concentration of the pentaaquovanadyl(IV) to observe meaningful changes in the electronic absorption spectrum, thus indicating that the chloride anion marginally coordinates to the vanadyl cation in aqueous solution.40 Moreover, previous characterization of the [VOCl4]2− anion in Cl-based ionic liquids identified two bands at 859 and 739 nm associated with B2 to B1 and B2 to E transitions respectively; and two weak extra bands at 430 nm and 364 nm associated with the transition from B2 to A1.41,42 In our experiment, the vanadyl cation was highly diluted with a Cl− to VO2+ ratio of ∼1200. In this diluted vanadyl solution, a broad wave centred at 737 nm was observed, likely arising from the convolution of the expected bands. The high energy bands were not detected, probably obscured by the strong charge-transfer absorption and the solvent absorption. The electronic absorption spectra of the vanadyl cation in ChCl/EG (1:
2) and ChCl/AA (1
:
2) exhibit the same characteristic broad wave centred at 740 nm. The onset of the charge-transfer absorption takes places at lower energy in HCl compared to H2SO4 and then again, at lower energy in DES compared to HCl. This is attributed to the lower degree of solvation of the vanadyl complex in DES. Both DES exhibited another wave at 390 to 395 nm. In ChCl/EG (1
:
2), this band was four times more intense than in the case of ChCl/AA (1
:
2). Neither of these features were observed in aqueous solutions of the DES components in a ratio of 7
:
1 with respect the vanadyl cation. In those cases, the spectra resembled that of the sulfuric acid solution. Therefore, the spectroscopical characterization shows that the vanadyl species exists as chlorovanadyl complexes in ChCl-based DES.
Entry | DES | (mV dec−1) | (mV dec−1) | ΔEp,a–p/2 (mV) | ΔEp/2–p,c (mV) | αa | ks (cm s−1) × 10−8 | DV(V) (cm s−2) × 10−8 | DV(V) (cm s−2) × 10−8 |
---|---|---|---|---|---|---|---|---|---|
αc | |||||||||
a 30 °C.b 60 °C. | |||||||||
1a | ChCl/EG (1![]() ![]() |
65 ± 5 | 179 ± 22 | 91 ± 5 | 206 ± 24 | 0.53 ± 0.03 | 0.23 ± 0.21 | 0.52 ± 0.06 | 0.58 ± 0.09 |
0.23 ± 0.03 | |||||||||
2b | ChCl/EG (1![]() ![]() |
33 ± 2 | 25 ± 7 | 84 ± 2 | 130 ± 5 | 0.63 ± 0.02 | 4.63 ± 1.00 | 2.27 ± 0.21 | 0.87 ± 0.08 |
0.41 ± 0.02 | |||||||||
3b | ChCl/AA (1![]() ![]() |
29 ± 2 | 162 ± 23 | 82 ± 2 | 185 ± 18 | 0.65 ± 0.02 | 1.59 ± 1.63 | 4.96 ± 0.43 | 2.17.±0.30 |
0.29 ± 0.03 | |||||||||
4b | ChCl/MA (1![]() ![]() |
51 ± 1 | 52 ± 2 | 92 ± 4 | 162 ± 10 | 0.58 ± 0.03 | 11.28 ± 0.44 | 0.83 ± 0.09 | 0.42 ± 0.05 |
0.33 ± 0.02 | |||||||||
5b | AcChCl/AA (1![]() ![]() |
22 ± 2 | 329 ± 19 | 75 ± 4 | 198 ± 52 | 0.71 ± 0.03 | 0.03 ± 0.03 | 5.39 ± 0.53 | 1.24 ± 0.30 |
0.28 ± 0.06 |
The V(IV/V) anodic process was characterized by peak A(I) maximum located around 1.04 V in ChCl/EG (1:
2) at 30 °C (all potentials are reported against the saturated Ag/Ag/Cl electrode) and a peak-to-half-peak width (ΔEp–p/2) value of 91 mV (Table 2, entry 1). At faster scan rates, the peak shifts towards anodic potentials at a rate of 65 mV per decade. The residual anodic current (RAC) increased linearly with the applied overpotential from an onset potential of 0.41 V for 5 < v < 50 mV s−1, which suggests an earlier unresolved irreversible anodic process. The cathodic peak C(I) was characterized by a broader width (ΔEp–p/2 = 206 mV). The onset was observed at around 0.50 V vs. Ag/AgCl. The peak centre was observed around 0.05 V vs. Ag/AgCl and shifted towards cathodic potentials at faster scan rates at a rate of 179 mV per decade. A shoulder centred around 0.30 V vs. Ag/AgCl was detected only at scan rates between 5 and 50 mV s−1, which could indicate that the broadness of the cathodic peak is due to the convolution of two irreversible reduction processes.
The overlap of the supporting electrolyte background CV with the electrolyte containing VOSO4 suggested that the presence of vanadium disfavoured the oxidation of chloride from the solvent. The background CV showed higher anodic and cathodic currents at potentials close to the electrolysis barrier compared to the experiment with vanadium (Fig. S1 in SI). The transfer coefficients of the forward and reverse pathways were not complementary (αa + αc < 1). The analysis suggested that the merge of C(I) and C(II) generated a convoluted broad wave. Since the calculation of the transfer coefficient depends on the peak ΔEp–p/2 parameter, the convolution of the two peaks resulted in an underestimation of the cathodic transfer coefficient.
The ΔEp(I) values ranged from 841 mV to 1164 mV between 5 and 200 mV s−1. Therefore, obtaining ks values in the order of 10−9 cm s−1. The Kinglier and Kochi model assumes the transfer coefficients are complementary (αa + αc = 1) and that the peaks related by ΔEp(I) correspond to the forward and reverse steps of the same redox process. Therefore, the convolution of the cathodic peaks makes the interpretation of the heterogeneous rate constant challenging, because the calculated αc does not strictly correspond to the reverse process of the V(IV/V) oxidation. Despite the lack of complementarity in the transfer coefficients, the rather small ks values were consistent with similar systems previously reported in the literature. For context, Pardo et al. calculated ks for the FeCl2/FeCl3 pair in ChCl/EG (1:
2) at 25 °C using Pt electrodes obtaining values of ks ≈ 10−7 cm s−1.43 The ΔEp of their redox process was ∼120 mV with a transfer coefficient of 0.57. Since the iron redox process follows a simpler outer-sphere electron transfer mechanism than V(IV/V), it is reasonable for the latter to display ks that are orders of magnitude lower.
Due to the low water concentration of DES, which is largely committed to the solvent's hydrogen bond network, the VO3+ intermediate species generated after the Nernstian oxidation of VO2+ likely reacts directly with the alcohols present in the DES, forming a mixture of vanadium(V) chloroalkoxide complexes rather than undergoing hydrolysis.44 These chemical reactions may contribute to the overall irreversibility of the electrochemical process by rearranging the active V(V) species or by depleting its concentration at the electrode surface due to poorer solvation. This way, the redox reaction would limited by the slowest of the solvolysis reactions, as such the coupling of a second order rate law to the electron-transfer process predicts a peak shift rate of 19.7 mV per decade.34 However, all the studied anodic processes exhibit larger peak shift rates, suggesting that the EC mechanism alone does not fully account for the irreversibility of the redox process.
The V(V) species can undergo several side reactions. For instance, the reduction of VOCl3 by alcohols and specific carboxylic acids such as propionic or n- and iso-butyric acid has been reported in organic solvents, leading to mixtures of chloroalkoxide vanadium complexes.45
Dent et al. reported that dissolving VOCl3 in 1-ethyl-3-methylimidazolium chloride ionic liquid, resulted in the formation of [VOCl4]2− instead of [VOCl4]− attributed to V(V) deoxochlorination.42 The same study also reported the disproportionation between [VO2Cl4]2− and [VCl6]3− to obtain [VOCl4]2−.
In chloride-rich aqueous media, at high states of charge, i.e., at near quantitative oxidation to V(V), the Nerst equation predicts a positive shift of the V(IV/V) redox potential, which may promote the reduction of VO2+ by chloride anions. However, previous research on highly concentrated aqueous acidic electrolytes have not found substantial deoxochlorination of VO2+.26–28
In our experiments, the observed RAC is unlikely to originate from the V(III/IV) redox couple. Even if observed at similar redox potentials, this is not commonly seen, due to sluggish electrochemical kinetics. Instead, we attributed this activity to vanadium adducts originating from solvolysis reactions following the anodic process.
Additional experiments were conducted at 60 °C to assess the impact of electrolyte temperature on the electrochemical performance. Previous characterization of the V(II/III) redox couple in DES demonstrated an improvement in electrochemical reversibility and available currents at 55 °C compared to room temperature.46 Operating vanadyl electrolytes in sulfuric acid at high temperatures is not advised, as dioxovanadium(V) cations dimerize and precipitate above 40 °C.47 However, it has been reported that chloride anions stabilize V(V), preventing precipitation.26–28 At higher temperature, the reduction of Cl became more evident, following the DESs anodic oxidation barrier, as a shoulder located at ∼0.8 V (Fig. 2c). The cathodic current associated with the reduction of the solvent anodic products varied with the cutoff potential, i.e. it depends on how much solvent was electrolyzed.
The temperature increase promoted a nearly threefold improvement of the anodic current peaks and overall positive effect on the anodic process. The anodic peak potential A(I) was observed −70 mV with respect to the peak at 30 °C. The peak shift rate was reduced in ∼50% and the ΔEp–p/2 value in ∼10% (Table 2, entry 2). RAC was still observed between 0.30 V and 0.75 V. However, this was evident at all scan rates studied, which supports the idea that this current originates from a sluggish vanadium oxidation preceding V(IV/V).
The previously observed broad cathodic wave was resolved into two reduction peaks C(I) and C(II) centred around 0.31 V and −0.03 V respectively. C(I) shifted slightly across the studied scan rates (25 mV per decade), whereas C(II) appeared only as residual current at scan rates below 50 mV s−1. Rising the temperature also promoted a 50% reduction in C(I) peak's ΔEp–p/2 parameter. ΔEp(I) ranged between 581 mV at 5 mV s−1 and 680 mV at 200 mV s−1, which still suggests complete irreversibility, but shows an enhancement compared to 30 °C. The transfer coefficients calculated from each peak's ΔEp–p/2 parameter resulted in (αa + αc ≈ 1). Increasing the temperature had a positive but differentiated effect on the diffusion constant of the V species, showing a fourfold increase for V(IV), but only 50% increase for V(V). Also, the rate constant increased an order of magnitude, driven by the reduction of the ΔEp parameter. Overall, the vanadyl cation exhibited a complex electrochemistry in ChCl/EG (1:
2). Naturally, increasing the temperature from 30 °C to 60 °C promoted an increase of the peak currents, lower overpotential and resolved the convoluted cathodic wave into at two clear reduction processes. Based on these observations, the following experiments were conducted at 60 °C. This temperature also provided a more realistic comparison with ChCl/MA (1
:
1), due to its higher viscosity. The voltammograms from the acidic DES at 50 mV s−1 are shown in Fig. 2d. A(I) in ChCl/AA (1
:
2) was observed at potentials around 0.830 V and showed ∼50% larger currents despite ChCl/AA (1
:
2) being slightly more viscous than ChCl/EG (1
:
2) (70 vs. 37 mPa s at 25 °C).6,29 The anodic peak shift rate and ΔEp–p/2 parameter showed only marginal improvements with respect to ChCl/EG (1
:
2) (Table 2, entry 3). In this case, RAC was also observed at potentials between 0.35 V and 0.66 V. However, this was more noticeable in ChCl/EG (1
:
2).
The cathodic activity of ChCl/AA (1:
2) was characterized by two processes. Unexpectedly, the onset of reduction was observed at slightly lower potentials than in ChCl/EG (1
:
2) and the first peak was located at potentials around 0.07 V, which translated into larger reduction overpotentials despite the acidity of the solvent. The C(I) shift rate and ΔEp–p/2 parameters also resulted significantly larger than in ChCl/EG (1
:
2). Finally, C(II) was prominent at scan rates above 50 mV s−1 similarly as observed for ChCl/EG (1
:
2). Based on the previous metrics, the ΔEp(I) value ranged from 565 mV at 5 mV s−1 to 867 mV at 200 mV s−1, reinforcing the idea that in this DES, the cathodic process was more irreversible than ChCl/EG (1
:
2). The transfer coefficients were close to complementarity (αa + αc ≈ 0.95). The deviation from unity was due to the relatively large cathodic ΔEp–p/2 values. A twofold increase in the diffusion coefficients of V(IV/V) were also observed, which explains the improvements in peak currents. However, a twofold decrease of the rate constant compared to ChCl/EG (1
:
2) was calculated, mainly driven by larger ΔEp(I) values. The large shift rate of the cathodic peak potential also contributed to the high uncertainty of the rate constant, which was calculated as an average of the rate constant at each scan rate.
The anodic region of the V(IV/V) redox process in ChCl/MA (1:
1) was characterized only by the A(I) with no traces of RAC at lower potentials. The peak shift rate and the ΔEp–p/2 resulted slightly larger than the previously studied electrolytes at 60 °C, due to the DES high viscosity. The cathodic region exhibited two peaks: C(I) at 0.43 V and C(II) at 0.28 V. C(I) was observed to shift towards more negative potentials at a rate of 51 mV per decade, while C(II) remained relatively constant which caused a merge of both peaks at scan rates above 50 mV s−1, leading to a broadening of the main cathodic peak, with ΔEp–p/2 values comparable with ChCl/AA (1
:
2) (Table 2, entry 4). The V(IV/V) process in ChCl/MA (1
:
1) exhibited ΔEp(I) values between 540 mV at 5 mV s−1 and 683 mV at 200 mV s−1, similarly as observed for ChCl/EG (1
:
2), but the diffusion coefficient values were comparable to those in ChCl/EG (1
:
2) at 30 °C due to the larger viscosity of this DES. The transfer coefficients resulted not close to complementarity (αa + αc ≈ 0.91) due to the cathodic peak broadening. Moreover, the anodic peak ΔEp–p/2 was ∼12% larger than the previous DESs, which resulted in a transfer coefficient value of αa = 0.58. Although this value could suggest a more symmetrical potential energy surface (αa closer to 0.5), the interpretation should be taken with care, as the broadening of the anodic peak could simply be a consequence of the larger viscosity, which would explain why ChCl/EG (1
:
2) at 30 °C also displayed similar transfer coefficient values. Regardless, αa and ΔEp(I) were the main promoters of a nearly three-fold increase of the calculated rate constant compared to ChCl/EG (1
:
2) at 60 °C.
Finally, the CVs of the V(IV/V) process in AcChCl/AA (1:
2) exhibited ∼9% larger ip values than ChCl/AA (1
:
2), whereas the onset of oxidation was observed at practically the same potentials (∼0.820 V). The anodic peak shift rate and ΔEp–p/2 parameters were the smallest across the studied DES (Table 2, entry 5). RAC was only observed at scan rates below 20 mV s−1. The cathodic activity was characterized by two peaks C(I) and C(II) centred at ΔEp,c(I) = 0.05 V and ΔEp,c(II) = −0.4 V. C(I) exhibited the largest shift rate across the studied DES, which caused a merge of the two peaks into a single broad peak at faster scan rates, thus exhibiting the largest ΔEp–p/2 across the heated samples as well. The significant cathodic peak shift also promoted the largest ΔEp(I) values across the studied samples. As discussed in the case of ChCl/EG (1
:
2), since the broad cathodic ΔEp–p/2 value is a consequence of the convolution of two peaks, the derivation of the cathodic transfer coefficient implies an underestimation. As such, the asymmetry of the electrochemical process evidenced by the narrow shape of the anodic peak leads to a fortuitous complementarity of the transfer coefficients (αa + αc ≈ 0.99). As opposed to ChCl/MA (1
:
1), for AcChCl/AA (1
:
2) the rather asymmetric forward transfer coefficient (αa ≈ 0.71) and the large ΔEp(I) values were the main contributors to two orders of magnitude decrease on the estimated rate constant.
Overall, replacing ethylene glycol with acetic acid as HBD improved the peak currents in both redox processes, the diffusion coefficients of V(IV/V) and, to a lesser extent, the kinetics of the anodic process. Unexpectedly, the acidic DES did not show improvements for the V(V) reduction process compared to ChCl/EG (1:
2), as initially hypothesized. These observations suggest that organic acids had a worse impact on the V(V) reduction process in DES compared to ethylene glycol.
Notably, the worst performing sample was AchChCl/AA (1:
2), where the alcohol group in the cholinium cation was completely esterified, meaning no alcohol functional groups were involved in the formulation. Therefore, the presence of alcohols resulted more beneficial for the reduction electrochemical kinetics of vanadium than organic acids, although all the redox processes were found to be irreversible. Additionally, the RAC was also more pronounced in ChCl/EG (1
:
2) than in the acidic DES.
The addition of water led to notable improvements in electrochemical performance, primarily by reducing viscosity, increasing current densities, and lowering overpotentials. However, the extent of these benefits varied depending on the composition of the DES and the water content. The best performing samples from each set of ternary DES mixtures are displayed in Fig. 3.
Moderate water contents (xH2O < 2.0) improved the cathodic process by decreasing peak overpotentials and peak widths, while also enhancing current densities. However, higher water contents (xH2O = 4.0) often resulted in an overall destabilization of the redox process, leading to larger peak separations and increased cathodic shift rates. This suggests that while reducing viscosity facilitates charge transfer, excessive dilution may disrupt stabilizing interactions with vanadium, such chloride coordination or specific hydrogen bonding interactions, which would promote better solvation. Interestingly, in the case of AcChCl/AA (1:
2), which lacks alcohol functional groups, water addition significantly improved cathodic stability, likely due to the hydrolysis of acetylcholine chloride, leading to acetate anions influencing the redox environment. Despite these improvements, the V(IV/V) redox process remained fully irreversible across all studied systems. As an example, the lowest ΔEp(I) value obtained was 410 mV for the ChCl/EG/H2O (1
:
2
:
0.5) mixture, with the cost of lower available currents than its more diluted counterparts. The full analysis is provided in the SI and displayed in Fig. S42.
The voltammetric experiments performed on ChCl/EG/AA (1:
x
:
y) mixtures showed mixed performance trends depending on the base DES used. CVs obtained from ChCl/EG/AA (1
:
2
:
2) ternary mixtures based on ChCl/EG (1
:
2) exhibited different features compared to those arising from ChCl/AA (1
:
2). We attributed these observations to differences in the water content and the degree of esterification of the base DESs. For clarity, the electrochemical performance metrics and the CVs corresponding to the ChCl/EG (1
:
2)-based and ChCl/AA (1
:
2)-based mixtures are displayed separately in Fig. S59.
Overall, in agreement with the previous binary mixture's characterization, better anodic performance was correlated with higher acetic acid content, whereas higher ethylene glycol fractions resulted better for stabilizing the cathodic process. Lower fractions of choline chloride also resulted in performance increases, thus underscoring the benefits of diluting the DES. The best performing sample of the ChCl/EG/AA (1:
x
:
y) group of mixtures resulted ChCl/EG/AA (1
:
2
:
2), as it was the sample exhibiting the smallest ΔEp(I) (0.576 V), the second largest peak currents and shorter anodic and cathodic ΔEp–p/2 widths than the corresponding binary supporting electrolytes. However, as found for the ternary mixtures, vanadium follows completely irreversible electrochemical kinetics. The full analysis is provided in the SI.
The ChCl/MA/EG (1:
x
:
y) set resulted the best performing of the studied ternary mixtures in terms of the ΔEp(I) parameter, which resulted similar to those observed in aqueous acidic solutions.49 A summary of the CV metrics and voltammograms is displayed in Fig. 4. The anodic region of these CVs was characterised only by one peak A(I) at potentials between 0.85 V and 0.94 V. As observed for the ChCl/MA (1
:
1) binary mixtures, no RAC was detected even when using high ethylene glycol content. The cathodic region of the CVs was characterised by only one reduction peak C(I) at potentials between 0.25 V and 0.53 V. Unlike ChCl/EG (1
:
2), the ternary mixtures did not show any peaks at potentials were C(II) was observed, regardless of the amount of ethylene glycol employed (Fig. 4a).
Some correlations were identified between the mass fractions of the diluting agents (wcomponent) and the CV performance metrics. However, these were challenging to disentangle since electrochemical performance depends on multiple factors, including viscosity, pH, ion coordination and vanadium interaction with specific functional groups, that are also interconnected (Fig. 4b). For example, malonic acid reduces the solution pH but increases its viscosity.
The ChCl/MA/EG (1:
x
:
y) electrolytes promoted the smallest ΔEp(I) values of this work. The improvements compared to the parent DES were explained by an overpotential reduction of both anodic and cathodic processes, with ChCl/MA/EG (1
:
2
:
2) exhibiting ΔEp(I) = 327 mV. It is important to note that although these metrics reflect differences in redox kinetics amongst the different formulations, the analysis is not intended to predict full-cell performance, but rather to identify electrolyte composition trends that promote the most favourable environments for V(IV/V) redox reactions.
Higher wChCl and wEG values generally led to increasing anodic peak potentials. Conversely, intermediate to large wMA correlated with lower anodic overpotentials. As such, ChCl/EG (1:
2) (wChCl = 0.53, wEG = 0.47) exhibited the largest anodic overpotential, whereas ChCl/MA/EG (1
:
0.5
:
2) (wChCl = 0.44, wMA = 0.17, wEG = 0.39) and ChCl/MA/EG (1
:
2
:
2) (wChCl = 0.30, wMA = 0.44, wEG = 0.26) resulted in the lowest. On the other hand, smaller cathodic peak overpotentials loosely correlated with higher wMA and wEG and consequently lower wChCl. Therefore, ChCl/MA/EG (1
:
2
:
2) exhibited the lowest cathodic overpotential.
The analysis of the binary mixture showed that the acid moderately contributed to the stabilisation of the anodic process when comparing polyol-based DES against organic acid-based DES, which is in line with the ternary mixture's findings. This suggests that the A(I) peak potential stabilization mostly depended on the pH. Naturally, the fact that higher overpotentials were correlated with higher ChCl contents indicates that the anodic process was negatively impacted by the viscosity. Conversely, the presence of alcohol functionalities as in ChCl/EG (1:
2) were observed to stabilize the cathodic process, whereas the organic acids had an opposite effect. In this case, an improvement arising from the combination of malonic acid and ethylene glycol was evident, compared to the parent DESs.
The anodic ΔEp–p/2 width, was correlated with higher wChCl and correspondingly, with lower wMA values. On the other hand, no trends between this parameter and wEG were observed. Therefore, A(I) peak width appeared most affected by the concentration of chloride, whereas viscosity and pH had a lower impact. This way, ChCl/MA (1:
1) and ChCl/MA/EG (1
:
1
:
0.5) promoted the shortest anodic peak widths. The shift for the A(I) peak potential at faster scan rates decreased with decreasing lower wMA and wChCl and increasing wEG. Therefore, the lowest observed anodic shift rates corresponded to ChCl/MA/EG (1
:
0.5
:
2) and ChCl/EG (1
:
2), which suggest that changes in viscosity/conductivity are mostly responsible for the variation in peak shift rate.
Shorter C(I) ΔEp–p/2 widths and lower peak potential shift rates were correlated with higher wEG, and lower wMA, whereas wChCl had relatively little influence in the variations of these parameters despite the increased viscosity associated with high ChCl contents. Even though there was a correlation between the cathodic peak potential and higher fractions of malonic acid, its presence was observed to increase C(I) shift rate and width, indicating an overall destabilisation of the cathodic process, as observed in the binary mixture analysis. Therefore, ChCl/EG (1:
2) exhibited the best performance according to these metrics.
As expected, larger V(IV) diffusion coefficients and in consequence, larger anodic currents, were obtained in correlation with lower wChCl and wMA and larger wEG. However, the largest values were observed for ChCl/MA/EG (1:
0.5
:
2) and (1
:
2
:
2) instead of ChCl/EG (1
:
2). This is attributed to the significant RAC in the parent binary DES. Since the current was measured from the onset of the main peak, the segment corresponding to the RAC was not considered. The C(I) peak current and the calculated diffusion coefficient were equally observed to correlate with lower wChCl and larger wEG and to a lesser extent with larger wMA. The contribution of wMA was attributed to the fact that malonic acid discouraged the process associated with C(II), which consequently increased the maximum cathodic currents in all the studied ternary mixtures.
The electrochemical properties of the V(IV/V) redox couple were evaluated in ternary mixtures formulated by diluting ChCl/EG (1:
2), ChCl/AA (1
:
2), AcChCl/AA (1
:
2) and ChCl/MA (1
:
1) with water, ethylene glycol, or acetic acid. Dilution with water improved the cathodic performance by reducing peak-to-peak potential differences in up to 35%, and cathodic peak widths at low water contents. However, at higher water contents e.g. xH2O = 4.0, an overall destabilization of the redox process was observed, as suggested by increased peak overpotentials, cathodic peak shift rates, and broader cathodic peaks. This indicates that, while a moderate amount of water enhances mass transport and lowers viscosity, excessive amounts of water negatively impact the redox stability, likely due to pH modulation or disruption of stabilizing interactions.
Across all compositions of ChCl/EG/AA and ChCl/AA/EG mixtures, the inclusion of acetic acid led to a progressive reduction in viscosity, which in turn facilitated mass transport and resulted in higher anodic peak currents and lower overpotentials. Higher contents of acetic acid showed only moderate improvements in the anodic peak reversibility. However, increasing content also led to a gradual destabilisation of the cathodic process, as evidenced by larger peak separations, higher cathodic peak shift rates, and, in some cases, the emergence of additional cathodic features. Conversely, mixtures with a higher fraction of ethylene glycol exhibited a more balanced electrochemical response, where the cathodic process was comparatively more stable, although still irreversible. This was reflected in lower peak shift rates at faster scan rates. The opposing effects of these two components highlight the competing influences of viscosity reduction (favouring mass transport) and solvation interactions (governing redox stability) in DES-based electrolytes. An increase in malonic acid content led to a progressive stabilisation of the anodic process, reducing the RAC and minimizing anodic peak broadening. This effect suggests that malonic acid plays a role in stabilizing the oxidized vanadium species, potentially through specific solvation or coordination interactions. However, increasing malonic acid concentration also led to a slight increase in cathodic overpotentials, indicating that while the anodic step benefited from the presence of carboxyl groups, the cathodic reduction of V(V) to V(IV) remained kinetically hindered. A higher ethylene glycol content, in contrast, contributed to a more balanced electron transfer process, improving cathodic stability while still preserving moderate anodic stabilization. This was reflected in lower peak shift rates, suggesting that glycol-rich compositions provided a more favourable solvation environment for vanadium species in both oxidation and reduction. The most optimized behaviour was observed in ChCl/MA/EG (1:
2
:
2), which exhibited peak-to-peak separations comparable to those observed in aqueous acidic electrolytes, moderate cathodic overpotentials, and a well-defined anodic/cathodic response.
These results highlight the complex interplay between viscosity, solvation structure, and electrochemical kinetics, emphasizing that reducing viscosity alone is insufficient to achieve full redox reversibility in DES-based electrolytes. This work also emphasizes the importance of the DES composition to design systems with optimized mass transport, solvation effects, and kinetic barriers in the V(IV/V) redox process. Despite improvements in specific electrochemical parameters, the V(IV/V) process remained fully irreversible across all studied systems, reinforcing the need for further molecular engineering of DES electrolytes to reduce viscosity and enhance charge transfer kinetics and redox stability for vanadium redox flow battery applications. As such, future work could explore alternative HBA anions, complexing agents, or additional additives to further improve charge transfer rates and reversibility in DES-based electrolytes.
Supplementary information is available. See DOI: https://doi.org/10.1039/d5eb00138b.
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