John F. Koonsa,
Samantha C. Cullom
a and
Jeffrey E. Dick
*ab
aJames Tarpo Jr. and Margeret Tarpo Department of Chemistry, Purdue University, West Lafayette, IN 47907, USA. E-mail: jdick@purdue.edu
bElmore Family School of Electrical and Computer Engineering, Purdue University, West Lafayette, IN 47907, USA
First published on 13th August 2025
The oxygen evolution reaction plays a key role in many modern energy conversion and storage devices, making the development of catalysts for the reaction of utmost importance. Transition metal hydroxides represent a promising category of oxygen evolution catalysts in alkaline environments, due to the affordability and abundance of material, high activity and good stability. However, precipitation of these catalysts directly on electrode surfaces can be energy intensive, requiring high overpotentials. In this work, we present a new method of electrodeposition using the confined environment of aqueous microdroplets adsorbed on an electrode to produce a high pH through heterogeneous reduction of solvated oxygen, O2. Using O2 reduction in this manner requires less cathodic applied potentials compared to other electrodeposition techniques and avoids direct metal reduction. Additionally, this methodology allows for the precipitation of a wide variety of stoichiometrically controlled transition metal hydroxides by only changing the starting metal precursor salts. Through this method, we precipitate a variety of transition metal hydroxides ranging from monometallic to penta-metallic alloys and analyze their morphology, composition and catalytic performance toward oxygen evolution. Overall, this work presents a new, facile method to be used toward electrodepositing a range of highly desirable transition metal hydroxide catalysts.
Transition metal-based catalysts offer a promising alternative to precious metal catalysts for OER. Recent years have seen the development of transition metal oxides, hydroxides, phosphides, and other similar materials with exceptional catalytic performance.14–16 Currently, their usefulness in acidic water electrolysis devices like proton-exchange-membrane (PEM) electrolyzers is limited due to their instability at low pH.17–19 However, transition metal oxides and hydroxides have exceptional stability in alkaline environments, making them promising candidates for catalysts in advanced alkaline water electrolyzers (AWEs), which account for most of the industrial level electrolyzers used today.4,15,20,21 In recent years, researchers have made significant strides in finding a range of high-performance transition metal hydroxide compositions for OER catalysis and elucidating the catalytic mechanisms at work.22–25 For example, Ni/Co-based hydroxides with small amounts of Fe either from coprecipitation or Fe impurities in water have been shown to have exceptionally low overpotentials, η, under alkaline conditions.26–28
Despite this progress in catalyst design and mechanistic understanding, the methods of synthesis remain relatively underdeveloped. Many synthetic pathways utilize additives such as potassium hydroxide, hydrogen peroxide or bromine, often coupled with solvothermal methods to precipitate sheets of hydroxides on top of an electrode.29–31 Still more methods utilize added base or nitrate/chloride anions to produce hydroxide at the electrode interface via water reduction, nitrate reduction, chloride oxidation, or some other mechanism to electro-precipitate catalysts directly on an electrode.32–35 While these methods are relatively simple, there are some significant drawbacks. First, few universal methods exist across different transition metals or even different precursor salts (MCl2, M(NO3)2, M(SO4), M(ClO4)2, etc.), which makes the development and optimization of methods for new stoichiometries and combinations labor intensive. Additionally, the reduction of water or nitrate anions require varying degrees of negative applied potentials at the working electrode for different metal combinations and concentrations. These potentials usually provide more than enough cathodic energy to electroreduce the metal itself to the zero-valent state rather than precipitating it as a hydroxide. Finally, while transition metal hydroxides are often synthesized as sheets, this geometry does not maximize electrocatalytic surface area (ECSA) per gram of material, and therefore, it may be useful for OER catalyst research to explore methods that allow for the precipitation of discrete nano- or micro-structures.
One seemingly unexplored methodology that could provide an answer to these considerations is that of electrodeposition via aqueous microdroplets suspended in a water-in-oil emulsion.36,37 In this system, a small volume of aqueous solution (25 μL) containing relatively low concentrations of metal precursor salts is added to a larger volume of organic solvent (∼5 mL) and sonicated to form an emulsion of aqueous microdroplets. Metal precursor salts are confined in these droplets due to insolubility in the organic phase, creating an electrochemical microreactor when the droplet collides with the electrode, irreversibly adsorbing to the surface. Electroneutrality is maintained in the droplet by partitioning of organic supporting electrolytes such as tetrabutylammonium perchlorate ([TBA]+[ClO4]−) across the organic|aqueous phase boundary. This system has been used in the past to synthesize high entropy alloy nanoparticles and other materials by applying a cathodic potential in excess of −1.5 V versus 1 M Ag/AgCl to rapidly electrochemically reduce all metals in the droplet, along with water and any other species present.38–40 However, a more subtle mechanism may be utilized at less cathodic applied potentials to quickly create a basic pH inside the droplet without reducing any metal. In addition to supporting electrolyte, the organic solvent will also dissolve significant amounts of gaseous oxygen, O2, over time if exposed to ambient conditions. Therefore, if a cathodic potential is applied that is sufficiently negative to reduce O2, a strongly basic pH gradient may be created inside the aqueous droplet. This will be aided by the subsequent partitioning of dissolved O2 into the aqueous droplet from the O2 rich organic phase in order to maintain concentration equilibrium across the two phases. Our group has recently shown that driving O2 reduction during metal electrodeposition indeed creates such a basic environment in the droplet that it acts as a switch between depositing zero-valent Cu nanoparticles and Cu(OH)2 nanoparticles.41 Applying this now to a system where the aqueous microdroplets contain transition metals that reduce exclusively at more negative potentials than O2 reduction (unlike Cu), it should be possible to achieve the selective precipitation of transition metal hydroxide catalysts by simply reducing dissolved O2 in the aqueous phase.
Herein, we utilize this method of reducing O2 in confined aqueous microdroplets to precipitate transition metal hydroxides. This method allows for the synthesis of a wide variety of compositions ranging from mono- to penta-metallic hydroxides with simple stoichiometric control by varying precursor salt concentrations. Importantly, this method avoids additives and only requires a small concentration and volume of metal precursor salt. It does not rely on electrochemical interactions with specific metal anions at the electrode interface and avoids the application of negative potential sufficient to electroreduce transition metals of interest, such as Ni, Co, Fe, Zn, and Mn. We investigate the structure, composition and catalytic performance of these materials, and gain mechanistic insights into the roles of O2 reduction rate and droplet volume. This work introduces a facile new method to be used for the synthesis of a wide range of transition metal hydroxide nano- and microstructures without significant modification to the process while simultaneously avoiding unwanted electroreduction of metals during the process.
When preparing samples for TEM characterization, the working electrode was a TEM grid electrically connected by tweezers to the potentiostat. The same washing procedure was used for TEM grids; however, they were stored in vacuum for 1 hour to remove excess solvent before characterization.
The method for electrodepositing transition metal hydroxides by selectively reducing O2 in aqueous microdroplets is illustrated in Fig. 1c. Metal chloride salts are confined inside of aqueous microdroplets that are suspended in a continuous phase of 1,2-dichloroethane which contains [TBA]+[ClO4]− as an electrolyte. These aqueous droplets will collide randomly with the working electrode as they diffuse throughout the emulsion. After this, they become electrically connected to the working electrode and serve as nano- or picoliter volume reactors. When the working electrode is held at a sufficiently cathodic potential to drive O2 reduction in the droplets and not reduce any of the metal cations directly – between 0.4 V and −0.25 V vs. RHE for a glassy carbon working electrode – a basic pH gradient will be created in the droplet by O2 reduction either consuming protons in acidic conditions or producing hydroxide in basic conditions as seen in eqn (1)–(4),42 Once dissolved O2 in the aqueous droplet is reduced more O2 should continually partition into the aqueous droplet from the higher concentration dissolved in the surrounding organic phase to maintain an equilibrium concentration gradient. Hence there will be a constantly replenishing source of O2 to be reduced in the aqueous droplets, causing a sharp increase in pH.
Acidic conditions:
O2 + 4H+ + 4e− ⇌ 2H2O | (1) |
O2 + 2H+ + 2e− ⇌ H2O2 | (2) |
Basic conditions:
O2 + 2H2O + 4e− ⇌ 4OH− | (3) |
O2 + H2O + 2e− ⇌ HO2− + OH− | (4) |
Applying the results of the cyclic voltammograms in Fig. 1, we used an applied cathodic potential, Eappl, of −0.2 V vs. RHE for 400 s to a glassy carbon working electrode that was submerged in a water-in-oil emulsion as seen in Fig. 1c, readily reducing aqueous dissolved O2, while not reducing any of the metal salts. In this first case, the aqueous droplets contained CoCl2, NiCl2, ZnCl2, FeCl3, and MnCl2. The resulting current–time (i–t) curve is seen in Fig. S1, showing a large current for its entirety as would be expected from O2 reduction at that Eappl. The SEM image in Fig. 2a shows some of the common resulting morphologies of the precipitated material on the electrode surface. They range from sheets in the μm range to single particles in the nm range and appear to be randomly distributed across the surface (Fig. S2). In many cases, the precipitated material resides primarily in a ring-like structure likely along the edge of the collided droplet where the water|oil|electrode interface was located (Fig. S3). The abundance of cases with most material focused on the edge of the droplet collision suggests that the interface is the source of the high pH gradient due to O2 partitioning in and being subsequently reduced. However, the rings do not appear in every case, highlighting the stochastic and heterogeneous nature of these droplet collisions.
Fig. 2b(i) shows a STEM-HAADF image of the MnFeCoNiZn(OH)x sheet precipitated on a carbon TEM grid. The image displays a heterogeneous distribution of the transition metals across the sheet, seen as the high scattering bright areas. This heterogeneity was consistent for nearly all cases (Fig. S4). A higher magnification HAADF image in Fig. 2b(ii) reveals rows of atoms with a d-spacing of 0.250 nm. While, this value alone cannot be directly correlated with any specific transition metal layered double hydroxide (LDH), it does highlight the crystalline nature of the transition metal rich regions. Other areas of the transition metal-rich regions of the precipitate revealed similar crystalline nature (Fig. S5). In contrast, regions of the precipitate with a less abundant metal signal revealed no obvious signs of crystalline fringes in HAADF (Fig. S6). Overall, this reveals a mix of crystalline and amorphous regions in the transition metal precipitates. X-ray diffraction (XRD) could provide further insight into the crystal planes present in these precipitates, but this characterization method has proven to be very limited at characterizing metals deposited from nano- or microdroplets, likely due to relatively low surface coverage and the randomness of precipitate orientation.
Fig. 2c shows EDX mapping of an SEM image for Mn, Fe, Co, Ni, and Zn – all of which were originally contained in the aqueous droplets. All 5 metals were present in the precipitates and consistently appeared to have a homogeneous distribution. Significantly, chlorine and nitrogen signals were largely absent from these materials, which would be present if the precipitates were either metal chloride salts or some complex with the organic [TBA]+ salt, respectively (Fig. S7). Instead, the lack of signal suggests precipitation of transition metal hydroxides rather than salt complexes. Fig. 2d shows the EDX ratios of each metal and their standard deviations. These results indicate that the transition metal precipitates are at the high end of mid-entropy with a ΔSconf = 1.56R ± 0.028 (Fig. S8). STEM/EDX also revealed a homogeneous and random distribution of metals across the precipitates (Fig. S9). The homogenous distribution of all five transition metals suggests that the microdroplet confined O2 reduction method is generalizable for multiple transition metals as expected.
While the Eappl value and EDX data indicate that the metals are likely precipitated as transition metal hydroxides, XPS provides clearer insight into the specific transition metal and oxygen species present. For XPS characterization, we coprecipitated Mn, Fe, Co, Ni, and Zn for 1200 s (versus the original 400 s) at the same Eappl on a glassy carbon working electrode. This increase in reaction time allows for more randomly diffusing droplets in the emulsion to collide with the cathodically biased working electrode and increases the surface coverage of catalyst. The full XPS survey spectrum obtained for the sample can be seen in Fig. S10. In Fig. 2e the O1s signal indicates a majority peak that corresponds well with typical transition metal hydroxide (M–OH) binding energies, with a smaller peak consistent with transition metal oxide (M–O) binding energies. The water peak (M–OH2) aligns well with values assigned to surface oxidation layers formed on certain transition metal hydroxides resulting from moisture in the air.31,43,44 Fig. 2f shows the different 2p regions for Mn, Fe, Co, Ni, and Zn. The regions showed no indication of zerovalent or monovalent signals. Rather, all peaks fit exclusively for either hydroxide or (oxy)hydroxide species of each metal.43 In all cases, the metals are still present in the original valency of the metal chloride salt, indicating a lack of metal electroreduction at the electrode surface. Together these XPS data demonstrate that the MnFeCoNiZn hydroxides are being precipitated via hydroxide or oxide formation with no competing electroreduction of the metals themselves, thereby maximizing the amount of metal precursor salt that forms the desired catalytic product rather than zerovalent metal structures.
In addition to precipitating all five metals together, we also precipitated them separately by adding 25 mM of each metal salt into the aqueous phase. We observed similar morphologies for the individual cases compared with the penta-metallic hydroxide (Fig. S11). This again highlights the generalizability of this technique in its ability to precipitate transition metals both individually and as alloys.
Having precipitated five transition metals together in a homogeneous and nearly equimolar ratio, we sought to explore the level of control over the relative amounts of each metal in a case with just two starting components. We tested Ni and Fe together since hydroxide alloys of these materials have been shown to have superior catalytic performance toward OER.25,28,45 Specifically, alloys with a ratio of Ni0.75Fe0.25 perform exceptionally well in basic environments. We added 75 mM NiCl2 and 25 mM FeCl3 to the aqueous phase in the water-in-oil emulsion and used the same Eappl, −0.2 V vs. RHE, on a glassy carbon working electrode for 400 s. The resulting precipitates, seen in Fig. 3a, had similar morphologies to the previous cases. EDX mapping of the NiFe(OH)x precipitates shows a mostly homogeneous distribution of both metals (Fig. 3b and c). EDX point scans of the bimetallic precipitates revealed a range of atomic ratios centered around the target value of a 75:
25 Ni
:
Fe atomic ratio (Fig. 3d(i)). While the mean and median values are approximately equal to the ratios of each metal added to the aqueous phase, there is a significant amount of deviation around those values. We also demonstrated this with a 50
:
50 Ni
:
Fe ratio added to the aqueous phase, which yielded the atomic ratios seen in Fig. 3d(ii). Once again, the mean and median are centered near the target value with some deviation. While some heterogeneity occurs in the precipitation of NiFe(OH)x, O2 reduction in aqueous microdroplets shows significant promise in its ability to selectively precipitate specific ratios of these starting metals by simply adding the desired ratio of the metal precursor salts without having to change anything else about the procedure.
We next sought to gain more insight into the mechanism of microdroplet mediated precipitation via O2 reduction by comparing our results to those attained by applying the same potential to an electrode either suspended in a bulk aqueous phase with no adsorbed droplets or suspended in an organic phase with a large adsorbed aqueous droplet (approximately 1 mm radius and 1 μL volume). Given that pH is a function of H+ concentration, its value will not only depend on the physical number of H+ molecules in a droplet, but also the volume of the droplet. Imagining shrinking the radius of a droplet from the scale of 1 mm down to 1 μm, both the size of the water|oil|electrode interface and the volume of the droplet will change significantly. Decreasing the radius will decrease the droplet contact interface with the electrode in proportion to the radius since the circumference is equal to 2πr. Hence the amount of O2 reduced may also experience a decrease that is roughly proportional to the droplet radius. However, volume is equal to meaning that volume will have a much sharper decrease compared to the size of the water|oil|electrode interface as the droplet radius shrinks. Applying this to the formula for concentration,
, where n is moles and V is volume, we can see that shrinking a droplet will result in larger changes in concentration of species such as H+ and OH−. Consequently, aqueous microdroplets likely provide a much more suitable environment for precipitating transition metal hydroxides compared to larger droplets, which might not sufficiently concentrate the produced OH−. Additionally, not only will a bulk aqueous environment fail to confine any OH−, but it also likely contains too low of a concentration of dissolved O2 to precipitate the catalysts.
To investigate this theory, we applied 0.47 V, 0.22 V and −0.03 V vs. RHE to these three different environments – a bulk aqueous phase, a 1 μL aqueous droplet and an emulsion of aqueous microdroplets. Fig. 5a shows where each of these potentials fall on the reduction curve of O2 reduction in 0.1 M KCl, and are marked by Eappl 1, 2, and 3, respectively. In the case of a bulk aqueous phase containing 20 mM each of MnCl2, FeCl3, CoCl2, NiCl2, and ZnCl2, we saw no precipitation or electrodeposition of the metals at any of these potentials (Fig. S12) – likely due to the insufficient O2 concentration and diffusion of any basic pH gradient formed away from the electrode surface that it was formed at. In the case of a 1 μL droplet adsorbed on the electrode, there was a small amount of precipitation around the interface only at −0.03 V (Fig. S13), which is consistent with previous observations and may be due to a localized pH gradient at the interface.46 The preferential formation of precipitate around the interface likely indicates once again that the O2 reduces primarily around the interface as soon as it partitions into the aqueous droplet. This effect is more pronounced in large droplets since OH− will only be concentrated at this point before diffusing away into the larger aqueous volume of the droplet. Our group is currently investigating ways to visualize this interfacial pH effect and its potential ability to form precipitate rings further.
We next applied all three of these potentials to a glassy carbon working electrode submerged in an emulsion of aqueous microdroplets for 120 s. The resulting current densities, j, on the j–t curves for Eappl 1, 2 and 3 were about 0.01 mA cm−2, 0.04 mA cm−2 and 0.2 mA cm−2, respectively (Fig. 4b), which reflect the j of O2 reduction driven at each Eappl. Additionally, we held a fourth electrode at the open circuit potential (OCP) for 120 s, during which no bias or current is applied as the potential is held at the OCP, which was about 1.1 V vs. RHE (Fig. S14). In all four of these cases, transition metal precipitates were formed with a range of compositions.
Fig. 4c–f show SEM images of the precipitated materials in each case and the EDX ratios of these precipitates. Fig. 4c shows the precipitates formed when holding the electrode at the OCP and passing negligible current. We found it surprising that precipitation happened in this case, and that the materials showed no chloride peak in EDX (Fig. S15). These materials were hydroxide alloys of Ni and Fe in a ratio of approximately Fe0.85Ni0.15. This precipitation likely occurs through some spontaneous galvanic interaction with another species in the aqueous droplets but the exact cause remains unclear. Fig. 4d shows precipitates synthesized at Eappl 1, which have more similar morphologies to those precipitated at −0.2 V vs. RHE compared to the films formed at OCP, but EDX analysis of these revealed that the materials only contained Fe. The precipitates formed at Eappl 2 in Fig. 4e and at Eappl 3 in Fig. 4f displayed the most similar morphologies and atomic ratios of all 5 metals compared to those deposited at −0.2 V. These observations show that increased levels of O2 reduction lead to better stoichiometric control over the resulting transition metal hydroxides.
The variety of precipitate morphologies and compositions might be explained by Pourbaix diagrams and the relative pH sensitivity of each metal. All of the metals used in these cases – Mn, Fe, Co, Ni, Zn – are likely to form hydroxides, oxides or oxyhydroxides rather than be reduced by the electrode at all three values of Eappl, given that a sufficiently basic pH is present in the droplet.47,48 Mn requires the most basic pH to form precipitates, suggesting that a pH value of 10 or higher is present when Mn is precipitated. However, the pH in the microdroplets likely does not reach this value when the electrode is held at Eappl 1 or OCP. Despite this, Fe will precipitate as an (oxy)hydroxide even at low pH values, possibly explaining why it is still present in all four cases. Still, the mechanism of precipitation at OCP and the reason for Ni coprecipitating with Fe are not yet fully clear – especially given that these materials are produced without passing any current. Given that many intriguing spontaneous redox phenomena have been observed at the water|air and water|oil interfaces in aqueous microdroplets, it will be an interesting avenue of inquiry to probe this mechanism further.49–54 This drastic change in pH based on slight changes in Eappl is enabled both by the confinement of the aqueous microdroplets and the continuous O2 supply from the surrounding organic phase. Consequently, this method is likely compatible with any organic solvent that has a higher O2 solubility than water and will create a stable emulsion with water. Solvents such as chloroform and dichloromethane have been shown to work similarly to 1,2-dichloroethane in multiphase electrochemistry applications, and we expect that they will also work well for this method.
Finally, we tested the utility of MnFeCoNiZn(OH)x, Ni(OH)2, and Ni0.75Fe0.25(OH)x as OER catalysts in 0.1 M KOH (Fig. 5a). These materials were precipitated onto glassy carbon electrodes using the same method as above. Ni(OH)2 was synthesized by adding 100 mM NiCl2 to the aqueous phase. The electrocatalytic surface area (ECSA) of each of these materials was estimated by determining the double layer capacitance, Cdl, and dividing by the specific capacitance of the materials.34 Cdl was estimated by plotting the capacitive current versus potential scan rate while doing linear sweep voltammetry in a purely capacitive potential window (Fig. S16–S19). Details for these calculations can be seen in the Experimental Section and SI. We found that the MnFeCoNiZn(OH)x had an onset potential – set as the potential at which j = 10 mA cm−2 – of approximately 1.8 V vs. RHE. Ni(OH)2 yielded a nearly identical onset potential. Ni0.75Fe0.25(OH)x had an onset potential of approximately 1.75 V vs. RHE. All three had a far lower onset potential than the undecorated glassy carbon macro electrode, which was about 2.6 V vs. RHE. These onset potential values represent OER overpotentials, η, of 0.57 V for MnFeCoNiZn(OH)x and Ni(OH)2, and 0.52 V for Ni0.75Fe0.25(OH)x. While these η values are over 100 mV larger than the lowest reported catalysts, they nevertheless show that this technique can be used to electrodeposit active catalytic materials toward OER. We also tested the precipitates formed in Fig. 4, all of which exhibited similar η values (Fig. S20–S24).
In addition to determining the η of these catalysts, we also tested their stability when doing OER in 0.1 M KOH. Fig. 5b shows chronopotentiograms where the catalysts were held at j = 10 mA cm−2. All three showed relatively stable behavior with slight increases in η over the course of 2 hours. The slight discrepancies in η values between the original linear sweep voltammograms likely results from different coverages of precipitate between different electroprecipitation trials. The droplets' rate of collision with the electrode will differ in subsequent trials due to the stochastic nature, which will cause slight variations in catalyst ECSA. Linear sweep voltammograms from before and after the 2 hour testing time also show a slight decrease in catalytic performance over time, as seen by the decreased i following stability testing (Fig. 5c(i)–(iii)). To determine the cause of this catalytic loss, we ran the MnFeCoNiZn(OH)x catalyst until it changed to the η expected for glassy carbon (Fig. S26). After imaging this electrode, it was determined that the catalyst had fallen off of the surface and only ClO− salt remained – possibly due to oxidation of Cl− impurities in solution (Fig. S27). Finally, a linear sweep voltammogram confirmed that the electrode only showed the electrochemical characteristics of a glassy carbon electrode. Overall, the catalyst precipitates themselves appear to be relatively stable, but the glassy carbon substrate is not ideal for long term catalysis. Despite this issue on glassy carbon, it remains an interesting avenue of inquiry to test this technique on other materials commonly used for OER catalyst substrates such as a Ni foam or C mesh. Since this method relies on reducing dissolved aqueous O2, it should be viable on other electrode materials as long as they reduce O2 at less cathodic potentials than the added aqueous metal salts, which we demonstrated on a Pt working electrode (Fig. S28).
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