A PROCESS FOR ENHANCING THE CATALYTIC EFFICIENCY OF OER

Abstract

The present invention relates to a process for enhancing the catalytic efficiency of a catalyst for the oxygen evolution reaction (OER), comprising exposing the catalyst to an external magnetic field of between 65×10−6 mT and ≤200 mT during the oxygen evolution reaction, wherein the catalyst is a material which exhibits an increased Berry phase induced by the exposure of the catalyst to the external magnetic field.

Claims

1. A process for enhancing the catalytic efficiency of a catalyst within an oxygen evolution reaction (OER) cell, said process comprising exposing the catalyst to an external magnetic field of between 65×10.sup.−6 mT and ≤200 mT during an oxygen evolution reaction, wherein the catalyst is a material which exhibits an increased Berry phase induced by the exposure of the catalyst to the external magnetic field.

2. The process of claim 1, wherein the catalyst exhibits a non-zero Berry phase at the OER cell operating temperature.

3. The process of claim 1, wherein the catalyst exhibits a non-zero Berry phase at 25° C.

4. The process of claim 1, wherein the catalyst is a metal, metal oxide, metal sulfide, metal carbide, or Heusler alloy.

5. The process of claim 4, wherein the metal is selected from the group consisting of Cr, Mn, Fe, Co and Ni.

6. The process of claim 4, wherein the metal oxide is selected from the group consisting of compounds comprising oxygen and one or more metallic elements.

7. The process of claim 4, wherein the metal sulfide is selected from the group consisting of compounds comprising sulfur and one or more metallic elements.

8. The process of claim 4, wherein the metal carbide is selected from the group consisting of compounds comprising carbon and one or more metallic elements.

9. The process of claim 4, wherein the Heusler alloy has a composition of TT′Z (half-Heusler) or T.sub.2T′R (full-Heusler), wherein T and T′ are selected from the group consisting of transition metals, and R is an element from IUPAC group 13, 14 or 15.

10. The process of claim 1, wherein the catalyst has a plate-like form comprising a planar surface.

11. The process of claim 10, wherein the magnetic field which is applied to the plate-like catalyst has field lines, and the magnetic field is arranged such that the field lines run at least not parallel to and through the planar surface of the plate-like catalyst.

12. An electrochemical cell comprising a cathode, an anodic working electrode with oxygen evolution reaction (OER) catalyst(s), and a constant external magnetic field of ≤200 mT that increases the efficiency of an oxygen evolution reaction.

13. The electrochemical cell of claim 12, wherein the catalyst is a material which exhibits an increased Berry phase in an OER under the influence of an external magnetic field of ≤200 mT.

14. The process of claim 5, wherein the metal is Fe, Co or Ni.

15. The process of claim 6, wherein the metal oxide is a binary metal oxide having the formula T.sub.xO.sub.y, wherein T is selected from the group consisting of transition metals, and/or ternary metal oxide having the formula T.sub.xT′.sub.1-xO.sub.y, wherein T and T′ are independently selected from the group consisting of transition metals; and wherein x and y independently from one another represent an integer from 1 to 8.

16. The process of claim 6, wherein the metal oxide is selected from one or more of Fe.sub.3O.sub.4, Fe.sub.2O.sub.3, NiO, Co.sub.3O.sub.4, MnFe.sub.2O.sub.4, CoFe.sub.2O.sub.4 and NiFe.sub.2O.sub.4.

17. The process of claim 7, wherein the metal sulfide is a binary metal sulfide having the formula T.sub.xS.sub.y, wherein T is selected from the group consisting of transition metals; and/or ternary metal sulfide have the formula T.sub.xT′.sub.1-xS.sub.y, wherein T and T′ are selected from the group consisting of transition metals; wherein x and y independently from one another represent an integer from 1 to 8.

18. The process of claim 7, wherein the metal sulfide is selected from one or more of Fe.sub.3S.sub.4, Fe.sub.7S.sub.8, Ni.sub.3S.sub.4, Co.sub.3S.sub.4, NiFe.sub.2S.sub.4, ZnFe.sub.2S.sub.4 and NiFeZnS.sub.4.

19. The process of claim 8, wherein the metal carbide is a binary metal carbide having the formula of T.sub.xC.sub.y, wherein T is selected from the group consisting of transition metals; and x and y independently from one another represent an integer from 1 to 5.

20. The process of claim 8, wherein the metal carbide is selected from one or more compounds selected from Fe.sub.2C, Fe.sub.5C.sub.2, Fe.sub.3C, Co.sub.3C, and NiC.

21. The process of claim 9, wherein the Heusler alloy is selected from one or more of Mn.sub.2NiSb, Ni.sub.2MnGa, Co.sub.2MnGa, Cu.sub.2MnSb, NiCrSi, NiCrGe and NiCrGa.

22. The process of one of claim 11, wherein the magnetic field is arranged such that the field lines run perpendicular to and through the planar surface of the plate-like catalyst.

23. The electrochemical cell of claim 12, wherein the catalyst has a plate-like form comprising a planar surface.

24. The electrochemical cell of claim 23, wherein the magnetic field which is applied to the plate-like catalyst has field lines, and the magnetic field is arranged such that the field lines run perpendicular to and through the planar surface of the plate-like catalyst.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0015] The accompanying drawings are included to provide a further understanding of the present invention. The drawings illustrate exemplary embodiments of the present invention and, together with the description, serve to explain the principles of the present invention.

[0016] FIG. 1 shows an exemplary experimental set-up of an electrochemical cell for OER in the presence of a constant external magnetic field.

[0017] FIG. 2 shows the distance depended magnetic field strength of the used magnet. The distance is measured between the indicated catalyst and the magnet.

[0018] FIG. 3 shows linear sweep voltammogram (LSV) OER curves of Ni foam with and without the application of an external magnetic field.

[0019] FIG. 4 shows the linear LSV curves of Ni foam with and without the application of the external magnetic field.

[0020] FIG. 5 shows the Galvanostatic (constant potential) measurement of electrochemical activity of Ni foam with and without an external magnetic field.

[0021] FIG. 6 shows the distance-dependent Galvanostatic (constant potential) electrochemical activity of Ni foam in the presence of external magnetic field.

[0022] FIG. 7 shows the long-time stability performance of Ni foam with an magnetic field.

[0023] FIG. 8 shows the magnetic field lines with reference to the surface of the catalyst plate; on the left side the field lines are oriented perpendicular to the plate face of the catalyst (=preferred embodiment) and on the right side the field lines are oriented parallel to the plate face of the catalyst.

DETAILED DESCRIPTION OF THE INVENTION

[0024] The present invention provides a simple method to increase the activity of OER catalyst through an increase of the Berry phase induced by the presence of a constant magnetic field that is larger than the average magnetic field of the earth (which is about 65×10.sup.−6 mT). It was found that the catalytic activity of electrocatalysts can be increased with only a small magnetic field of ≤200 mT. This enhancement of OER catalytic efficiency under a small constant magnetic field occurs in OER catalysts which exhibits an increased Berry phase induced by the exposure of the catalyst to the low external magnetic field that is larger than the average magnetic field of the earth (which is about 65×10.sup.−6 mT). It is possible to tailor the Berry phase and as a consequence to enhance the OER activity.

[0025] Berry phase is a quantity that describes the accumulation of a phase (or phase shift) when a vector is carried around a closed loop in a complex vector space. Recent studies confirmed that the existence of a Berry phase can influence the Hall effect in materials. The appearance of an anomalous Hall effect and a topological Hall effect is strongly dependent on the Berry phase of the given material.

[0026] In the presence of a magnetic field, one can tailor (tune) the value and/or the sign of the Berry phase. The macroscopic effect that goes along with the magnetic field exposure is a change of the anomalous Hall effect. This means that one can control the transport of electrons including their spin by altering the Berry phase.

[0027] Some materials exhibit a non-zero Berry phase outside (or without) a magnetic field; these are certain metals, metal oxides, metal sulphides, and alloys, specifically Heusler alloys. These materials are also potential catalysts for the oxygen evolution reaction because the OER process requires the transfer of electrons with their two basic properties: electric charge and spin; and electrons have vector characteristics, which can lead to a non-zero Berry phase.

[0028] The Berry phase of a material can be calculated based on the tight-binding model Hamiltonian:

[00001]${\sigma }_{xy}^z={\left(1/2\pi \right)}^{1/3}\int d\stackrel{.fwdarw.}{k}\underset{E\left(n,\stackrel{.fwdarw.}{k}\right)<E_F}{.Math.}f\left(n,\stackrel{.fwdarw.}{k}\right){\Omega }_{n,\mathrm{xy}}^z\left(\stackrel{.fwdarw.}{k}\right)$${\Omega }_{n,\mathrm{xy}}^z\left(\stackrel{.fwdarw.}{k}\right)=2\mathrm{Im}\underset{n^{\prime }\ne n}{.Math.}\frac{.Math.n,\stackrel{.fwdarw.}{k}\left|{\hat{v}}_x\right|n^{\prime },\stackrel{.fwdarw.}{k}\left|{\hat{v}}_y\right|n^{\prime },\stackrel{.fwdarw.}{k}.Math.}{{\left[E\left(n,\stackrel{.fwdarw.}{k}\right)-E\left(n^{\prime },\stackrel{.fwdarw.}{k}\right)\right]}^2}$

where σ is the Berry phase, Ω is the Berry curvature, f(n, {right arrow over (k)}) is the Fermi-Dirac distribution, E(n, {right arrow over (k)}) is the eigenvalue of the nth or n'th eigenstate of u(n, {right arrow over (k)}) at ({right arrow over (k)}) point, E.sub.F is the velocity operator, and Im is the imaginary (Im) part of the Berry phase. An external magnetic field can change the Hamiltonian of the system and consequently the Berry phase.

[0029] An experimental set-up of an OER electrolysis cell is shown in FIG. 1. The electrochemical cell comprises within a vessel a graphite cathode, a reference electrode, and a working electrode (anode) made of a catalytic material. In the proximity of the vessel a permanent magnet is located which creates a constant magnetic field of substantially homogeneous strength across the catalyst. In the set-up of FIG. 1 a disc magnet is shown, but a constant electromagnet can also be used. The magnetic strength which is exerted on the catalyst can be varied by changing the distance between the magnet and the catalyst.

[0030] The OER process is an oxidation reaction that occurs at the anode side of the electrochemical cell. It involves the formation of chemical bonds between the active sites of the electrocatalyst and the adsorbates. An electron transfer process concludes the oxidation reaction. The OER reaction kinetics strongly depends on the bond strength. A high bond strength results in strong adsorption of reaction intermediates, while a low bond strength leads to low coverage of the electrode surface with reactants. Both situations result in slow OER kinetics.

[0031] For transition metals, the octahedral splitting of the d orbitals results in the formation of a lower energy t.sub.2g triplet and a higher energy e.sub.g doublet. In the oxygen evolution process, the e.sub.g orbitals participate in σ-bonding with the oxygen-containing adsorbates at the surface of the catalyst. Thus, the filling of e.sub.g orbitals has a strong influence on the binding energy of the OER intermediates and, thus, on the OER catalytic activity.

[0032] The OER process on the catalyst surfaces involves the combination of two oxygen atoms at the active sites. Each of the oxygen atom carries an electron with specified spin orientation. According to the molecular orbital theory, two-unpaired electrons in the oxygen molecular orbital (MO) occupy the antibonding orbitals; these electrons are parallelly aligned. This is the reason why oxygen exhibits paramagnetic behavior at room temperature. In the presence of an external magnetic field, the electrons on the two 0 atoms are likely to be parallelly orientated. This favours the formation of oxygen molecules within the framework of molecular orbital theory.

[0033] An important reason for a low catalytic efficiency in OER is the formation of side products like H.sub.2O.sub.2. Generally, the OER process can be described as follows:

H.sub.2O+*.Math.HO*+H.sup.++e.sup.−  (1)

HO*.Math.O*+H.sup.++e.sup.−  (2)

where HO* is a reaction intermediate and O* is the adsorbed oxygen atom at the metal active site. In the next step, two O* atoms are combined and lead to the formation of molecular oxygen. However, two HO* radicals may also be combined before the formation of the oxygen radical, leading to H.sub.2O.sub.2 as a side product. A parallel electron alignment indicates a difficult combination and, thus, slower OER kinetics because of the spin-selection rule (ΔS=0 or ΔM.sup.S=0; M.sup.S=2S+1; S=Σs=n/2). While an anti-parallel alignment suggests an easier combination and faster OER process.

[0034] The formation of H.sub.2O.sub.2 is a result of the random spin on the HO* intermediate. Without the interference of an external magnetic field, the HO* radical carries arbitrary spins with 50% up and 50% down. Thus, there is a high probability for the formation of H.sub.2O.sub.2 in case of anti-parallel spin alignment on HO*. Accordingly, if one can align the spin orientation of HO* (in the same direction), the formation of H.sub.2O.sub.2 as a side product can be depressed and more oxygen radicals can be produced. Based on the above concept, the inventors predicted that the combination of a non-zero Berry phase and an external magnetic field may control the spin direction of the OER reaction intermediate, and thus increase the OER efficiency.

[0035] Also, it was found that the direction of the magnetic field which is applied to the catalyst is also of importance. For a plate-like catalyst with small thickness, the contact area with the magnetic field lines is much bigger for the plate-face than for the plate-side section (see FIG. 8). A magnetic field with field lines which run perpendicular to and through the surface (left side of FIG. 8) of the plate polarize the spins of the electrons in the catalyst and induce them to point to the electrolyte. This means that at least a substantial proportion (i.e. more than 50%) of the magnetic field lines which emerge from either the north or the south pole of the magnet are directed to the surface of the catalyst at an angle of 30-90°, preferably 60-90°, more preferred 80-90° and most preferred 90°. This results in a much higher transfer probability of electrons to the surface adsorbates (like HO* or O*) and as a consequence to higher catalytic efficiency. Thus, in a preferred embodiment of the invention the magnetic field is oriented such that the magnetic field lines run at least not parallel but preferably perpendicular to and through the plate surface of the catalyst (see FIG. 8, left side).

[0036] As mentioned above the present method of increasing the electrochemical activity of catalysts for the Oxygen Evolution Reactions (OER) is applicable to materials with the property to increase a non-zero Berry phase under the influence of a magnetic field. Preferably to materials which have a non-zero Berry phase at room temperature (25° C.). More preferably to metals, intermetallic compounds, metal oxides, metal sulfides, metal carbides and alloys, preferably Heusler alloys, in an electrochemical cell having a cathode, an anodic working electrode, and a low constant external magnetic field that surrounds the cell and the anodic working electrode.

[0037] In a preferred embodiment the metals are selected from the group consisting of Cr, Mn, Fe, Ni, and Co.

[0038] In a further preferred embodiment, the intermetallic compounds are selected from the group consisting of materials comprising two or more elemental metals of defined proportions (x and y) which exhibit a room temperature non-zero Berry phase. Preferred binary phase intermetallic compounds are those of the formula A.sub.xB.sub.y, wherein A=Fe, Co, or Ni, and B is selected from the group consisting of transition metals and x and y independently from one another represent an integer from 1 to 8. Typical binary phase intermetallic compounds which can be used in the present invention are Fe.sub.3Cr, Fe.sub.3Ga.sub.4, Fe.sub.3Pt, FeRh, CoGa, CoPt, Co.sub.3Ti, Ni.sub.3Fe, Ni.sub.3Mn, NiPt, etc.

[0039] In another preferred embodiment the metal oxides are selected from the group consisting of compounds comprising oxygen and one or more metallic elements. Binary metal oxides preferably have the formula T.sub.xO.sub.y, wherein T is selected from the group consisting of transition metals. Ternary metal oxides have the formula T.sub.xT′.sub.1-xO.sub.y, wherein T and T′ are independently selected from the group consisting of transition metals. x and y in both, the binary and the ternary oxides, independently from one another represent an integer from 1 to 8 in the above formulae. All of these metal oxides exhibit a non-zero Berry Phase at the working temperature of the OER-cell. Typical metal oxide compounds which can be used in the present invention are Fe.sub.3O.sub.4, Fe.sub.2O.sub.3, NiO, Co.sub.3O.sub.4, MnFe.sub.2O.sub.4, COFe.sub.2O.sub.4, NiFe.sub.2O.sub.4, etc.

[0040] In another preferred embodiment the metal sulfides are selected from the group consisting of compounds comprising sulfur and one or more metallic elements. Binary metal sulfides have the formula T.sub.xS.sub.y, wherein T is selected from the group consisting of transition metals; ternary metal sulfides have the formula T.sub.xT′.sub.1-xS.sub.y, wherein T and T′ are selected from the group consisting of transition metals. x and y, in both, the binary and the ternary sulfides, independently from one another represent an integer from 1 to 8 in the above formulae. All of these metal sulfides exhibit a non-zero Berry Phase at the working temperature of the OER-cell. Typical metal sulfide compounds which can be used in the present invention are Fe.sub.3S.sub.4, Fe.sub.7S.sub.8, Ni.sub.3S.sub.4, Co.sub.3S.sub.4, NiFe.sub.2S.sub.4, ZnFe.sub.2S.sub.4, NiFeZnS.sub.4, etc.

[0041] In another preferred embodiment the metal carbide is selected from the group consisting of compounds comprising carbon and one or more transition metal elements. Preferably binary metal carbides have the formula T.sub.xC.sub.y, wherein T is selected from the group consisting of transition. x and y independently from one another represent an integer from 1 to 5. All of these metal carbides exhibit a non-zero Berry Phase at the working temperature of the OER-cell. More preferably the metal carbide is selected from one or more compounds selected from Fe.sub.2C, Fe.sub.5C.sub.2, Fe.sub.3C, Co.sub.3C, and NiC.

[0042] In another preferred embodiment the Heusler alloys have a composition of TT′Z (half-Heusler) or T.sub.2T′R (full-Heusler), wherein T and T′ are selected from the group consisting of transition metals, and R is in element from IUPAC group 13, 14 or 15. All of these metal alloys exhibit a non-zero Berry Phase at the working temperature of the OER-cell. Typical Heusler alloys that can be used in the present invention are Mn.sub.2NiSb, Ni.sub.2MnGa, Co.sub.2MnGa, Cu.sub.2MnSb, NiCrSi, NiCrGe, NiCrGa, etc.

[0043] It was very surprising that the increase in electrochemical activity occurred already at a constant magnetic field strength as low as ≤200 mT. It was believed that the increase of OER activity by a constant magnetic field is a result of the Magneto Hydrodynamic Effects (MHD). This would imply that the bigger the applied magnetic field, the faster of desorption of oxygen bubbles and also the transport of oxygen radicals to the surface of the catalyst. Accordingly, it was assumed that an increase in magnetic field strength inevitably goes along with an increase in OER activity. Surprisingly, the catalysts defined and selected in the present invention work even better at lower magnetic field strength, e.g. at 200 mT, which is against all previous understanding. Without wishing to be bound by this theory it is believed that this is caused by modifying the spin structure of the catalysts, rather than the oxygen bubbles and solution. Catalysts with unfilled e.sub.g orbitals have unpaired electrons, the spin orientation of which can easily be controlled by a small magnetic field, even as lower as 200 mT and lower.

[0044] The magnetic field strength in the present invention can be varied e.g. by varying the distance of the catalyst from a permanent magnet as shown in FIG. 2 or by using an electromagnet with variable but constant magnetic field strength. The magnetic field strength at a given distance can be measured with a magnetometer.

Examples

[0045] The invention is explained in more detail below with reference to examples.

[0046] Catalytic Measurement Method

The OER catalytic measurements were performed on an Autolab PGSTAT302N electrochemistry workstation with an impedance module (Metrohm Autolab, B.V. Utrecht, The Netherlands). A conventional three electrode cell configuration was used in the measurement. An Ag/AgCl (3 M KCl) electrode was used as reference electrode, and a graphite rod was used as the counter electrode. The Ni foam with loaded electrocatalysts was attached to a Ti-plate and served as working electrode. The electrolyte was an Ar saturated 1 M KOH solution. Linear sweep voltammograms were recorded with a scan rate of 5 mV/S. All potentials used in this work were referenced to a reverse hydrogen electrode (RHE).

[0047] The experiment setup is shown in FIG. 1 and consists of a counter electrode (1), reference electrode (2), OER catalyst (3) and a permanent magnet (4). The permanent magnet (4) was placed in line with the glass reaction vessel facing the electrocatalyst. The applied magnetic field strength on the electrocatalyst can be controlled by the distance between the magnet and the catalyst.

[0048] FIG. 1 shows the electrochemical setup for OER in the presence of an external magnetic field. The magnetic field is perpendicular to the catalyst surface. Thus, the whole catalyst is submerged in a homogeneous magnetic field.

[0049] FIG. 2 shows the distance depended magnetic field strength of the used magnet. The distance is defined as the length between the surface of the magnet and the surface of the catalyst. From the distance, one can determine the applied magnetic field strength on the catalyst with the graph of FIG. 2.

[0050] FIG. 3 shows the linear sweep voltammogram (LSV) OER curves of Ni foam with and without the application of an external magnetic field. The y-axis represents the absolute OER current of the Ni foam.

[0051] FIG. 4 shows the linear LSV curves of Ni foam with and without the application of an external magnetic field. The y-axis represents the current density. This is commonly used to evaluate the OER performance of electrocatalysts.

[0052] FIG. 5 shows the Galvanostatic (constant potential) measurement of electrochemical activity of Ni foam with and without an external magnetic field.

[0053] FIG. 6 shows the distance dependent Galvanostatic (constant potential) measurement of electrochemical activity of Ni foam in the presence of an external magnetic field.

[0054] FIG. 7 shows the stability test of Ni foam in the presence of an external magnetic field.

[0055] FIG. 8 shows the magnetic field lines with reference to the surface of the catalyst plate; on the left side the field lines are oriented perpendicular to the plate face of the catalyst (=preferred embodiment) and on the right side the field lines are oriented parallel to the plate face of the catalyst.