CA2922876C - Process for forming a metal supported solid oxide fuel cell - Google Patents
Process for forming a metal supported solid oxide fuel cell Download PDFInfo
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- CA2922876C CA2922876C CA2922876A CA2922876A CA2922876C CA 2922876 C CA2922876 C CA 2922876C CA 2922876 A CA2922876 A CA 2922876A CA 2922876 A CA2922876 A CA 2922876A CA 2922876 C CA2922876 C CA 2922876C
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B05—SPRAYING OR ATOMISING IN GENERAL; APPLYING FLUENT MATERIALS TO SURFACES, IN GENERAL
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- B05D5/00—Processes for applying liquids or other fluent materials to surfaces to obtain special surface effects, finishes or structures
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- C25B9/00—Cells or assemblies of cells; Constructional parts of cells; Assemblies of constructional parts, e.g. electrode-diaphragm assemblies; Process-related cell features
- C25B9/17—Cells comprising dimensionally-stable non-movable electrodes; Assemblies of constructional parts thereof
- C25B9/19—Cells comprising dimensionally-stable non-movable electrodes; Assemblies of constructional parts thereof with diaphragms
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- H01M4/90—Selection of catalytic material
- H01M4/9016—Oxides, hydroxides or oxygenated metallic salts
- H01M4/9025—Oxides specially used in fuel cell operating at high temperature, e.g. SOFC
- H01M4/9033—Complex oxides, optionally doped, of the type M1MeO3, M1 being an alkaline earth metal or a rare earth, Me being a metal, e.g. perovskites
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- H01M8/00—Fuel cells; Manufacture thereof
- H01M8/10—Fuel cells with solid electrolytes
- H01M8/1097—Fuel cells applied on a support, e.g. miniature fuel cells deposited on silica supports
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- H01M8/00—Fuel cells; Manufacture thereof
- H01M8/10—Fuel cells with solid electrolytes
- H01M8/12—Fuel cells with solid electrolytes operating at high temperature, e.g. with stabilised ZrO2 electrolyte
- H01M8/1213—Fuel cells with solid electrolytes operating at high temperature, e.g. with stabilised ZrO2 electrolyte characterised by the electrode/electrolyte combination or the supporting material
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- H01M2008/1293—Fuel cells with solid oxide electrolytes
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Abstract
Description
Background
The device is generally ceramic-based, using an oxygen-ion conducting metal-oxide derived ceramic as its electrolyte. As most ceramic oxygen ion conductors (for instance, doped zirconium oxide or doped cerium oxide) only demonstrate technologically relevant ion conductivities at temperatures in excess of 500 C (for cerium-oxide based electrolytes) or 600 C (for zirconium oxide based ceramics), SOFCs operate at elevated temperatures.
anode has consisted of a porous ceramic-metal (cermet) composite structure, with nickel as the metallic phase and an electrolyte material (usually yttri a or Scandia-stabilised zirconia) as the ceramic phase, although less commonly a doped ceria-based electrolyte material such as gadolinia or samaria-doped ceria have also been used. In this structure, the nickel performs the role of catalyst, and the volume fraction of nickel is high enough that a contiguous metal network is formed, thus providing the required electronic conductivity.
The electrolyte material forms a contiguous ceramic backbone to the anode, providing mechanical structure, enhancing the bond between the anode and the electrolyte and also extending the anode-electrolyte interfacial region some distance into the anode.
However, should the supply of fuel gas be interrupted with the SOFC at operating temperature, the atmosphere within the anode will become oxidising. Under these conditions the metallic nickel will oxidise back to nickel oxide. This oxidation is associated with a volume increase of greater than approximately 40% because the metallic nickel which has been formed by the reduction of sintered nickel oxide does not oxidise back to the same morphology as the original nickel oxide from which it was formed.
Instead it generates mesoporosity, occupying a larger volume than the original nickel oxide. This volume change on reoxidation can generate large stresses in the anode structure, which in turn can result in cracking of the anode and potential destruction of the SOFC cell.
systems generally require the presence of complex and expensive purge gas systems to maintain a reducing atmosphere over the anodes in the event of an unexpected fuel interruption, for example due to a failure elsewhere in the system which requires an emergency shutdown of the system for safety reasons.
As thinner layers can be used in anode supported cells, operation temperatures can be reduced, which is generally desirable as it facilitates the use of lower-cost materials in the SOFC system, and reduces the rate of various material degradation mechanisms such as the oxidation of metallic components.
cell in an anode-supported cell, the cells are very prone to catastrophic failure on repeated REDOX cycling, as stress-induced cracking can result in the cell completely breaking up.
= Not using an anode supported cell - the anode can therefore be thinner;
reducing the overall volume change through REDOX cycling and the danger of catastrophic cracking.
= Operating at a lower temperature - the rate of nickel oxidation increases exponentially with increasing temperature, starting at >300 C. The lower the temperature of operation, the less risk of nickel oxidation and volume expansion.
Further, nickel particles tend to oxidise though a core-and-shell mechanism, where the outer surface oxidises rapidly, but then the core of the particle oxidises more slowly as this is diffusion limited. Thus at lower temperatures, it is likely that only the outer surface of the nickel particles in the anode will reoxidise, not the entire particle and any volume change will be reduced.
= Provide the anode with a contiguous ceramic 'backbone' - As the electrolyte-based ceramic phase used in SOFC anodes is largely unaffected by changes in oxygen partial pressure, this part of the anode will not change volume during REDOX cycles affecting the nickel phase. Thus the structural integrity of the anode and its bond to the electrolyte will be enhanced if there is a sintered porous ceramic network within the anode.
cell uses a fenitic stainless steel foil as a structural support. The foil being made porous in its central region to allow fuel access to the anode. The active cell layers (anode, electrolyte and cathode) are all deposited on top of the substrate foil as films. This means the anode only needs to be around 15um thick as it is not the structural support for the cell. This cell also allows operation at temperatures in the range 450 to 650 C, much lower than standard operating temperatures. This is achieved through the use of predominantly cerium oxide (ceria)-based ceramic materials such as CO010 (gadolinium doped-cerium oxide.
for CGO
- Ce09Gd0.101.95) as the oxygen ion conducting electrolyte, which have an intrinsically higher oxygen ion conductivity than zirconia-based materials. A thin film of stabilised zirconia is deposited in the electrolyte to prevent internal short-circuiting of the cell due to 10 the mixed ionic-electronic conductivity of ceria-based electrolytes, as disclosed in GB 2 456 445, but as the zirconia layer is so thin, its resistance to oxygen ion transport is sufficiently low that low-temperature operation is not prevented. The SOFC
cell of GB 2 368 450 uses a porous metal-CG010 composite cermet anode fabricated as a thick film with a thickness between 5 and 30 m. The anode is generally deposited by screen-printing an ink containing metal oxide and CG010 powders and formed into a porous ceramic layer by thermal processing to sinter the deposited powders together to form a contiguous structure bonded to the steel substrate.
This upper limit is substantially below the 1200 to 1500 C typically used when sintering ceramics and so methods have been developed for sintering rare earth-doped ceria electrolytes to >96% of theoretical density at <1100 C, facilitating the formation of the gas-tight layer desired (GB 2 368 450, GB 2 386 126 and GB 2 400 486).
This is because composites of two different oxide materials have been found to sinter more poorly than a single phase material. Thus nickel oxide or the ceramic alone will sinter adequately at these temperatures, but as a composite sintering in air can be poor, leading to weak necks between particles and a weak ceramic structure. This can result in cell failure as a result of REDOX cycling, as the weak bonds between nickel particles break as a result of the volume changes during the REDOX cycle. This can ultimately result in the catastrophic failure of the cell through delamination of the electrolyte from the anode.
Vieweger, R
Muecke, N. Menzler, M. Ruettinger, Th. Franco and H. Buchkremer. Lucerne:
s.n., 2012. Proceedings of the 10th European SOFC forum. Vol. Chapter 7, pp. 13/109-19/109) and Rodriguez-Martinez et al. (Tubular metal supported solid oxide fuel cell resistant to high fuel utilisation. L. Rodriguez-Martinez, L. Otaegui, A. Arregi, M.
Alvarez an I.
Villareal. Lucerne: s.n., 2012. Proceeding of the 10th European SOFC forum.
Vol.
Chapter 7, pp. 39/109-48/109) have avoided these issues by firing the ceramic layers onto the metal support in a strongly reducing atmosphere, usually a mixture of hydrogen and an inert gas such as nitrogen or argon. The reducing atmosphere avoids excessive oxidation of the steel, allowing higher processing temperatures more typical of those used in conventional ceramic processing to be used. However the use of such an atmosphere has a number of drawbacks for metal supported SOFCs of the type disclosed in GB 2 368 450:
= Method inappropriate for use with ceria-based electrolytes - which cannot be fired in a strongly reducing atmosphere, as the volume expansion associated with the reduction of Ce4+ ions to Ce3+ ions at high temperature generates mechanical stresses sufficient to crack the electrolytes.
= The reducing atmosphere means the anodic nickel is present as nickel metal -which tends to sinter excessively at >1100 C, resulting in an anode with inadequate porosity and poor electrochemical performance due to low catalytic surface area at the anode-electrolyte interface.
= Interdiffusion of nickel - at high temperatures in a reducing atmosphere, there tends to be extensive interdiffusion of nickel from the anode with ions from the support (where the support is steel, typically with iron ions). This can result in an unstable anode containing a high percentage of metals, such as iron, other than the nickel, and regions of the support where the presence of nickel in the support causes the formation of an austenitic phase in the support, the austenitic phase having a much higher coefficient of thermal expansion (CTE).
= Limited choice of cathode materials - most SOFC cathode materials cannot be sintered in a reducing atmosphere as they are usually mixed metal oxide materials which tend to reduce and decompose irreversibly into their constituent oxides and/or native metals under these conditions. As such, even if the anode and electrolyte are sintered in a reducing atmosphere, the cathode must be sintered in air. Exposing the nickel in the anode to air will cause it to reoxidise.
2009.
ECS Proc. Vol. 25(2), p. 681). This allows for the ceramic to be fired in a reducing atmosphere as it contains no nickel. The nickel content which should be present for the anode to function can be added post-electrolyte sintering by infiltration of the porous ceramic network with a solution of nickel salts, followed by thermal decomposition to form nickel oxide. However, the infiltration step, whilst allowing the use of a reducing atmosphere during sintering, may be difficult to scale up to industrial production because of the requirement for multiple infiltration, drying and decomposition steps in order to deposit the >20 volume% nickel into the porous ceramic structure required to form an electronically conductive network. As a further issue, the very high surface area nickel oxide formed by low-temperature decomposition of metal salts tends to readily sinter as nickel metal under typical SOFC operating conditions, leading to the potential for loss of catalytic activity and/or electronic conductivity, both of which can lead to rapid cell performance degradation.
Prenninger, J. Nielsen, P. Blennow, T. Klemenso, S. Ramousse, A. Kromp and A.
Weber. Lucerne: s.n., 2012. Proceedings of the 10th European SOFC forum. Vol.
Chapter 7, pp. 20/109-29/109) requires the formation of the anode structure as a cermet of zirconia and powdered stainless steel, co-sintered in a reducing atmosphere. The stainless steel acts as the electronically conductive network of the anode, meaning that a much smaller amount of nickel needs to be post-infiltrated into the network to act as an electrocatalyst.
Whilst this approach can work, there are risks of anode poisoning due to the very close proximity of the catalytically active part of the anode and the chromium-containing stainless steel. The support is also potentially vulnerable to corrosion of the stainless steel particles if they are not fully coated with a passivating chromium oxide scale.
Summary
a) applying a green anode layer including nickel oxide and a rare earth-doped ceria to a metal substrate;
b) prefiring the anode layer under non-reducing conditions to form a composite;
c) firing the composite in a reducing atmosphere to form a sintered cermet;
d) providing an electrolyte; and e) providing a cathode;
wherein the atmosphere comprises an oxygen source.
2 (1) 112 + CO, CO + 1120 (2) CO + ¨2 02 CO2 (3)
This results in significant amounts of contamination (often, where steel is used in the form of iron oxide) being present in the anode during subsequent firing steps, and, where steel is used, distortion of the substrate due to the formation of an austenitic phase within the steel.
This distortion occurs as the austenitic phase has a much higher coefficient of thermal expansion than the rest of the substrate.
Date Recu/Date Received 2021-10-13
Further, the reduction of nickel oxide to nickel may be substantially fully complete, or mostly fully complete, for instance the reduced nickel may be present in the range 95 -99.9 wt% nickel, perhaps 98 - 99.5 wt% nickel, perhaps 99 to 99.5 wt%.
As such, there is provided a process wherein in firing step c) the nickel oxide is reduced to nickel metal prior to sintering. These methods provide for full reduction of nickel oxide to nickel before sintering, and are believed to cause less stress to the anode, and result in less cracking, than where nickel oxide is sintered prior to reduction.
Each of these features contribute to an efficient transfer of fuel through the substrate to the anode, whilst allowing the metal substrate to support the fuel cell, facilitating the use of dramatically reduced thicknesses of the electrochemically active layers within the cell.
These compounds are generally used as they have a higher oxygen ion conductivity than many electrolyte materials, including zirconia-based materials; thereby allowing operation of the fuel cell at lower temperatures than conventional SOFCs, the temperature of operation of the fuel cell of the invention typically being in the range 450 to 650 C, often 500 to 620 C.
Operating the fuel cell at lower temperatures has a number of benefits, including reduced rate of oxidation of nickel in non-reducing atmospheres, which in turn often results in only the outer shell of the particle oxidising, reducing volume change within the anode and hence risk of cracking in the event that the reducing atmosphere of the fuel supply is interrupted. Further, it makes the use of metal supports possible, allowing thinner layers of electrode and electrolyte material to be used, as these play less of a structural role, if any at all.
Where a porous region is present, the application of the ink to the substrate will typically be such that a layer is formed over the porous region, but the non-porous region is left substantially uncovered. This ensures that the fuel cannot bypass the anode, but minimises material costs and weight by covering no more of the substrate than necessary.
Gentle heat is often used to speed up the formation of the printed layer. Temperatures in the range 50 to 150 C would be typical. The drying step evaporates solvents and sets any binders in any ink formulation used, solidifying the ink and forming an initial, albeit fragile, anode layer, termed here the printed layer. This layer will generally be of thickness in the range 5 to 40 [tm, often 7 to 20 [tm, often 9 to 15 um. As the fuel cells of the invention are not anode supported cells, the anode layer can be much thinner than in many conventional fuel cells, which has the advantage that the overall volume change during REDOX cycling is smaller, and so cracking of the anode over time is significantly reduced. The application of the green anode layer may therefore include the steps of initial application of the ink to the metal substrate, and drying the ink to provide a printed layer of thickness in the range 5 to
[0040] In many cases, the process of the invention will further comprise the step of compressing the green anode layer at pressures in the range 100 to 300 MPa.
This compression step increases the density of the of the unsintered green anode layer, ensuring that the particles of nickel oxide and rare earth-doped ceria are in sufficiently close contact to sinter effectively at the temperatures employed in the process of the invention.
However, the use of a compression step is not essential, as firing the anode layer in reducing conditions as defined in firing step c) strongly favours sintering of the rare earth-doped ceria and the nickel oxide, and so it may be that this step is omitted.
Where present, it will often be the case that the compression step is used in combination with a step of heating the printed layer to remove residual organic materials from the ink base prior to compression, to leave a green anode layer comprising nickel oxide and a rare earth-doped ceria that may be compressed. A variety of compression methods may be used, as would be known to the person skilled in the art, although often uniaxial or cold isostatic pressing will be used.
Whilst the firing period must be sufficient to allow removal of any residual organic matter from the ink, initial sintering of the oxide-ceramic composite, and to allow the furnace to reach thermal equilibrium; too long a firing period can increase oxidation of the metal support and lead to contamination of the anode with, where ferritic stainless steel is used, chromium evaporating from the support. Hence, the optimal firing period is in the range 15 to 60 minutes.
This is particularly important during the heating steps which lead to the formation of the anode, as once the anode cermet is formed, this will help to maintain the substrate conformation. Typically, the substrate will be thick relative to the electroactive layers, and layers of electroactive substances will be formed on the substrate to produce the SOFC, bracing will therefore generally be to keep the substrate flat, and the bracing may be achieved using a wide variety of methods, as would be known to the person skilled in the art. This could include pinning, clamping or weighting of the substrate.
Weighting of the substrate would often include the application of a ceramic frame around the edge of the anode.
Further, it has been found that residence times in the range 15 to 60 minutes are appropriate to ensure good sintering without unnecessary contamination of the anode with, where ferritic stainless steel is used, chromium evaporating from the support.
Further, metallic nickel sinters far more readily than nickel oxide at the same temperature, and is also highly ductile, meaning it can easily move to accommodate sintering of the rare earth-doped ceria phase. At this temperature range the sintering of metallic nickel is not excessive (as would be the case at more conventional ceramic sintering temperatures), but a strong porous sintered network of metallic nickel is formed. In conventional anode formation methods, the nickel oxide would not be reduced, but sintered as nickel oxide with the rare earth-doped ceria. The nickel oxide would then be reduced for the first time upon commencement of operation of the cell, resulting in a volume change of the anode and hence possible cracking of the anode and separation from the electrolyte as a result of stresses at the anode-electrolyte interface. Reducing the nickel oxide to nickel and sintering as described above, before the electrolyte is present, dramatically reduces this volume change upon initial operation, and goes a long way to addressing the problem of cracking as described above.
This provides for an anodic material which has completed an entire reduction and oxidation cycle, forming a stable microstructure before the electrolyte is applied. As much of the microstructural change in the anode happens in the first REDOX cycle, including this reoxidation step reduces the risk of damaging microstructural changes due to subsequent REDOX
cycles in service, or in the case of loss of reducing atmosphere in use (for instance where there is a system failure preventing the fuel from flowing to the cell), oxidation of nickel to nickel oxide at operating temperature as described above.
.. [0049] The steps of providing the electrolyte and cathode are steps well known in the art.
Typically, the electrolyte for use with the fuel cells of the invention will be of thickness in the range 5 to 30 vim, often in the range 10 to 20 lam. The provision of such a thin electrolyte layer provides for rapid transfer of oxygen ions from the cathode, to the anode.
Often the electrolyte will comprise a rare earth-doped ceria, appropriate rare earth cerias being as defined above for the anode. In some examples, the electrolyte may comprise a rare earth-doped ceria combined with a low level of cobalt oxide, as a sintering aid, for instance, there may be in the range 0.5 to 5 wt% cobalt oxide, the remaining electrolyte being the rare earth-doped ceria. The use of rare earth-doped cerias for both the anode and electrolyte helps to enhance the compatibility between these components of the fuel cell both chemically and in terms of the thermal expansion, which is closely matched reducing the mechanical stress between layers during REDOX cycling, and hence also reducing the .. likelihood of cracking and fuel cell failure in use. Further, as these cerias have high charge transfer rates, their inclusion ensures a good rate of charge transfer between the electrolyte and the anode.
[0050] The electrolyte will generally be sintered in a separate firing step after the anode is fully formed, and optionally after the nickel has been reoxidised to nickel oxide.
.. [0051] Typically the cathode will be of thickness in the range 30 to 60 1..tm, often 40 to 50 pm. The cathode will generally comprise two layers, a thin active layer where the reduction of oxygen takes place, and a thicker current collector layer, to allow the current to be collected from a cell in the stack. The current collector layer will generally be a perovskite such as lanthanum strontium cobaltite, although any electronically conductive ceramic material may be used.
[0052] The active layer cathode may comprise a sintered powdered mixture of perovskite oxide mixed conductor and rare earth-doped ceria, the rare earth-doped ceria being as defined above. The perovskite may comprise Lai,SrxCoyFei_y03_6, where 0.5>x>0.2 and 1>y>0.2. In particular, the perovskite oxide mixed conductor may comprise one or more of .. Lao6Sro4Coo2Feo s03-8. Gdo5CoO3_s, and RE1Sr1_xCo03_d, (where RE= La, Sm, Pr and 0.5<x<0.8). It can be useful to use these compounds as they have a higher ionic conductivity than most perovskites. In some cases, the mixture comprises in the range 20 to 50 wt% rare earth-doped ceria, in some cases 30 to 45 wt%, in some cases 35 to 45 wt%, or around 40 wt% rare earth-doped ceria as defined above. This helps to enhance the .. compatibility between the cathode and electrolyte both chemically and in terms of the thermal expansion described above, and as these cerias have high charge transfer rates, their inclusion ensures a good rate of charge transfer between the electrolyte and the cathode.
[0053] The cathode will generally be sintered before use. The cathode will typically be .. applied as one or more layers (for instance active and current collecting) directly or indirectly over the sintered electrolyte and sintered under conditions similar those described above for the anode. This provides an intermediate temperature metal supported SOFC, which is robust to repeated REDOX cycling, and as a result of the anode structure formed, to fuel depravation whilst at high temperature.
[0054] In a second aspect of the invention there is provided a metal supported solid oxide fuel cell formed by a process according to the first aspect of the invention.
[0055] In some instances, the fuel cell will be a fuel cell of the type described in the applicants granted patent GB 2 368 450. In such cases. the fuel cell may comprise:
(i) a ferritic stainless steel support including a porous region and a non-porous region bounding the porous region;
(ii) a ferritic stainless steel bi-polar plate located under one surface of the porous region of the support and being sealingly attached to the non-porous region of the support about the porous region thereof;
(iii) an anode comprising an anode layer located over the other surface of the porous region of the support;
(iv) an electrolyte comprising an electrolyte layer located over the anode layer; and (v) a cathode comprising a cathode layer located over the electrolyte layer;
[0056] wherein the anode includes nickel and a rare earth-doped ceria and wherein the fuel cell has been formed by a process according to the first aspect of the invention.
[0057] The fuel cell may be present in a fuel cell stack, comprising two or more fuel cells, and there is therefore provided in a third aspect of the invention, a fuel cell stack comprising fuel cells according to the second aspect of the invention. Each fuel cell may comprise a bi-polar plate, as described above, to which the support may be welded, or otherwise sealed.
[0058] In a fourth aspect of the invention there is provided the use of a fuel cell according to the second aspect of the invention, in the generation of electrical energy.
[0059] The process of the invention is intended to provide a method for the manufacture of a highly sintered nickel-rare earth-doped ceria thick film anode suitable for use in a metal supported SOFC cell, whilst avoiding the problems of poor anodic sintering, degradation of the support, and delarnination of the electrolyte in use. It may he the case that the process is a process for forming a metal supported solid oxide fuel cell, the process comprising the steps of:
Date Recu/Date Received 2021-10-13 a) applying a green anode layer including nickel oxide and a rare earth-doped ceria (optionally both powdered, and optionally of particle size distribution d90 in the range 0.2 to 3 gm) optionally in the form of an ink to a metal substrate;
b) optionally, drying the ink to provide a printed layer of thickness in the range 5 to 40 gm;
c) optionally, compressing the green anode layer at pressures in the range 100 to 300 MPa;
d) optionally, bracing the metal, optionally for the steps of prefiring the anode layer and firing the composite, optionally by weighting the metal support;
e) prefiring the anode layer under non-reducing conditions (optionally in air) to form a composite optionally at a temperature in the range 950 to 1100 C;
f) firing the composite in a reducing atmosphere to forma sintered cermet, wherein the atmosphere optionally comprises an inert gas, a gaseous reducing agent and a gaseous oxygen source, the reducing agent optionally comprising 0.5 to 50 volume%
hydrogen, the oxygen source optionally comprising 0.01 to 50 volume% water vapour and the inert gas optionally comprising argon; wherein the firing of the composite optionally occurs at a temperature in the range 950 to 1100 C and the firing conditions optionally provide for reduction of the nickel oxide to nickel metal prior to sintering of the nickel containing component g) optionally, reoxidising the sintered nickel prior to the provision of the electrolyte;
h) providing an electrolyte; and i) providing a cathode.
[0060] The use of the processes described herein provide for a SOFC which because of the anodic structure is highly REDOX stable at intermediate operating temperatures (less than 650 C), the SOFC being capable of withstanding hundreds of high temperature fuel interruptions without significant cell performance degradation.
[0061] Unless otherwise stated each of the integers described in the invention may be used in combination with any other integer as would be understood by the person skilled in the art. Further, although all aspects of the invention preferably "comprise"
the features described in relation to that aspect, it is specifically envisaged that they may -consist" or "consist essentially" of those features outlined. In addition, all terms, unless Date Recu/Date Received 2021-10-13 specifically defined herein, are intended to be given their commonly understood meaning in the art.
[0062] Further, in the discussion of the invention, unless stated to the contrary, the disclosure of alternative values for the upper or lower limit of the permitted range of a parameter, is to be construed as an implied statement that each intermediate value of said parameter, lying between the smaller and greater of the alternatives, is itself also disclosed as a possible value for the parameter.
[0063] In addition, unless otherwise stated, all numerical values appearing in this application are to be understood as being modified by the term "about".
Brief Description of the Drawings [0064] In order that the present invention may be more readily understood, it will be described further with reference to the figures and to the specific examples hereinafter.
[0065] Figure 1 is a schematic representation of a SOFC as described in GB 2 368 450;
[0066] Figure 2 is a scanning electron micrograph (SEM) showing a cross section through a SOFC of Figure 1(15.0 kV, 7.9 mm x 1.50k);
[0067] Figure 3 is a thermodynamic phase diagram for a nickel/nickel oxide system covering the temperature range 500 to 1100 C and oxygen partial pressures in the range log p02 0 to -40;
[0068] Figure 4 is a thermodynamic phase diagram for a chromium/chromium oxide system covering the temperature range 500 to 1100 C and oxygen partial pressures in the range of log p02 0 to -40;
[0069] Figure 5 is a thermodynamic phase diagram for a nickel/nickel oxide system at 1030 C and 1 bar total pressure as a function of hydrogen and steam partial pressures;
[0070] Figure 6 is a thermodynamic phase diagram for a chromium/chromium oxide system at 1030 C and 1 bar total pressure as a function of hydrogen and steam partial pressures;
[0071] Figure 7 is a SEM showing a cross-section through a metallic support and anode of an SOFC of the invention after pre-firing in air (15.0 kV. 7.0 mm x 4.0k);
[0072] Figure 8 is a SEM also showing a cross-section through the metallic support and anode of firing in the reducing hydrogen atmosphere and reoxidation as described below (20.0 kV, 4000x);
[0073] Figure 9 is a SEM showing the cross-section of Figure 8 at higher magnification (20.0 kV, 13000x);
[0074] Figure 10 is a SEM showing a cross section through a SOFC made using the process of the invention;
[0075] Figure 11 is a current-voltage curve for the SOFC of Figure 10 as a function of cell operating temperature (56% hydrogen-44% nitrogen fuel, excess air fed to cathode);
[0076] Figure 12 is a power-cycle graph of the SOFC of Figure 10; and [0077] Figure 13 is a table of the results of mechanical strength tests undertaken on SOFC cells both after initial manufacture and after cells have operated in an initial performance characterisation test, for both standard nickel-CGO anodes as illustrated in Figure 2, and reduced fired nickel-CGO anodes as illustrated in Figure 8 .
Detailed Description [0078] A SOFC 10 as described in GB 2 368 450 is shown schematically in Figure 1, .. and in SEM cross-section in Figure 2. Both figures show a ferritic stainless steel substrate 1, made partially porous by laser-drilling thousands of holes though the central region of the substrate 2. The porous substrate includes a chromium oxide passivation layer 11, a nickel oxide and CGO anode layer 3 covering the porous region 2 of the substrate 1. Over the anode layer 3 is deposited a CGO electrolyte layer 4 (10 to 20 um, CGO), which overlaps the anode 3 onto the undrilled area 9 of the substrate 1, thus forming a seal around the edge of the anode 3. The cathode 5,6 has a thin active layer 5 (CGO
composite) where the reduction of oxygen takes place, and a thicker current collector layer 6 (lanthanum strontium cobaltite) to allow current to be collected from the cell 10 in a stack.
Figure 2 additionally shows a very thin stabilised zirconia layer 7 and an even thinner doped ceria layer 8, which block electronic conductivity (preventing short circuiting from undesirable chemical reactions between the cathode 5,6 and zirconia layer 7) and form the interface between the anode and electrolyte respectively.
[0079] SOFC 10 of Figures 1 and 2 was prepared by applying a screen-printing ink containing suspended particles of nickel oxide powder and CGO powder (d90 =
0.7 to 1.2um, ratio of nickel oxide to CGO in the ink being 1:0.55 by weight). The ink was screen printed onto _Lennie stainless steel substrate 1 using conventional methods, and dried in an oven to evaporate the solvents and set the binders thereby forming a dried, Date Recue/Date Received 2021-03-25 printed layer of thickness 9 to 15 p.m. The dried, printed layer was compressed using cold isostatic pressing at pressure of 300 MPa. The green anode layer was placed in a furnace and heated to a temperature of 960 C in air atmosphere for 40 minutes, to produce a sintered anode layer 3. A CGO electrolyte layer 4 was sprayed onto the anode layer 3 and fired in a furnace at 1020 C for 40 minutes. Finally, zirconia layer 7 was applied to the fired electrolyte layer by means of the method disclosed in GB 2 456 445 followed by application of the doped ceria layer 8 and the two cathodic layers 5,6 also using the methods of GB 2 456 445, before firing at a temperature of 825 C to produce the SOFC 1 structure.
[0080] In contrast the SOFC 10 of the invention, whilst appearing to have a similar structure to the SOFC 10 of Figures 1 and 2, is prepared in a different way and (as shown in Figures 7 to 10) exhibits a good sintering of the nickel oxide phase, a porous anode structure and a contiguous chromium oxide passivation layer 11, between the support 1 and the anode 3. In Figure 10 the electrolyte layer 4, cathodic layers 5,6, zirconia layer 7 and doped ceria layer 8 are also shown.
[0081] The SOFC of Figures 7 to 10 is prepared by applying screen printed ink containing suspended particles of nickel oxide powder and CGO powder (d90 =
0.7 to 1.2 pm, ratio of nickel oxide to CGO being 1:0.78). The ink was screen printed onto a ferritic stainless steel substrate using conventional methods and dried to evaporate the solvents and set the binders thereby forming a dried, printed layer of thickness 9 to 15 pm. The dried printed layer was fired in air at a temperature of 1020 C for 40 minutes to produce a sintered anode layer 3. The furnace was then allowed to cool to room temperature and the air purged from the system using a 5% hydrogen/argon mix.
[0082] An atmosphere comprising 4.85 volume% hydrogen, 2.91 volume% water vapour, the remainder being argon was introduced and the furnace heated to 1045 C. The water vapour was introduced into the dry mixture of hydrogen and argon by bubbling the hydrogen and argon mixture through deionised water resulting in an oxygen partial pressure in the reducing atmosphere in the range 10-17 to 10-19 bar. The composite was fired in this atmosphere and at this temperature for a time period of 40 minutes allowing reduction of nickel oxide to metallic nickel and sintering of the nickel and rare earth-doped ceria to form a cermet.
[0083] After 40 minutes the furnace was allowed to cool and the atmosphere switched to nitrogen bubbled through deionised water. This allowed the partial pressure of oxygen to rise to above 10-13 bar, leading to oxidation of nickel metal to nickel oxide.
[0084] After cooling completely, the anode was re-oxidised by heating it in a furnace in air to 700 C for 60 min.
[0085] The sintered anode 3 was then treated as described above for Figures 1 and 2 in order to form a complete solid oxide fuel cell comprising CGO electrolyte layer 4, zirconia layer 7, doped ceria layer 8, and two cathodic layers 5,6.
Examples Nickel Oxide and Chromium Oxide Stabilities [0086] The stability of nickel, nickel oxide, chromium, and chromium oxide are of interest in the systems of the invention, as the reduction of nickel oxide to nickel is a key to the functioning of the anode. The formation and preservation of the passivation layer on the SOFC support, which will typically be chromium oxide as ferritic stainless steel substrates are the substrates most commonly used, is important to the prevention of diffusion between the support and the anode, which can potentially contaminate both the anode, reducing it's efficiency, and the support, forming austenitic phases and reducing the supports structural integrity. In addition, the passivation layer prevents degradation of the support during the firing steps used in formation of the fuel cell, and then in use.
[0087] Figure 3 shows a thermodynamic phase diagram for a nickel/nickel oxide system showing the limits of thermodynamic stability of metallic nickel as a function of temperature and oxygen partial pressure. It can be seen that at 1000 to 1100 C, the .. metallic nickel is stable at an oxygen partial pressures as high as 10-13 to 10-14 bar.
Therefore, at these and lower partial pressures of oxygen, nickel oxide will reduce to metallic nickel.
[0088] Figure 4 shows the equivalent phase diagram for a chromium/chromium oxide system showing that at 1000 to 1100 C, metallic chromium is only stable at oxygen partial pressures of 10-22 to 10-24 bar or below. Therefore, at oxygen partial pressures above around 10-22 bar a chromium oxide passivation layer will be retained.
[0089] Figure 5 shows a phase diagram for the nickel/nickel oxide system at 1030 C and 1 bar total pressure as a function of hydrogen and steam partial pressures, showing that any gas mixture containing 0.5-10% water vapour and 1-20% hydrogen is sufficiently reducing that the only stable phase is metallic nickel.
[0090] Figure 6 shows the equivalent phase diagram for the chromium/chromium oxide system showing that for the same range of gas mixtures the only thermodynamically stable phase is chromium oxide.
SOFC Structure [0091] Figure 7 shows a SEM cross-section of an anode 3 produced by the method described herein, after the initial firing in air. This image shows the ferritic stainless steel substrate 1, a thermally grown chromium oxide scale 11 on the substrate 1, and a weakly sintered porous anode structure 3 consisting of nickel oxide (dark phase - 45 volume%) and CGO (light phase - 55 volume%). Figure 8 is a cross-section of this anode 3 after firing in the reducing atmosphere subsequent reoxidation, and Figure 9 a higher magnification image of the same anode 3 microstructure. These figures show that the chromium oxide passivation layer 11 remains intact after firing, and that a good sintering of both the nickel oxide phase 12 and the lighter CGO phase 13 is present.
Good sintering is evidenced by a clear distinction between ceramic and metallic regions. The ceramic regions appearing as light regions and the metallic regions as dark patches.
[0092] Figure 10 shows a complete SOFC cell 10 with an anode 3 produced by the method described herein after operation of the fuel cell 10. The anode structure 3 can be seen after reduction of the nickel oxide in the anode 3 back to metallic nickel during SOFC
operation, along with the other parts of the SOFC 10 as described above.
[0093] The resulting anode structure has been demonstrated to be highly REDOX-stable at operating temperatures of <650 C, being capable of withstanding hundreds of high-temperature fuel interruptions without significant cell performance degradation.
SOFC Performance [0094] Figure 11 is a current-voltage polarisation curve for the fuel cell of Figure 10, at different operating temperatures. Fuelling rate was calculated to give approximately 60%
fuel utilisation at 0.75V/cell at each of the measured temperatures, showing that the system can be operated across a range of temperatures at least as broad as 492 to 608 C, allowing the operational temperature to be optimised for application, number of cells in the stack, output required etc.
[0095] Figure 12 shows the very good REDOX stability possible with this anode structure. A series of cycles are run at 600 C on a seven-layer short stack, where a current-voltage curve is run to establish the stack performance. The stack is then returned to open circuit, and the hydrogen supply to the stack is cut whilst maintaining the stack at 580-600 C. Air and nitrogen are maintained to the stack during this period. The fuel interruption is sustained for 20 minutes, allowing time for the anode to partially reoxidise.
The hydrogen feed is then restored, and after giving the stack a few minutes to recover, another current-voltage curve is run to determine if stack performance has been lost as a result of the REDOX cycle of the anode. This sequence continues until stack performance starts to fall, indicating damage to one or more cells as a result of REDOX
cycling.
[0096] It can be seen from Figure 12 that with the SOFC cell of Figure 10, the seven cells within the stack will tolerate more than 200 REDOX cycles without any measurable loss of performance after a small initial burn-in, with 291 cycles being run in total. A loss of performance observed after 200 cycles was in this instance was due to the failure of one cell at the bottom of the stack; it is believed that mechanical optimisation of the stack design can avoid failure of that layer leading to even greater REDOX
stability.
[0097] Figure 13 is a table of the results of mechanical strength tests undertaken on SOFC cells both after initial manufacture and after cells have operated in an initial performance characterisation test, for both standard nickel-COO anodes as illustrated in Figure 2, and reduced fired nickel-COO anodes as illustrated in Figure 8. The after operating test for the reduced fired nickel CGO anodes included over 250 REDOX
cycles.
[0098] In the as-manufactured cells, the anodes are in the oxidised state and prior to the mechanical test they are reduced in order to mimic the anode structure in the cell at the start of operating, whereas the anodes in the after operating cells are in the final cermet state of the working anodes.
[0099] In order to perform the mechanical strength measurement on the cells, the metal substrates of the cells are first glued to a flat steel plate to prevent the cells flexing when a pulling force is applied. The cathodes of the cells are removed mechanically, exposing the electrolyte.
[00100] To assess the mechanical strength of the anode and/or the anode-electrolyte bond, circular metal test pieces are glued to the electrolyte surface in the four corners of the electrolyte and the middle of the cell. A diamond scribe is used to cut through the ceramic layers of the cell around the metal test piece. A calibrated hydraulic puller is then attached .. to the test piece and used to measure the stress required to pull the test piece off the cell substrate. A maximum pulling stress of 17MPa may be applied using this technique, after which the glue holding the test piece to the electrolyte tends to fail rather than the fuel cell layers on test. Should the test piece be pulled off at less than 17MPa this indicates the failure stress of the weakest cell layer (usually the internal structure of the anode).
[00101] It can be seen that whilst the standard nickel-CGO anodes are strong in the as-manufactured state, they fail at much lower stresses after reduction of the nickel oxide to metallic nickel in the after operating cell. Without being bound by theory, it is believed this is largely because of the lack of a contiguous ceramic structure within the anode, meaning the mechanical strength of the anode is provided entirely by relatively weak necks between nickel particles. By contrast it can be seen that the reduced fired nickel-COO anodes retain their strength after reduction to the cermet structure, indicating much greater sintering of both metallic and ceramic phases.
[00102] It should be appreciated that the processes and fuel cells of the invention are capable of being incorporated in the form of a variety of embodiments, only a few of which have been illustrated and described above.
Claims (14)
a) applying a green anode layer including nickel oxide and a rare earth-doped ceria to a metal foil substrate;
b) thereafter, pre-firing the anode layer at a temperature in the range 950 to under non-reducing atmosphere to fonn a composite and an oxide passivation layer interposed between the composite and the metal substrate;
c) thereafter, firing the composite in a reducing atmosphere to form a sintered cermet, form nickel metal, maintain the rare earth-doped ceria in a partially-reduced state, and retain the passivation layer;
d) thereafter, providing an electrolyte; and e) thereafter, providing a cathode;
wherein the reducing atmosphere comprises a reducing agent and an oxygen source, wherein an oxygen partial pressure in the reducing atmosphere of step c) is in the range 10' to 1022 bar.
Date Recu/Date Received 2021-10-13
Date Recu/Date Received 2021-10-13
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| GB1315744.1A GB2517927B (en) | 2013-09-04 | 2013-09-04 | Process for forming a metal supported solid oxide fuel cell |
| GB1315744.1 | 2013-09-04 | ||
| PCT/GB2014/052546 WO2015033103A1 (en) | 2013-09-04 | 2014-08-20 | Process for forming a metal supported solid oxide fuel cell |
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| CA2922876C true CA2922876C (en) | 2022-07-12 |
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| EP (1) | EP3042412B1 (en) |
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2013
- 2013-09-04 GB GB1315744.1A patent/GB2517927B/en active Active
- 2013-10-14 US US14/053,216 patent/US10003080B2/en active Active
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2014
- 2014-08-20 SG SG11201601148SA patent/SG11201601148SA/en unknown
- 2014-08-20 JP JP2016539626A patent/JP2016533016A/en not_active Withdrawn
- 2014-08-20 RU RU2016105829A patent/RU2670423C2/en active
- 2014-08-20 CA CA2922876A patent/CA2922876C/en active Active
- 2014-08-20 KR KR1020167005831A patent/KR102232286B1/en active Active
- 2014-08-20 WO PCT/GB2014/052546 patent/WO2015033103A1/en not_active Ceased
- 2014-08-20 EP EP14756114.6A patent/EP3042412B1/en active Active
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Also Published As
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|---|---|
| GB2517927B (en) | 2018-05-16 |
| HK1204150A1 (en) | 2015-11-06 |
| US10003080B2 (en) | 2018-06-19 |
| JP6794505B2 (en) | 2020-12-02 |
| JP2016533016A (en) | 2016-10-20 |
| GB2517927A (en) | 2015-03-11 |
| RU2670423C2 (en) | 2018-10-23 |
| CN105518921A (en) | 2016-04-20 |
| KR20160048810A (en) | 2016-05-04 |
| US20150064596A1 (en) | 2015-03-05 |
| JP2019204788A (en) | 2019-11-28 |
| CA2922876A1 (en) | 2015-03-12 |
| MX381827B (en) | 2025-03-11 |
| SG11201601148SA (en) | 2016-03-30 |
| WO2015033103A1 (en) | 2015-03-12 |
| GB201315744D0 (en) | 2013-10-16 |
| EP3042412B1 (en) | 2020-11-25 |
| EP3042412A1 (en) | 2016-07-13 |
| RU2016105829A (en) | 2017-10-09 |
| CN105518921B (en) | 2019-06-25 |
| MX2016002175A (en) | 2016-07-05 |
| KR102232286B1 (en) | 2021-03-26 |
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