This application is a § 371 application from PCT/EP2008/066783 filed Dec. 4, 2008, which claims priority from German Patent Application No. 10 2007 058 596.0 filed Dec. 4, 2007, each of which is herein incorporated by reference in its entirety.
The invention relates to a blocking layer in a fuel cell for preventing reactions between the electrolyte and anode and the electrolyte and cathode.
The anode and the electrolyte and also the cathode and the electrolyte are in direct material contact in fuel-cell applications. In particular, high-temperature fuel cells, for example SOFC (solid oxide fuel cells), with working temperatures >400° C. are to be mentioned here. In accordance with the prior art, the anode and the electrolyte and also the electrolyte and the cathode react at temperatures >400° C. in a solid chemical manner. This reaction results in the material of the anodes being able to migrate into the electrolyte or vice versa, or that material of the cathodes can migrate into the electrolyte or vice versa. The effect thereof is the change in the electrical energy yield of the fuel cells. This change is a process that is accelerated by rising temperatures and/or sustained duration.
In order to prevent the diffusion, at the present time blocking layers are used whose property is a material density that is as high as possible, a so-called dense structure, as shown in
The object of the invention consists in putting forward a blocking layer that eliminates the solid chemical reactions between the electrolyte and the anode and cathode to the greatest possible extent.
The object is achieved with the aid of the characterising features of the first claim; advantageous developments of the invention are claimed in the dependent claims.
In contrast with the prior art, in accordance with the invention a porosity is introduced into the blocking layer in a controlled manner, as shown in
As a result of the pores 6 a deficiency of material is produced in which diffusion can take place, because only the frame structure formed by the material of the blocking layer presents the possibility for diffusion. It is not the pore 6 as a hollow space that is the actual functional carrier, but the frame structure. The pore, whether open or closed, is therefore intended to displace material. As a result of the pores, solid chemical reaction paths which are as narrow as possible are created that hinder free or large-area diffusion from the anode into the electrolyte or vice versa and/or from the cathode into the electrolyte or vice versa.
The blocking layer is an electrochemical functional layer and preferably consists of a ceramic material.
The layer thickness of the blocking layer amounts to 0.1 to 40 μm. It is dependent upon the particle size which in turn has influence upon the size of the pores. As a rule, with a small particle size of the material, a small pore diameter and a large proportion of pores, the selected thickness of the blocking layer can be small. No channels may develop through open pores through the blocking layer that render possible percolation of the material or cause a short circuit. If the functional layer is too thick, the electrical resistance rises and the energy discharge out of the fuel cell becomes lower. The thickness and the porosity are parameters that can be used as a definition for this functional layer.
As shown in
Material paths develop in the blocking layer as a result of the porosity, as already explained. These lengthen the diffusion stretch for the material that is diffusing in, as can be seen from
As a result of the porosity a surface-enlargement of the material of the blocking layer develops. With bulk material, the surface is defined by length—breadth—thickness. The pore is to be seen as a thinning of the bulk material. The function of the pore and frame is interchanged, that is, the “filter effect” takes place by way of the frame.
For the blocking layer a total porosity of 1 to 55% by volume is of particular technical significance.
Advantageously, the porosity is graduated. The graduation can be designed on the basis of two different functions. The first principle is the tooth construction with the adjacent layers. The second principle is the direction of diffusion, that is, if the adjacent layer presents that substance that would diffuse across the material of the blocking layer, then here, for example, the blocking layer starts with a high proportion of pores that diminishes in the direction of the bulk material of the blocking layer. Since there are a great variety of possibilities for graduation here, this is to be regarded as an example and not as a restriction.
The blocking layer can lie between the electrolyte and the cathode. It can, however, also lie between the electrolyte and the anode. Furthermore, a combination of the layers can also be provided. The blocking layer can be applied by means of screen printing or laminating techniques or coating methods, such as spraying or roller coating.
The material of the blocking layer is of particular technical significance and consists, for example, of cerium oxide and/or technical cerium oxide and/or doped cerium oxide and/or zirconium oxide and/or technical zirconium oxide and/or doped zirconium oxide and mixtures thereof. As dopants, the oxides of Sm and Gd are to be mentioned by way of example. Technical substances always have a proportion of foreign substances and secondary constituents. Cerium oxide is as a rule obtained from a ground single crystal and therefore has the highest material purity.
The blocking layer is applied to part of or all over at least one surface, as can be seen from
Number | Date | Country | Kind |
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10 2007 058 596 | Dec 2007 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2008/066783 | 12/4/2008 | WO | 00 | 8/18/2010 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2009/071624 | 6/11/2009 | WO | A |
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Entry |
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MAchine translation in English of JP 2008186798. |
Number | Date | Country | |
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20100310968 A1 | Dec 2010 | US |