In an embodiment according to the invention, a combination of the following means (1) and (2) is proposed. That is, a flattened tubular type fuel cell comprises:
means (1) for optimizing the constitution of an current-collecting electrode thereby making the flow distribution of a fuel or air uniform across the entire cell region, and
means (2) for shunting the flow of the fuel into a flow directing toward the anode of the cell and a flow directly directing toward the downstream of the current-collecting electrode. Further, such a structure is applicable also to a cell of a cylindrical shape.
A current of the cell 5 flows from the anode 2 to the cathode 3 by way of the solid electrolyte 1. Further, it flows from the cathode 3 to the interconnector 4 for taking out the current. Since most of the current of the anode 2 flows in the circumferential direction, the current path is increased. In order to prevent the increased current path from becoming a large resistor factor, the current-collecting electrode 6 serves to increase a cross-sectional area of the current path in an auxiliary manner. Incidentally also in the cathode, a current path in the circumferential direction is present although it is not so larger in the anode 2. An air-feeding hole 7 is formed inside of the cathode 3 to feed air as an oxidizing agent, and thereby air region through which air flows is formed. On the other hand, the fuel flows along an outer circumference of the cell 5 to form a fuel region.
While the description for
In the fuel cell of the present invention, the flow of the fuel in the current-collecting electrode of the flattened tube cell is shunted into a flow toward the cell and a flow directly flowing to the downstream of the fuel (in the direction of exit). In addition, the thickness of the anode electrode is decreased to provide the current-collecting electrode with a role of the anode electrode to thereby increase the power generation amount of the cell.
The solid electrolyte 1 is in a flattened tubular shape with a bottom, and its material is yttrium stabilized zirconia (YSZ). The anode 2 is made of a porous cermet (sintered body of a metal ceramic) comprising nickel and YSZ. The cathode 3 is made of lanthanummanganate. The interconnectors 4 are made of a lanthanum chlomide. The fuel flows through the outside of the cell. The oxidizing agent (air) flows through air feeding holes 7 at three positions inside the cathode.
The current-collecting electrode 6 is filled in a fuel region 8 on the outside of the cell through which the fuel flows. The current-collecting electrode 6 is comprised of an inner current-collecting electrode 9 adjacent to the anode and an outer current-collecting electrode 10 placed outside the inner current-collecting electrode 9.
The outer current-collecting electrode 10 mainly constitutes a flow path for feeding the fuel in the axial direction of the cell. Further, the outer current-collecting electrode 10 also functions as a current path. Accordingly, the conditions required for the outer current-collecting electrode 10 are preferably as follows. That is,
(1) the fuel gas can flow more easily compared with that in the inner current-collecting electrode 9 (with low flow resistance); and
(2) the electro-conductivity is high.
The inner current-collecting electrode 9 mainly has a role of transporting the fuel fed to the outer current-collecting electrode 10 into the anode 2. Further, the inner current-collecting electrode 9 functions also as a current path. Accordingly, the conditions required for the inner current-collecting electrode 9 are preferably as follows. That is,
(1) the fuel gas is fed from the outer current-collecting electrode 10 and
(2) the electro-conductivity is high.
For the inner current-collecting electrode 9 and the outer current-collecting electrode 10, a porous member having through pores, for example, a three-dimensional mesh porous member can be used. The gas flow rate V in the porous member can be represented by the following equation.
V=ε
0
3
D
2
ΔP/{80μ(1−ε0)2}l (1)
in the equation, ε0 represents a porosity, D represents a diameter of strand constituting the porous member, l represents the length of a porous layer, ΔP represents a differential pressure between the upstream and the downstream of the porous layer, and μ represents the viscosity of a flood. Accordingly, the flow rate increases more as the porosity is larger and the strand diameter constituting the porous member is larger assuming that the differential pressure on the porous layer with a length of l is identical. Naturally, the flow resistance increases more as the porosity is smaller and the wire diameter is smaller.
It is preferable that the gas flows more easily in the outer current-collecting electrode 10 compared with the inner current-collecting electrode 9 and it is preferable to flow at a fast flow rate. The outer current-collecting electrode 10 used in this case had a porosity of about 95% and the strand diameter of about 10 μm. On the other hand, for the inner current-collecting electrode 9, those having a porosity of about 90% and a strand diameter of about 10 μm was used. This can make the flow rate in the outer current-collecting electrode 10 higher by about one digit compared with the flow rate in the inner current-collecting electrode 9. Naturally, it is not necessary to provide a difference between the flow rate in the outer current-collecting electrode 10 and the flow rate in the inner current-collecting electrode 9 by so much as described above, and it may suffice that the difference of the flow rate may be at least about from 1.2 to 1.5.
As a material for the inner current-collecting electrode 9 and the outer current-collecting electrode 10, it is preferable that the electroconductivity is high as shown by the required condition (2) above. Then, a nickel material was used both for the inner current-collecting electrode 9 and the outer current-collecting electrode 10. Nickel was used as a three-dimensional mesh porous member. It may also be a stainless steel, nickel-based alloy, etc.
Further, for the outer current-collecting electrode 10 having a main purpose of flowing the gas, a ceramic material may also be used not being restricted to metal materials. Naturally, in a case of using a highly conductive material for the outer current-collecting electrode 10, the current path is enlarged, thereby contributing to the lowering of the internal resistance.
The cell reaction is shown here. At first, a method of reforming a hydrocarbon type fuel to form a reformed gas containing hydrogen is to be described in the case of methane as example of the hydrocarbon type fuel. On the reforming catalyst, methane and steams are reacted (reforming reaction) to generate hydrogen mainly according to the reaction of the following formula (1). As the reforming catalyst, catalysts such as Ni and Ru systems are used generally.
CH4+H2O=CO+3H2 (1)
Simultaneously, CO reacted according to the chemical formula (1) is further converted into hydrogen as a fuel by the reaction with H2O represented by the following formula (2) (CO conversion reaction).
CO+H2O=CO2+H2 (2)
Since the reaction of forming hydrogen from a hydrocarbon type fuel is an endothermic reaction, heat has to be supplied for keeping the reaction and, generally, the reforming catalyst has to be kept at about 600 to 800° C.
The cell reaction (power generating reaction) occurs at the anode 2, which is an exothermic reaction represented by the following formulae (3) and (4):
H2+½O2=H2O (3)
CO+½O2=CO2 (4)
A current in the cell of this embodiment is schematically shown in
In this embodiment, the interconnector 4 is circumferentially divided at two positions and also divided longitudinally at two positions but it may be divided at three or more portions with no problem.
For the mesh size, a coarse mesh of about #30 was used for the outer current-collecting electrode 17 and a fine mesh of about #100 was used for the inner current-collecting electrode 16.
While the embodiment has been described with reference to a cell structure in which the outside of the flattened tube double-sided power generation type cell is provided the anode, the present invention can provide the same effect also in the cell structure in which the outside of the flattened tube double-sided power generation type cell is provided with the cathode.
While the embodiment has been described with reference to the examples in which the tubular shape with a bottom for the fuel cell is adapted for the flattened tube shape, the effect is not impaired at all also in an flattened tube with bottomless.
Further, since the cell shape is not restricted to the flattened tubular shape but the invention is applicable also to a cell of an oval shape in cross section or a cell of a cuboidal, rectangular or cylindrical shape with similar effect, the shape is not restricted to the flattened tubular shape.
In the fuel cell of this embodiment, since substantially the entire region of the flattened tubular cell contributes to the cell reaction and the area of power generation can be increased to increase the amount of power generation and the internal resistance can be decreased, the energy efficiency can be improved. In this case, the cell performance can further be improved by providing the current-collecting electrode not only to the anode but also to the cathode.
Number | Date | Country | Kind |
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2006-185074 | Jul 2006 | JP | national |