H01M8/0215

ALLOY MEMBER
20200136154 · 2020-04-30 ·

The alloy member includes a base member constituted by an alloy material containing chromium, a chromium oxide layer for covering at least a portion of a surface of the base member, a pore that is formed in an interface region of the base member that is located 30 m or less from an interface between the chromium oxide layer and the base member, and an extending portion extending from the pore into the base member. The pore is configured to inhibit separation of the chromium oxide layer from the base member The extending portion contains an oxide of an element whose equilibrium oxygen pressure is lower than that of a major element of the base member.

ELECTRICALLY-CONDUCTIVE MEMBER AND METHOD OF MANUFACTURING THE SAME

An electrically-conductive member having sufficient corrosion resistivity even when the electrically-conductive member is exposed to high potential environment and a method of manufacturing the electrically-conductive member are offered. An electrically-conductive member is obtained by a mist CVD method, by forming a metal oxide film on a base member of a separator, and the electrically-conductive member has an active potential range and a passive potential range in an anode polarization curve that is measured in a sulfuric acid aqueous solution having a sulfuric acid concentration that is 5.010.sup.4 mol/dm.sup.3 at pH3 and having a temperature of 25 C., an anode current density that is 110.sup.7 A/cm.sup.2 or less in the passive potential range, and the passive potential range reaching to an electric potential that is 1V.

Preparation method for bipolar plate for redox flow battery

Disclosed is a method of manufacturing a bipolar plate for a redox flow battery. The method includes (a) mixing epoxy, a curing agent, and a conductive filler to manufacture a mixture, and (b) manufacturing the bipolar plate including a conductive filler composite manufactured by compression-molding the mixture.

Preparation method for bipolar plate for redox flow battery

Disclosed is a method of manufacturing a bipolar plate for a redox flow battery. The method includes (a) mixing epoxy, a curing agent, and a conductive filler to manufacture a mixture, and (b) manufacturing the bipolar plate including a conductive filler composite manufactured by compression-molding the mixture.

Low temperature co-fired ceramic substrate miniature fuel cell and manufacturing therefor

A low temperature co-fired ceramic substrate miniature fuel cell and manufacturing method therefor is disclosed. The method can be used for rapid, flexible and precise fabrication of gas distribution network as well as for a conventional membrane electrode assembly, for providing high power density. The construction results in a light weight assembly offering 5 optimum cavity for robust set-up and planar series configuration as compared to other established methods of fabrication.

Low temperature co-fired ceramic substrate miniature fuel cell and manufacturing therefor

A low temperature co-fired ceramic substrate miniature fuel cell and manufacturing method therefor is disclosed. The method can be used for rapid, flexible and precise fabrication of gas distribution network as well as for a conventional membrane electrode assembly, for providing high power density. The construction results in a light weight assembly offering 5 optimum cavity for robust set-up and planar series configuration as compared to other established methods of fabrication.

FUEL CELL ANODE FLOW FIELD DESIGN CONFIGURATIONS FOR ACHIEVING INCREASED FUEL UTILIZATION
20200099066 · 2020-03-26 ·

An anode of a fuel cell has an anoe current collector defining an inlet configured to receive fuel gas and an outlet configured to output the fuel gas, a barrier that divides an active area of the anode current collector into a first area and a second area, and a flow passage configured to allow a flow of fuel gas from the inlet through the first area and the second area to the outlet. An obstacle is located in the flow passage in an inactive area of the anode current collector and is configured to change a flow direction of the fuel gas in the flow passage from the first area to the second area to achieve intra-cell mixing of the fuel gas.

FUEL CELL ANODE FLOW FIELD DESIGN CONFIGURATIONS FOR ACHIEVING INCREASED FUEL UTILIZATION
20200099066 · 2020-03-26 ·

An anode of a fuel cell has an anoe current collector defining an inlet configured to receive fuel gas and an outlet configured to output the fuel gas, a barrier that divides an active area of the anode current collector into a first area and a second area, and a flow passage configured to allow a flow of fuel gas from the inlet through the first area and the second area to the outlet. An obstacle is located in the flow passage in an inactive area of the anode current collector and is configured to change a flow direction of the fuel gas in the flow passage from the first area to the second area to achieve intra-cell mixing of the fuel gas.

Titanium Material, Separator, Cell, and Polymer Electrolyte Fuel Cell Stack

A titanium material including a base metal made of pure titanium or a titanium alloy and a titanium oxide film formed on the base metal. Peak intensities obtained by thin-film X-ray diffraction analysis performed on an outer layer of the titanium material using an incident angle of 0.3 satisfy (I(104)+I(200))/I(101)0.080.004I(200), where I(104) is the peak intensity resulting from a plane (104) of a Ti.sub.2O.sub.3 phase, I(200) is the peak intensity resulting from a plane (200) of a TiO phase, I(101) is the peak intensity resulting from a plane (101) of an -Ti phase, and 0<I(104), 0I(200), and 0<I(101). The titanium material is inexpensive and has both the electrical conductivity and corrosion resistance.

Titanium Material, Separator, Cell, and Polymer Electrolyte Fuel Cell Stack

A titanium material including a base metal made of pure titanium or a titanium alloy and a titanium oxide film formed on the base metal. Peak intensities obtained by thin-film X-ray diffraction analysis performed on an outer layer of the titanium material using an incident angle of 0.3 satisfy (I(104)+I(200))/I(101)0.080.004I(200), where I(104) is the peak intensity resulting from a plane (104) of a Ti.sub.2O.sub.3 phase, I(200) is the peak intensity resulting from a plane (200) of a TiO phase, I(101) is the peak intensity resulting from a plane (101) of an -Ti phase, and 0<I(104), 0I(200), and 0<I(101). The titanium material is inexpensive and has both the electrical conductivity and corrosion resistance.