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JP6956352B2 - Carbon fiber woven fabric and fuel cell for fuel cell gas diffusion layer - Google Patents
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JP6956352B2 - Carbon fiber woven fabric and fuel cell for fuel cell gas diffusion layer - Google Patents

Carbon fiber woven fabric and fuel cell for fuel cell gas diffusion layer Download PDF

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JP6956352B2
JP6956352B2 JP2017151192A JP2017151192A JP6956352B2 JP 6956352 B2 JP6956352 B2 JP 6956352B2 JP 2017151192 A JP2017151192 A JP 2017151192A JP 2017151192 A JP2017151192 A JP 2017151192A JP 6956352 B2 JP6956352 B2 JP 6956352B2
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carbon fiber
fuel cell
gas diffusion
diffusion layer
woven fabric
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JP2018026347A (en
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一郎 吉野
久司 永井
昌信 熊谷
順 高木
犬山 久夫
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Nachi Fujikoshi Corp
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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Description

本発明は、車両、船舶、航空機等の交通機関に搭載される燃料電池ガス拡散層(シート)用の炭素繊維織物および、その炭素繊維織物を組み込んだ燃料電池セルに関する。 The present invention relates to a carbon fiber woven fabric for a fuel cell gas diffusion layer (sheet) mounted on a transportation system such as a vehicle, a ship, or an aircraft, and a fuel cell in which the carbon fiber woven fabric is incorporated.

従来、環境問題の関心の高さから新たなエネルギー源として燃料電池による発電が注目されており、その中でも家庭用や車両用として主流である固体高分子形燃料電池(以下、「燃料電池」とする)は、高分子膜の両面に電極触媒層が接合された膜電極接合体と、燃料ガス、酸化剤ガスを電極反応域に導くガス拡散層(ガス拡散シート)と、ガス導入・排出溝を持つセパレータやシール材等からなる単位ユニット(以下、「燃料電池セル」とする)が繰り返し積層されており、概略A4版サイズの面積で数百枚の燃料電池セルを積層して組み上げ、これらを両側から板で締め上げる構造である。 Conventionally, fuel cell power generation has been attracting attention as a new energy source due to the high level of interest in environmental issues. Among them, solid polymer fuel cells (hereinafter referred to as "fuel cells"), which are the mainstream for households and vehicles. ) Is a film electrode joint in which electrode catalyst layers are bonded to both sides of the polymer film, a gas diffusion layer (gas diffusion sheet) that guides fuel gas and oxidant gas to the electrode reaction region, and a gas introduction / discharge groove. Unit units (hereinafter referred to as "fuel cell cells") made of separators, sealing materials, etc. are repeatedly laminated, and hundreds of fuel cell cells are laminated and assembled in an area of approximately A4 size. It is a structure that tightens with a plate from both sides.

中でも、燃料電池セルに組み込まれるガス拡散層は、低コストでの大量生産に向けて大いに期待されている炭素繊維が主な原料である。ここで、ガス拡散層とは一般的に1mm以下の薄いシート状に形成された部材である。 Among them, the gas diffusion layer incorporated in the fuel cell is mainly made of carbon fiber, which is highly expected for mass production at low cost. Here, the gas diffusion layer is generally a member formed in the form of a thin sheet of 1 mm or less.

このガス拡散層は、燃料電池セル外部からの水素を含む燃料ガス或いは酸素を含む酸化剤ガスの2つの反応ガスを膜電極接合体の電極触媒層に円滑に供給できる機能を有することが第一である。この他に、ガス拡散層の基本的な機能として、
1)電気エネルギーを効率的に取り出すために十分に低い電気抵抗を有すること、
2)大電流を取り出すための十分なガス透過性および電池で生成する生成水を目詰まり(クロッギング)させることなく排出させる良好な拡散性を有し、大電流を発電可能とすること、
3)積層部材の厚みムラを吸収できるクッション性(弾力性)を有すること、
などが必要となる。
The gas diffusion layer has a function of smoothly supplying two reaction gases, a fuel gas containing hydrogen and an oxidizing agent gas containing oxygen, from the outside of the fuel cell to the electrode catalyst layer of the membrane electrode assembly. Is. In addition to this, as a basic function of the gas diffusion layer,
1) Having a sufficiently low electrical resistance to efficiently extract electrical energy,
2) It has sufficient gas permeability to take out a large current and good diffusivity to discharge the generated water generated by the battery without clogging (clogging), so that a large current can be generated.
3) Having cushioning properties (elasticity) that can absorb uneven thickness of laminated members,
Etc. are required.

そのようなガス拡散層は大部分が紙構造であるため、厚みムラを吸収するクッション性も低く、何よりもエネルギーを消費する工程が多いので、製造コストがかかるという問題があった。したがって、燃料電池システムを普及させるには低い電気抵抗、十分なガス拡散性、適度なクッション性、十分な耐腐食性をもち、省エネ工程かつ低コストであることが決定的に重要であった。 Since most of such a gas diffusion layer has a paper structure, it has a low cushioning property for absorbing uneven thickness, and above all, there are many steps that consume energy, so that there is a problem that manufacturing cost is high. Therefore, in order to popularize the fuel cell system, it is crucial to have low electric resistance, sufficient gas diffusivity, appropriate cushioning property, sufficient corrosion resistance, energy saving process and low cost.

そこで、特許文献1では経糸または緯糸において、炭素繊維糸Aと、炭素繊維糸Aよりも細い炭素繊維糸Bとをそれぞれ複数本を交互に配列することによって、炭素繊維糸Aにより織物の表面に帯状に突出した凸条部が形成されてなり、炭素繊維糸Bにより溝状に陥没した凹条部が形成され、炭素繊維糸Aの太さ、炭素繊維糸Bの太さ、糸の太さ比(Aの太さ)/(Bの太さ)、凸条部の幅Wr、凹条部の幅Wd、並びに厚さ方向の電気抵抗値が所定範囲としていることが説明されている。 Therefore, in Patent Document 1, in the warp or weft, a plurality of carbon fiber threads A and carbon fiber threads B thinner than the carbon fiber threads A are alternately arranged, so that the carbon fiber threads A are used on the surface of the woven fabric. The ridges protruding in a band shape are formed, and the concave ridges recessed in a groove shape are formed by the carbon fiber thread B, and the thickness of the carbon fiber thread A, the thickness of the carbon fiber thread B, and the thickness of the thread are formed. It is explained that the ratio (thickness of A) / (thickness of B), the width Wr of the convex portion, the width Wd of the concave portion, and the electric resistance value in the thickness direction are within a predetermined range.

また、特許文献2ではアノード側電極を構成する第1ガス拡散層およびカソード側電極を構成する第2ガス拡散層は、第1および第2セパレータに設けられている第1および第2流路に対向して第1および第2ガス流路を設けることが説明されている。 Further, in Patent Document 2, the first gas diffusion layer constituting the anode side electrode and the second gas diffusion layer constituting the cathode side electrode are provided in the first and second flow paths provided in the first and second separators. It is described that the first and second gas flow paths are provided so as to face each other.

特開2012−12719号公報Japanese Unexamined Patent Publication No. 2012-12719 特開2000−113899号公報Japanese Unexamined Patent Publication No. 2000-1138999

草刈俊明、外3名「1Dセルを用いた燃料電池のガス拡散層のガス拡散抵抗解析」、学術講演会前刷集(秋季)、公益社団法人自動車技術会、No.111−13、p.1−3、2013年10月発行Toshiaki Kusakari, 3 outsiders "Analysis of Gas Diffusion Resistance of Gas Diffusion Layer of Fuel Cell Using 1D Cell", Pre-printing of Academic Lecture (Autumn), Society of Automotive Engineers of Japan, No. 111-13, p. 1-3, issued in October 2013

しかし、特許文献1に開示されている炭素繊維織物を燃料電池の単セル用の電極として組み込む際、炭素繊維織物の表面と膜電極接合体の平面との間は太い繊維部分との接触はまだしも、細い繊維部分は太い繊維部分と比べそれらの繊維径の差の半分の値で離れている。 However, when the carbon fiber woven fabric disclosed in Patent Document 1 is incorporated as an electrode for a single cell of a fuel cell, the contact between the surface of the carbon fiber woven fabric and the plane of the membrane electrode assembly is still in contact with the thick fiber portion. , The thin fiber portions are separated by half the difference in their fiber diameters compared to the thick fiber portions.

そのため、その部分での接触が相対的に弱く、細い繊維部分の導通が少なく膜電極接合体の触媒部分の発電効率が低下する。同文献の実施例で開示された発電性能も0.6mA/cmの条件で0.65Vしか出力されておらず、決して良好とはいえない。これでは大電力を必要とする移動車両用の燃料電池用途には多量の単セルが必要になる。 Therefore, the contact at that portion is relatively weak, the conduction of the fine fiber portion is small, and the power generation efficiency of the catalyst portion of the membrane electrode assembly is lowered. The power generation performance disclosed in the examples of the same document also outputs only 0.65 V under the condition of 0.6 mA / cm 2 , which cannot be said to be good at all. This requires a large number of single cells for fuel cell applications for mobile vehicles that require large amounts of power.

また、特許文献2に開示されている燃料電池に組み込まれたガス拡散層では、ガス拡散層に用いられる素材(カーボンペーパ或いはポーラス状カーボン)に微細な溝を切り込むという精密加工が必要である。そのため、部材としてのガス拡散層とするのには歩留まり等の問題を含め、製造コストが高くなる。これでは組み込まれる部材の数が大きい移動車両用の燃料電池の実現にむけた低コストでの部材供給の実現は困難となる。 Further, the gas diffusion layer incorporated in the fuel cell disclosed in Patent Document 2 requires precision processing of cutting fine grooves in the material (carbon paper or porous carbon) used for the gas diffusion layer. Therefore, in order to use the gas diffusion layer as a member, the manufacturing cost is high, including problems such as yield. This makes it difficult to supply members at low cost toward the realization of fuel cells for mobile vehicles in which a large number of members are incorporated.

そこで、本発明においては燃料電池内に積層した場合の厚みを小さく(薄く)し、膜電極接合体とセパレータとで挟み込んで積層した時の密着性を高めて電気抵抗を下げることのできるガス拡散層用の炭素繊維織物を提供することを課題とする。 Therefore, in the present invention, the thickness when laminated in the fuel cell is made small (thin), and the gas diffusion which can improve the adhesion when laminated by being sandwiched between the membrane electrode assembly and the separator and reduce the electric resistance. An object of the present invention is to provide a carbon fiber woven fabric for layers.

同時に、ガス拡散層として燃料電池内にて優れたガス拡散性を有し、大電流を発電できる低コストの燃料電池ガス拡散層用の炭素繊維織物を提供することを課題とする。 At the same time, it is an object of the present invention to provide a low-cost carbon fiber fabric for a fuel cell gas diffusion layer, which has excellent gas diffusivity in a fuel cell as a gas diffusion layer and can generate a large current.

前述した課題を解決するために、本発明者は炭素繊維織物に注目して鋭意研究を重ねた結果、それを応用したガス拡散層により燃料電池を構成した場合に、従来に無い優れた性能を発揮する特殊な織り方の炭素繊維織物の存在を知見するに至った。 In order to solve the above-mentioned problems, the present inventor has focused on carbon fiber woven fabrics and conducted intensive studies. We have come to discover the existence of carbon fiber woven fabrics with a special weave.

すなわち、燃料電池ガス拡散層用炭素繊維織物の発明については、経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物において、経糸または緯糸の一方の糸が実質的に無撚糸とする。また、その燃料電池ガス拡散層用炭素繊維織物の片面においては、無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い燃料電池ガス拡散層用炭素繊維織物とした。 That is, with respect to the invention of the carbon fiber woven fabric for the fuel cell gas diffusion layer, in the carbon fiber woven fabric for the fuel cell gas diffusion layer formed by interweaving the warp and the weft, one of the warp and the weft is substantially untwisted. And. Further, on one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer, the number of untwisted yarns above the other yarn interwoven with the untwisted yarn is below the other yarn interwoven with the untwisted yarn. A carbon fiber woven fabric for a fuel cell gas diffusion layer, which is larger than the number of untwisted yarns.

また、経糸および緯糸のいずれもが実質的な無撚糸であっても構わない。すなわち、経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物において、経糸および緯糸が共に実質的に無撚糸であり、燃料電池ガス拡散層用炭素繊維織物の片面において、経糸または緯糸のいずれか一方の糸は、交織されている他方の糸の上になる本数がその他方の糸の下になる本数よりも多い燃料電池ガス拡散層用炭素繊維織物とすることもできる。 Further, both the warp and the weft may be substantially untwisted. That is, in the carbon fiber woven fabric for the fuel cell gas diffusion layer formed by interweaving the warp and the weft, both the warp and the weft are substantially untwisted, and the warp is on one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer. Alternatively, one of the weft yarns may be a carbon fiber woven fabric for a fuel cell gas diffusion layer in which the number of yarns above the other yarn that is interwoven is larger than the number of yarns below the other yarn.

さらに、前述した燃料電池ガス拡散層用炭素繊維織物の片面とは反対側の面に凹条部を形成した燃料電池ガス拡散層用炭素繊維織物でもよい。また、凹条部が形成された反対側の面の剛性を、もう一方の片面側の剛性より高くした燃料電池ガス拡散層用炭素繊維織物でもよい。 Further, the carbon fiber woven fabric for the fuel cell gas diffusion layer having a concave portion formed on the surface opposite to one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer described above may be used. Further, a carbon fiber woven fabric for a fuel cell gas diffusion layer in which the rigidity of the opposite surface on which the concave portion is formed is higher than the rigidity of the other one surface side may be used.

前述の燃料電池ガス拡散層用炭素繊維織物を利用した燃料電池セルの発明については、燃料電池ガス拡散層用炭素繊維織物から成り凹条部を有するガス拡散層と、複数の溝部を有するセパレータと、を備える燃料電池セルであって、ガス拡散層の凹条部を有する面と、セパレータの溝部を有する面とが互いに接触し、かつガス拡散層の凹条部とセパレータの溝部との成す角度θを10°以上35°以下の範囲とする燃料電池セルとした。 Regarding the invention of the fuel cell using the carbon fiber woven fabric for the fuel cell gas diffusion layer described above, the gas diffusion layer made of the carbon fiber woven fabric for the fuel cell gas diffusion layer and having a concave portion, and the separator having a plurality of grooves are used. A fuel cell cell comprising the A fuel cell having θ in the range of 10 ° or more and 35 ° or less was used.

また、燃料電池ガス拡散層用炭素繊維織物から成り凹条部を有するガス拡散層と、平面を有するセパレータと、を備える燃料電池セルであって、ガス拡散層の凹条部を有する面と、セパレータの平面とが互いに接触している燃料電池セルであっても構わない。 Further, a fuel cell cell comprising a gas diffusion layer made of a carbon fiber woven fabric for a fuel cell gas diffusion layer and having a concave portion and a separator having a flat surface, and a surface having the concave portion of the gas diffusion layer. It may be a fuel cell in which the planes of the separator are in contact with each other.

なお、本願発明にて「実質的に無撚糸」とは、織物工程で糸切れが多発するような甘撚紡績糸、さらに糸にならないほど撚数の少ない紡績糸、もしくは撚りのほとんど無い長繊維を言うものとする。 In the present invention, the term "substantially untwisted yarn" refers to a sweet-twisted spun yarn in which yarn breakage occurs frequently in the weaving process, a spun yarn having a small number of twists so as not to become a yarn, or a long fiber having almost no twist. Suppose to say.

本発明では、経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物であって、経糸または緯糸の少なくとも一方の糸が実質的に無撚糸として、燃料電池ガス拡散層用炭素繊維織物の片面において、無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い燃料電池ガス拡散層用炭素繊維織物とした。 In the present invention, a carbon fiber woven fabric for a fuel cell gas diffusion layer formed by interweaving warp threads and weft threads, wherein at least one of the warp threads or the weft threads is substantially untwisted and carbon for the fuel cell gas diffusion layer. On one side of the textile fabric, the number of untwisted yarns above the other yarn interwoven with the untwisted yarn is greater than the number of untwisted yarns below the other yarn interwoven with the untwisted yarn. Carbon fiber woven fabric for use.

無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い面側に膜電極接合体(MEA)の触媒層を接触させることで、織物と膜電極接合体の触媒層との密着性が向上する。膜電極接合体の触媒層ではイオン交換が行われるため、イオン交換と電子の授受が効率良く行われる。 Membrane electrode assembly (MEA) on the surface side where the number of untwisted yarns above the other yarn interwoven with the untwisted yarn is greater than the number of untwisted yarns below the other yarn interwoven with the untwisted yarn By bringing the catalyst layers into contact with each other, the adhesion between the woven fabric and the catalyst layer of the membrane electrode assembly is improved. Since ion exchange is performed in the catalyst layer of the membrane electrode assembly, ion exchange and electron transfer are efficiently performed.

その結果、電気エネルギーを効率的に取り出すために十分に低い電気抵抗が実現できる。同時に、織物の表面の無撚糸が膜電極接合体の触媒層と接触することでより無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い面が扁平化して、ガス拡散層としての作用を維持しながら厚みを減少させることもできる。さらに、織物構造であるため厚み方向の寸法ばらつきを吸収する柔軟性がカーボンペーパに比べて向上する。 As a result, a sufficiently low electrical resistance can be realized to efficiently extract electrical energy. At the same time, the number of untwisted yarns on the other yarn that is interwoven with the untwisted yarn by contacting the untwisted yarn on the surface of the fabric with the catalyst layer of the membrane electrode assembly is the other that is interwoven with the untwisted yarn. It is also possible to flatten the surface under the yarn, which is larger than the number of untwisted yarns, and reduce the thickness while maintaining the action as a gas diffusion layer. Further, since it has a woven structure, the flexibility of absorbing dimensional variations in the thickness direction is improved as compared with carbon paper.

また、燃料電池ガス拡散層用炭素繊維織物の片面(無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い面)とは反対側の面において凹条部を形成すると、この凹条部が形成された面と、溝を有するセパレータの溝面とを接触させることで、より広範囲なガス流路が形成される。 In addition, one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer (the number of untwisted yarns above the other yarn interwoven with the untwisted yarn is below the other yarn interwoven with the untwisted yarn). When a concave portion is formed on a surface opposite to the number of surfaces), the surface on which the concave portion is formed is brought into contact with the groove surface of the separator having a groove, so that a wider gas flow path is formed. Is formed.

その結果、このガス流路を通して、酸化剤ガスを供給・拡散させ、同時に膜電極接合体の触媒層にて生成する水蒸気をガス拡散層内で目詰まりさせることなく速やかに吸い出し、系外に排出できるため、大電流を取り出すことができる。つまり、燃料電池を使用する際の大電流領域では燃料電池セル内が過加湿状態になり、良好なガス拡散抵抗が得られる。 As a result, the oxidant gas is supplied and diffused through this gas flow path, and at the same time, the water vapor generated in the catalyst layer of the membrane electrode assembly is quickly sucked out without clogging in the gas diffusion layer and discharged to the outside of the system. Therefore, a large current can be taken out. That is, in the large current region when the fuel cell is used, the inside of the fuel cell is in an overhumidified state, and good gas diffusion resistance can be obtained.

さらに、その反対面(無撚糸と交織されている他方の糸の上になる無撚糸の本数が無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い面)の剛性よりも高くする。 Further, the rigidity of the opposite surface (the surface in which the number of untwisted yarns above the other yarn interwoven with the untwisted yarn is greater than the number of untwisted yarns below the other yarn interwoven with the untwisted yarn) Also raise.

これにより、ガス拡散層の凹条部を形成する面側に溝を有するセパレータの溝面を接触させた場合に、セパレータの溝内にガス拡散層が入り込むことが軽減される。その結果、ガスの流路が確保されて、酸化剤ガスを供給する或いは生成水等を排水する能力を損なうことがなく、高い発電能力が維持される。 As a result, when the groove surface of the separator having a groove is brought into contact with the surface side forming the concave portion of the gas diffusion layer, the gas diffusion layer is prevented from entering the groove of the separator. As a result, a gas flow path is secured, and a high power generation capacity is maintained without impairing the ability to supply the oxidant gas or drain the generated water or the like.

また、ガス拡散層の凹条部の面とセパレータの平面とを互いに接触させた燃料電池セルとすることで、厚みの薄い燃料電池の単セルを実現可能とし、発電能力が高く、かつ数百枚の単セルを組み合わせた大電力取り出し可能な燃料電池スタックを薄型で軽量かつ低コストで実現できる。 Further, by forming a fuel cell in which the surface of the concave portion of the gas diffusion layer and the flat surface of the separator are in contact with each other, it is possible to realize a single cell of a thin fuel cell, which has a high power generation capacity and several hundreds. A fuel cell stack that can take out a large amount of power by combining a single cell can be realized with a thin weight, light weight, and low cost.

本発明の一実施形態である炭素繊維織物1の織形態を示す模式(斜視)図である。It is a schematic (perspective) figure which shows the weaving form of the carbon fiber woven fabric 1 which is one Embodiment of this invention. 経糸が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物11の織組織図(綾織の場合)である。It is a woven structure diagram (in the case of twill weave) of the carbon fiber woven fabric 11 which shows one Embodiment of this invention when the warp yarn is substantially untwisted yarn. 経糸が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物21の織組織図(朱子織の場合)である。It is a weave structure diagram (in the case of satin weave) of the carbon fiber woven fabric 21 which shows one Embodiment of this invention when the warp yarn is substantially untwisted yarn. 経糸が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物31の織組織図(たてうね織の場合)である。It is a woven structure diagram (in the case of warp ridge weave) of the carbon fiber woven fabric 31 which shows one Embodiment of this invention when the warp yarn is substantially untwisted yarn. 図4に示す炭素繊維織物31のA−A線模式断面図である。FIG. 6 is a schematic cross-sectional view taken along the line AA of the carbon fiber woven fabric 31 shown in FIG. 炭素繊維織物の片面側の剛性を測定する方法を示す模式図である。It is a schematic diagram which shows the method of measuring the rigidity of one side of a carbon fiber woven fabric. 炭素繊維織物の剛性の測定方法において当該織物の片面側への加圧後の状態を示す模式図である。It is a schematic diagram which shows the state after pressurization to one side of the woven fabric in the method of measuring the rigidity of a carbon fiber woven fabric. 本発明の燃料電池セル10の構成を示す模式図である。It is a schematic diagram which shows the structure of the fuel cell 10 of this invention. 図8に示す溝付きセパレータ5のB矢視図である。It is a B arrow view of the grooved separator 5 shown in FIG. 図8に示す炭素繊維織物41のA矢視図である。FIG. 8 is a view taken along the line A of the carbon fiber woven fabric 41 shown in FIG. 炭素繊維織物41の凹条部4と溝付きセパレータ5の溝7とが交差する角度(交差角)θを説明する模式図である。It is a schematic diagram explaining the angle (intersection angle) θ at which the concave portion 4 of the carbon fiber woven fabric 41 and the groove 7 of the grooved separator 5 intersect. 実施例2の通水試験に用いた試験装置の模式平面図である。It is a schematic plan view of the test apparatus used for the water flow test of Example 2. 図12に示す通水試験に用いた試験装置のX−X断面図である。FIG. 12 is a cross-sectional view taken along the line XX of the test apparatus used for the water flow test shown in FIG.

本発明である燃料電池ガス拡散層用炭素繊維織物の実施形態の一例について図面を用いて説明する。図1は、本発明の一実施形態である燃料電池ガス拡散層用炭素繊維織物1(以下、「炭素繊維織物1」とする)の織形態を示す模式(斜視)図である。この炭素繊維織物1は、図1に示すように複数の経糸2(2A〜2J)および緯糸3(3a〜3j)が綾織によって交織された場合のものである。 An example of the embodiment of the carbon fiber woven fabric for the fuel cell gas diffusion layer of the present invention will be described with reference to the drawings. FIG. 1 is a schematic (perspective) view showing a weaving form of a carbon fiber woven fabric 1 for a fuel cell gas diffusion layer (hereinafter referred to as “carbon fiber woven fabric 1”) according to an embodiment of the present invention. As shown in FIG. 1, the carbon fiber woven fabric 1 is a case where a plurality of warp threads 2 (2A to 2J) and weft threads 3 (3a to 3j) are interwoven by twill weaving.

図1に示す炭素繊維織物1は、経糸2が実質的に無撚糸であり、緯糸3が撚りのある糸である場合を示している。撚りのある緯糸3は図1に示すようにその断面が比較的円形に近い形状を呈している。これに対して、実質的に無撚糸である緯糸2はその断面が楕円形状である。 The carbon fiber woven fabric 1 shown in FIG. 1 shows a case where the warp yarn 2 is a substantially untwisted yarn and the weft yarn 3 is a twisted yarn. As shown in FIG. 1, the twisted weft thread 3 has a shape whose cross section is relatively close to a circle. On the other hand, the weft 2 which is substantially untwisted has an elliptical cross section.

次に、炭素繊維織物1を構成する1本の経糸2Aと、それと交織している複数の緯糸3A〜3Jとの関係において、片面(図1の上面)側に着目して説明する。実質的に無撚糸である経糸2Aは、図1に示すようにまず経糸3aの上を飛び越えて、その後の2本の経糸3b、3cの下をくぐっている。次に、経糸2Aは3本の緯糸3d、3e、3fの上を飛び越した後、同様に2本の緯糸3gおよび3hの下をくぐっている。 Next, in the relationship between one warp yarn 2A constituting the carbon fiber woven fabric 1 and a plurality of weft yarns 3A to 3J interwoven with the warp yarn 2A, one side (upper surface in FIG. 1) side will be focused on. As shown in FIG. 1, the warp yarn 2A, which is substantially untwisted yarn, first jumps over the warp yarn 3a and then passes under the two warp yarns 3b and 3c thereafter. Next, the warp 2A jumps over the three wefts 3d, 3e, and 3f, and then passes under the two wefts 3g and 3h in the same manner.

つまり、本発明の炭素繊維織物1が図1に示す交織形態である場合、無撚糸(経糸2)はもう一方の糸(緯糸3)に対して、3本の糸(緯糸)の上を飛び越えて(上になる)、その後2本の糸(緯糸)の下をくぐる(下になる)という規則性を保った状態で交織されている。 That is, when the carbon fiber woven fabric 1 of the present invention has the mixed weaving form shown in FIG. 1, the untwisted yarn (warp yarn 2) jumps over the three yarns (weft yarn) with respect to the other yarn (weft yarn 3). It is woven in a state where it keeps the regularity of passing under (down) two threads (weft) after that (up).

したがって、炭素繊維織物1の片面において、図1に示すように無撚糸である経糸2Aは、経糸2Aと交織されている他方の糸(緯糸3a〜3j)に対して、他方の糸(緯糸)の上になる無撚糸(経糸)の本数がその無撚糸(経糸)と交織されている他方の糸(緯糸)の下になる無撚糸(経糸)の本数より多くなっている。この規則性は、経糸2Bなど他の経糸2B〜2Jについても同様である。 Therefore, on one side of the carbon fiber woven fabric 1, as shown in FIG. 1, the warp yarn 2A, which is a non-twisted yarn, is the other yarn (weft yarn) with respect to the other yarn (weft yarn 3a to 3j) interwoven with the warp yarn 2A. The number of untwisted yarns (warp yarns) on the top is larger than the number of untwisted yarns (warp yarns) below the other yarn (weft yarn) interwoven with the untwisted yarns (warp yarns). This regularity is the same for other warp threads 2B to 2J such as warp threads 2B.

なお、本願発明の炭素繊維織物1を形成している経糸2に着目した場合には緯糸3を飛び越している経糸2の本数、または炭素繊維織物1を形成している緯糸3に着目した場合には経糸2を飛び越している緯糸3の本数をそれぞれ「浮き(の)本数」と呼ぶこともできる。 When focusing on the warp threads 2 forming the carbon fiber woven fabric 1 of the present invention, the number of warp threads 2 jumping over the weft threads 3 or when focusing on the weft threads 3 forming the carbon fiber woven fabric 1. Can also refer to the number of weft threads 3 jumping over the warp threads 2 as the "floating number".

次に、本願発明の炭素繊維織物1の別の実施形態を織形態ごとに説明する。図2は経糸12が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物11の織組織図(綾織の場合)、図3は経糸22が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物21の織組織図(朱子織の場合)、図4は経糸32が実質的に無撚糸である場合の本発明の一実施形態を示す炭素繊維織物31の織組織図(たてうね織の場合)をそれぞれ示す。 Next, another embodiment of the carbon fiber woven fabric 1 of the present invention will be described for each woven form. FIG. 2 is a woven structure diagram (in the case of twill weave) of the carbon fiber woven fabric 11 showing an embodiment of the present invention when the warp 12 is substantially untwisted, and FIG. 3 is a diagram in which the warp 22 is substantially untwisted. The woven structure diagram (in the case of Akiko weave) of the carbon fiber woven fabric 21 showing one embodiment of the present invention, FIG. 4 shows the carbon fiber showing one embodiment of the present invention when the warp 32 is substantially untwisted yarn. The woven structure diagram (in the case of vertical ridge weave) of the woven fabric 31 is shown respectively.

図2に示す織組織は、10本の経糸(12A〜12J)および10本の緯糸(13a〜13j)の計100本の糸を用いて綾織により交織された場合の炭素繊維織物11の織組織である。図2中の黒い部分は経糸12が緯糸13よりも上に織り込まれている(浮いている)箇所を示し、白い部分は緯糸13が経糸12よりも上に織りこまれている(浮いている)箇所を示す。図2に示す織組織(綾織)の場合、本発明の炭素繊維織物11は実質的に無撚りである経糸12が緯糸13に対して上に交織されている本数が60本となることから、緯糸13の下になる経糸12の本数(40本)よりも多いことになる。 The weaving structure shown in FIG. 2 is the weaving structure of the carbon fiber woven fabric 11 when twill weaving is performed using a total of 100 threads of 10 warp threads (12A to 12J) and 10 weft threads (13a to 13j). Is. The black part in FIG. 2 shows the part where the warp thread 12 is woven (floating) above the weft thread 13, and the white part shows the part where the weft thread 13 is woven (floating) above the warp thread 12. ) Indicates the location. In the case of the woven structure (twill weave) shown in FIG. 2, the carbon fiber woven fabric 11 of the present invention has 60 warp threads 12 interwoven with respect to the weft threads 13, which are substantially untwisted. This is more than the number of warp threads 12 (40 threads) under the weft threads 13.

図3に示す織組織は、図2の織組織と同様に10本の経糸(22A〜22J)および10本の緯糸(23a〜23j)の計100本の糸を用いて朱子織により交織された場合の炭素繊維織物21の織組織である。図3中の黒い部分は図2の場合と同様に経糸22が緯糸23よりも上に織り込まれている(浮いている)箇所を示し、白い部分は緯糸23が経糸22よりも上に織りこまれている(浮いている)箇所を示す。図3に示す織組織の場合、本発明の炭素繊維織物21は実質的に無撚りである経糸22が緯糸23に対して上に交織されている本数が80本となることから、緯糸23の下になる経糸22の本数(20本)よりも多いことになる。 The weaving structure shown in FIG. 3 was interwoven by satin weaving using a total of 100 threads of 10 warp threads (22A to 22J) and 10 weft threads (23a to 23j), similarly to the weaving structure of FIG. This is the woven structure of the carbon fiber woven fabric 21 of the case. The black part in FIG. 3 shows the part where the warp 22 is woven (floating) above the weft 23 as in the case of FIG. 2, and the white part shows the weft 23 woven above the weft 22. Indicates a part that is rare (floating). In the case of the weaving structure shown in FIG. 3, the carbon fiber woven fabric 21 of the present invention has 80 warp threads 22 interwoven with respect to the weft threads 23, which are substantially untwisted. This is more than the number of warp threads 22 (20) below.

図4に示す織組織は、16本の経糸(32A〜32P)および15本の緯糸(33a〜33o)の計240本の糸を用いて、たてうね織により交織された場合の炭素繊維織物31の織組織である。図4中の黒い部分は図2、3の場合と同様に経糸32が緯糸33よりも上に織り込まれている(浮いている)箇所を示し、白い部分は緯糸33が経糸32よりも上に織りこまれている(浮いている)箇所を示す。図4に示す織組織の場合、本発明の炭素繊維織物31は実質的に無撚りである経糸32が緯糸33に対して上に交織されている本数が168本となることから、緯糸33の下になる経糸32の本数(72本)よりも多いことになる。 The woven structure shown in FIG. 4 is a carbon fiber when woven by warp ridge weaving using a total of 240 threads of 16 warp threads (32A to 32P) and 15 weft threads (33a to 33o). It is a woven structure of the woven fabric 31. The black part in FIG. 4 shows the part where the warp 32 is woven (floating) above the weft 33 as in the cases of FIGS. 2 and 3, and the white part shows the weft 33 above the warp 32. Indicates the woven (floating) part. In the case of the weaving structure shown in FIG. 4, the carbon fiber woven fabric 31 of the present invention has 168 warp threads 32 interwoven with respect to the weft threads 33, which are substantially untwisted. This is more than the number of warp threads 32 (72) below.

以上より、燃料電池ガス拡散層用炭素繊維織物を形成する経糸または緯糸の一方が実質的に無撚糸である場合について説明したが、本発明の燃料電池ガス拡散層用炭素繊維織物は経糸および緯糸のいずれもが実質的な無撚糸であって構わない。すなわち、経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物において、経糸および緯糸が共に実質的に無撚糸であり、燃料電池ガス拡散層用炭素繊維織物の片面において、経糸または緯糸のいずれか一方の糸が交織されている他方の糸の上になる無撚糸の本数がその無撚糸と交織されている他方の糸の下になる本数より多くすることもできる。 From the above, the case where one of the warp or weft that forms the carbon fiber fabric for the fuel cell gas diffusion layer is substantially untwisted has been described, but the carbon fiber fabric for the fuel cell gas diffusion layer of the present invention is the warp and the weft. Any of these may be substantially untwisted yarns. That is, in the carbon fiber woven fabric for the fuel cell gas diffusion layer formed by interweaving the warp and the weft, both the warp and the weft are substantially untwisted, and the warp is on one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer. Alternatively, the number of untwisted yarns above the other yarn in which one of the weft yarns is interwoven may be larger than the number of untwisted yarns below the other yarn interwoven with the untwisted yarn.

なお、本発明の燃料電池ガス拡散層用炭素繊維織物の織り方は、前述の綾織や朱子織などの他に平二重織で溝パターンが縦溝、横溝、ジグザグ(階段状)溝、斜め溝等の空間的に連続した溝が形成される織物でもよい。 The weaving method of the carbon fiber woven fabric for the fuel cell gas diffusion layer of the present invention is a flat double weave in addition to the above-mentioned twill weave and satin weave, and the groove pattern is a vertical groove, a horizontal groove, a zigzag (stepped) groove, and an oblique weave. It may be a woven fabric in which spatially continuous grooves such as grooves are formed.

また、織り上がった織物の片面には前述の実質的に無撚りの糸束が表面に現れ、各糸束の断面が扁平になり膜電極接合体の触媒面との接触面積を増やすように広がり平滑に当てることができる形態が望ましい。 Further, the above-mentioned substantially untwisted yarn bundle appears on one side of the woven fabric, and the cross section of each yarn bundle becomes flat and spreads so as to increase the contact area with the catalyst surface of the membrane electrode assembly. A form that can be applied smoothly is desirable.

さらに、綾織では経緯比(経糸と緯糸との割合)が2:3もしくは3:4が望ましく、朱子織なら3、4、5本の朱子織が良い。また、平二重織においては、緯糸を例えばメートル番手表示で1/20Nmと1/100Nmのように太糸と細糸を交互に打ち込めば焼成収縮時に経糸の均等ピッチが図5のようにずれて経糸方向に溝を形成する織物(いわゆる縦畝織物)とすることもできる。 Further, in the case of twill weave, the warp / weft ratio (ratio of warp to weft) is preferably 2: 3 or 3: 4, and in the case of satin weave, 3, 4 or 5 satin weaves are preferable. Further, in the plain double weave, if the weft yarns are alternately driven with thick yarns and fine yarns such as 1/20 Nm and 1/100 Nm in metric count display, the uniform pitch of the warp yarns shifts as shown in FIG. It can also be a woven fabric (so-called warp ridged woven fabric) that forms grooves in the warp yarn direction.

次に、炭素繊維織物に設けられる凹条部の構造について図5を用いて説明する。図5は、図4に示すたてうね織により交織された炭素繊維織物31のA−A切断線における模式断面図である。図5に示す炭素繊維織物31は図4の場合と同様に経糸32が無撚糸であるので、経糸32はA−A断面方向から見ると図5に示すように比較的に扁平形状を呈している。また、緯糸33も経糸32と同様には無撚りの糸であることから図1に示す炭素繊維織物1の場合と同様にその断面形状はほぼ楕円形状である。 Next, the structure of the concave portion provided on the carbon fiber woven fabric will be described with reference to FIG. FIG. 5 is a schematic cross-sectional view taken along the AA cutting line of the carbon fiber woven fabric 31 interwoven by the warp ridge weave shown in FIG. In the carbon fiber woven fabric 31 shown in FIG. 5, since the warp 32 is a non-twisted yarn as in the case of FIG. 4, the warp 32 has a relatively flat shape as shown in FIG. 5 when viewed from the AA cross-sectional direction. There is. Further, since the weft 33 is also a non-twisted yarn like the warp 32, its cross-sectional shape is substantially elliptical as in the case of the carbon fiber woven fabric 1 shown in FIG.

そして、炭素繊維織物31は太さが数倍以上差のある緯糸が交互に打ち込まれており、太くて実質的に無撚の緯糸は一本の経糸の上になるが7本の経糸の下になる7/1の朱子織とし、また細くて実質的に無撚の緯糸は経糸と平織となる、いわゆる2重織とする。 Then, in the carbon fiber woven fabric 31, wefts having a thickness difference of several times or more are alternately driven, and the thick and substantially untwisted weft is above one warp but below seven warps. It is a 7/1 satin weave, and the thin and substantially untwisted weft is a warp and a plain weave, so-called double weave.

その結果、炭素繊維織物31は図5に示す下面側が膜電極接合体の触媒部分側に当接するのに適当な平滑面を得る。次に、セパレータに当接する一方の面(図5の上面)について述べる。生機(きばた)では残っていた消失繊維は焼成収縮時には消失させてすき間ができており、収縮時に動かされやすい経糸が糸寄りして、等間隔で無くなる。 As a result, the carbon fiber woven fabric 31 obtains a smooth surface suitable for the lower surface side shown in FIG. 5 to abut on the catalyst portion side of the membrane electrode assembly. Next, one surface (upper surface in FIG. 5) that comes into contact with the separator will be described. The lost fibers remaining in the raw machine (Kibata) are lost during firing shrinkage to form a gap, and the warp threads that are easily moved during shrinkage are brought closer to each other and disappear at regular intervals.

そのために経糸32Fと経糸32Hおよび経糸32Hと経糸32Jの経糸同士の間隔が他の間隔より広くなり、経糸方向に都合のよい凹条部4(二点鎖線で示す包絡線部分)が形成される炭素繊維織物31を得る。ここでさらに重要なことは、経糸(太糸)33g等が膜電極接合体の触媒部分側に多く存在するため、断面方向にスライスした時の単位厚み当たりの空隙率は膜電極接合体の触媒部分側よりセパレータ側のほうが大きく、膜電極接合体の触媒部分側で発生する水蒸気は結露せずにセパレータ側に排出させやすい形態となる。 Therefore, the distance between the warp threads 32F and the warp thread 32H and the warp threads 32H and the warp threads 32J becomes wider than the other intervals, and the concave portion 4 (envelope portion indicated by the alternate long and short dash line) is formed, which is convenient in the warp thread direction. A carbon fiber woven fabric 31 is obtained. More importantly, since a large amount of warp (thick thread) 33 g or the like is present on the catalyst portion side of the membrane electrode assembly, the void ratio per unit thickness when sliced in the cross-sectional direction is the catalyst of the membrane electrode assembly. The separator side is larger than the partial side, and the water vapor generated on the catalyst partial side of the membrane electrode assembly is easily discharged to the separator side without dew condensation.

次に、本発明の炭素繊維織物の剛性について説明する。まず、炭素繊維織物の片面もしくは両面側に硬化樹脂を塗布し、乾燥させることで、その樹脂が塗布された面側の剛性を当該樹脂を塗布する前に比べて高めることができる。 Next, the rigidity of the carbon fiber woven fabric of the present invention will be described. First, by applying the cured resin to one side or both sides of the carbon fiber woven fabric and drying it, the rigidity of the side to which the resin is applied can be increased as compared with before the resin is applied.

具体的には、例えば炭素繊維織物の片面もしくは両面側にレゾール型の熱硬化性樹脂を分散させた液を塗布して、乾燥させた後、不活性ガス雰囲気内にて平滑板で圧縮し、加熱・冷却することにより、ガスの供給および透過性、ガスの拡散性を維持しながら樹脂を硬化させる。この際、炭化処理時と同じ要領で加圧し、不活性ガス中で樹脂が低抵抗になる600℃〜1250℃の温度範囲で焼成する。 Specifically, for example, a liquid in which a resole-type thermosetting resin is dispersed is applied to one or both sides of a carbon fiber woven fabric, dried, and then compressed with a smooth plate in an inert gas atmosphere. By heating and cooling, the resin is cured while maintaining the gas supply, permeability, and gas diffusivity. At this time, the pressure is applied in the same manner as in the carbonization treatment, and the resin is fired in a temperature range of 600 ° C. to 1250 ° C. in which the resin has low resistance in an inert gas.

レゾール型の熱硬化性樹脂としては水フェノールが好ましく、蒸留水に導電性カーボンブラックやグラファイトを均一に分散させた水フェノールのインキもしくはペーストを利用することができる。また、塗布方法としてはグラビア印刷方式、ドクターブレード法およびスプレー噴霧方式でもよく、また口金幅が均一のダイによる直接塗布法でもよい。 Water phenol is preferable as the resol type thermosetting resin, and water phenol ink or paste in which conductive carbon black or graphite is uniformly dispersed in distilled water can be used. Further, the coating method may be a gravure printing method, a doctor blade method, a spray spraying method, or a direct coating method using a die having a uniform mouthpiece width.

いずれの方法でも樹脂を塗布する前の炭素繊維織物の重量に対して、分散液を塗布して加熱硬化させた後の炭素繊維の増加重量が5〜50%の範囲が望ましい。なお、炭素繊維織物の片面側に塗布する硬化樹脂としては、PVA(ポリビニルアルコール)、SBR(スチレン・ブタジエンゴム)、PVDF(ポリフッ化ビニリデン)、PTFE(ポリテトラフルオロエチレン)などの硬化樹脂の中から必要な剛性に応じて適宜選択できる。 In either method, it is desirable that the increased weight of the carbon fibers after the dispersion is applied and heat-cured is in the range of 5 to 50% with respect to the weight of the carbon fiber woven fabric before the resin is applied. The cured resin to be applied to one side of the carbon fiber woven fabric is among cured resins such as PVA (polyvinyl alcohol), SBR (styrene / butadiene rubber), PVDF (polyvinylidene fluoride), and PTFE (polytetrafluoroethylene). Can be appropriately selected according to the required rigidity.

以上の方法により樹脂を塗布、硬化させた炭素繊維織物の剛性の測定方法について、図6および図7を用いて説明する。図6は炭素繊維織物の片面側の剛性を測定する方法を示す模式図、図7は炭素繊維織物の剛性の測定方法において織物の片面側への加圧後の状態を示す模式図である。 A method for measuring the rigidity of the carbon fiber woven fabric to which the resin is applied and cured by the above method will be described with reference to FIGS. 6 and 7. FIG. 6 is a schematic view showing a method of measuring the rigidity of one side of the carbon fiber woven fabric, and FIG. 7 is a schematic view showing a state after pressurization of the woven fabric to one side in the method of measuring the rigidity of the carbon fiber woven fabric.

本願発明の炭素繊維織物の剛性を測定する方法については、図6に示すように平坦状ブロック上に炭素繊維織物を置いて、炭素繊維織物の上方よりコの字型の治具(溝付きブロック:溝幅w)を所定の圧力Pで加圧することにより行う。コの字型の治具で押圧された炭素繊維織物は、図7に示すように当該治具のコの字の空隙部分(溝部分)にいくらかの浮き上がりを見せる。この炭素繊維織物の浮き上がり量(溝内への侵入量)δを測定することで、炭素繊維織物の剛性の度合いを測定する。 Regarding the method of measuring the rigidity of the carbon fiber woven fabric of the present invention, as shown in FIG. 6, the carbon fiber woven fabric is placed on a flat block, and a U-shaped jig (grooved block) is placed above the carbon fiber woven fabric. : Groove width w) is pressurized with a predetermined pressure P. The carbon fiber woven fabric pressed by the U-shaped jig shows some floating in the U-shaped gap portion (groove portion) of the jig as shown in FIG. The degree of rigidity of the carbon fiber woven fabric is measured by measuring the amount of floating (the amount of penetration into the groove) δ of the carbon fiber woven fabric.

次に、前述した炭素繊維織物41と溝付きセパレータ5から構成させる燃料電池セル10の発明に関する実施の形態について、図8〜図11を用いて説明する。図8は本発明の燃料電池セル10の構成を示す模式図、図9は図8に示す溝付きセパレータ5のB矢視図、図10は図8に示す炭素繊維織物41のA矢視図、図11は炭素繊維織物41の凹条部4と溝付きセパレータ5の溝7とが交差する角度(交差角)θを説明する模式図である。なお、図8において炭素繊維織物41と膜電極接合体8の間に存在する高分子膜や触媒層などの他の構成要素の図示は省略した。 Next, an embodiment of the invention of the fuel cell 10 composed of the carbon fiber woven fabric 41 and the grooved separator 5 described above will be described with reference to FIGS. 8 to 11. 8 is a schematic view showing the configuration of the fuel cell 10 of the present invention, FIG. 9 is a view taken along the line B of the grooved separator 5 shown in FIG. 8, and FIG. 10 is a view taken along the line A of the carbon fiber woven fabric 41 shown in FIG. FIG. 11 is a schematic view illustrating an angle (intersection angle) θ at which the concave portion 4 of the carbon fiber woven fabric 41 and the groove 7 of the grooved separator 5 intersect. In FIG. 8, other components such as a polymer film and a catalyst layer existing between the carbon fiber woven fabric 41 and the membrane electrode assembly 8 are not shown.

本発明の燃料電池セル10は、図8に示すように前述した炭素繊維織物41と、炭素繊維織物41の凹条部4を有する面側と接触している溝付きセパレータ5と、炭素繊維織物41の凹条部4を有する面側とは反対側の面側で接触している膜電極接合体8と、から構成される。溝付きセパレータ5の溝7は、図9に示すように縦方向に複数条設けられている。これに対して、炭素繊維織物41の凹条部4は斜め方向に複数条設けられている。 As shown in FIG. 8, the fuel cell 10 of the present invention includes the carbon fiber woven fabric 41 described above, a grooved separator 5 in contact with the surface side of the carbon fiber woven fabric 41 having the concave portion 4, and the carbon fiber woven fabric. It is composed of a membrane electrode assembly 8 that is in contact with the surface side opposite to the surface side having the concave portion 4 of 41. As shown in FIG. 9, a plurality of grooves 7 of the grooved separator 5 are provided in the vertical direction. On the other hand, a plurality of recessed portions 4 of the carbon fiber woven fabric 41 are provided in an oblique direction.

そのため、炭素繊維織物41と溝付きセパレータ5とを燃料電池セル10としてこれらの部材を重ね合わせた際には、図11に示すように炭素繊維織物41の凹条部4は溝付きセパレータ5の溝7に対して、角度θを以って構成されている。言い換えると、凹条部4と溝7との成す角度(交差角)θを以って、炭素繊維織物41と溝付きセパレータ5とが接触していることで燃料電池セル10を構成している。この角度θは、燃料電池セル10の特性の一つであるガス拡散抵抗値を向上させる観点から、10°以上35°以下であることが望ましい。 Therefore, when the carbon fiber woven fabric 41 and the grooved separator 5 are used as the fuel cell 10 and these members are overlapped with each other, the concave portion 4 of the carbon fiber woven fabric 41 is the grooved separator 5 as shown in FIG. It is configured with an angle θ with respect to the groove 7. In other words, the fuel cell 10 is formed by contacting the carbon fiber woven fabric 41 and the grooved separator 5 with an angle (intersection angle) θ formed by the concave portion 4 and the groove 7. .. This angle θ is preferably 10 ° or more and 35 ° or less from the viewpoint of improving the gas diffusion resistance value, which is one of the characteristics of the fuel cell 10.

本発明材および比較材の各GDLを用いて燃料電池セル(以下、「セル)という)を作製し、そのセルの発電性能を測定したので、その測定結果について説明する。本測定に使用したGDLは、2種類の本発明材(本発明材1および2)および2種類の比較材(比較材1および2)とした。本発明材1は、図1および図2に示す綾織(1本の経糸が3本の緯糸を乗り越えた後で2本の緯糸の下をくぐる織り方)のGDLであり、経糸のみが実質的に無撚りであるものとした。また、本発明材2は、発明材1と同様に図1および図2に示す綾織のGDLであり、経糸および緯糸が共に実質的に無撚りであるものとした。 A fuel cell (hereinafter referred to as "cell") was produced using each GDL of the material of the present invention and the comparative material, and the power generation performance of the cell was measured. The measurement result will be described. The GDL used for this measurement will be described. 2 types of the present invention materials (the present invention materials 1 and 2) and 2 types of the comparative materials (comparative materials 1 and 2). It is a GDL (a weaving method in which the warp threads pass under the two weft threads after passing over the three weft threads), and only the warp threads are substantially untwisted. Further, the material 2 of the present invention is the invention. Similar to the material 1, the twill weave GDL shown in FIGS. 1 and 2 is used, and both the warp and the weft are assumed to be substantially untwisted.

これに対して、比較材1は本発明材1と同一の糸で同一ピッチの平織り(1本の経糸が1本の緯糸を乗り越えた後で1本の緯糸の下をくぐる織り方)のGDLであり、経糸のみが実質的に無撚りであるものとした。比較材2は本発明材2と同一の糸で同一ピッチの平織りのGDLであり、経糸および緯糸が共に実質的に無撚りであるものとした。本測定で用いた各GDL(本発明材および比較材)の特徴を表1に示す。 On the other hand, the comparative material 1 is a GDL of the same yarn as the material 1 of the present invention and a plain weave with the same pitch (a weaving method in which one warp goes over one weft and then passes under one weft). Therefore, it was assumed that only the warp threads were substantially untwisted. The comparative material 2 is a plain weave GDL having the same yarn as the material 2 of the present invention and having the same pitch, and both the warp and the weft are substantially untwisted. Table 1 shows the characteristics of each GDL (material of the present invention and comparative material) used in this measurement.

Figure 0006956352
Figure 0006956352

次に、本測定において使用したセルの構造について説明する。本測定に使用したセルは、高分子膜(電解質膜:厚さ20μm)を中央に配置して、アノードおよびカソードの両側に触媒層(密度0.6mg/cm)を密着させた上でGDLを配置した後、各GDLに隣接する形態で最も外側にセパレータ(ストレート溝付)を取り付けた構造とした。 Next, the structure of the cell used in this measurement will be described. In the cell used for this measurement, a polymer membrane (electrolyte membrane: thickness 20 μm) is placed in the center, and catalyst layers (density 0.6 mg / cm 2 ) are brought into close contact with both sides of the anode and cathode, and then GDL. Was arranged, and then a separator (with a straight groove) was attached to the outermost side in a form adjacent to each GDL.

このセルに使用したGDLは、水素極(アノード側)にはSGL社のGDL(品番:SGL24BC)として、空気極(カソード側)には上述の本発明材または比較材(電極面積はいずれも1cm)の各GDLとした。なお、本測定のセルに組み込んだ各GDLの厚みは、100〜150μmの範囲に統一した。 The GDL used in this cell is SGL's GDL (product number: SGL24BC) for the hydrogen electrode (anode side), and the above-mentioned material of the present invention or comparative material (electrode area is 1 cm for each) for the air electrode (cathode side). It was set as each GDL of 2). The thickness of each GDL incorporated in the cell of this measurement was unified in the range of 100 to 150 μm.

上述のセルに対して、水素極には純水素、空気極には窒素で希釈した空気を毎分1Lの流量をそれぞれ圧送して、同時に水素極および空気極の両極ともにガス加湿温度55℃のガスを、発電部の温度が45℃のセルに供給して過加湿条件になるようにセルの運転条件を設定した。また、このセルにおける両極の平均背圧を0.15MPa(abs)とした。上述の条件でセルのIV(電流−電圧)特性を計測して、電圧が0.2Vの時の電流値を限界電流値として、数式1よりガス拡散抵抗値(GDR)を算出した。 To the above cell, pure hydrogen was pumped to the hydrogen electrode and air diluted with nitrogen was pumped to the air electrode at a flow rate of 1 L / min, and at the same time, both the hydrogen electrode and the air electrode had a gas humidification temperature of 55 ° C. The operating conditions of the cell were set so that the gas was supplied to the cell where the temperature of the power generation unit was 45 ° C. and the conditions were over-humidified. The average back pressure of both poles in this cell was 0.15 MPa (abs). The IV (current-voltage) characteristic of the cell was measured under the above conditions, and the gas diffusion resistance value (GDR) was calculated from Equation 1 with the current value when the voltage was 0.2 V as the limit current value.

なお、この数式1は先行文献(特開2010−027510号公報)の明細書中において開示されているものと同じ算出式とした。また、下式において、F:ファラデー定数、R:ガス定数、Pav:出入り口の平均絶対圧力をそれぞれ示す。 In addition, this formula 1 was the same calculation formula as that disclosed in the specification of the prior art (Japanese Patent Laid-Open No. 2010-027510). Further, in the following equation, F: Faraday constant, R: gas constant, and Pav: average absolute pressure at the entrance and exit are shown.

Figure 0006956352
Figure 0006956352

上述の各セルに共通のならし運転を十分に行った後、0.2Vの限界電流値(Ilim:A/cm)を求めて、過加湿におけるガス拡散抵抗値(s/m)を算出した。その結果、本発明材1を用いたセルのガス拡散抵抗値(GDR)は64s/m、本発明材2を用いたセルのガス拡散抵抗値は68s/mであり、本発明材を用いたセルのガス拡散抵抗値はいずれも70s/mを下回る値であった。 After sufficiently performing the break-in operation common to each of the above cells, the limit current value ( Ilim : A / cm 2 ) of 0.2 V is obtained, and the gas diffusion resistance value (s / m) in overhumidification is determined. Calculated. As a result, the gas diffusion resistance value (GDR) of the cell using the material 1 of the present invention was 64 s / m, and the gas diffusion resistance value of the cell using the material 2 of the present invention was 68 s / m, and the material of the present invention was used. The gas diffusion resistance values of the cells were all lower than 70 s / m.

なお、ここで「ならし運転」とは、発電パターン(VI条件やその時間)を変えながら、高分子膜、触媒層、GDLの間の馴染みを良くしながら、発電能力を定常状態に向上させて、性能評価を行う前段階のセルの試運転行為をいうものとする。 Here, "break-in operation" means improving the power generation capacity to a steady state while changing the power generation pattern (VI conditions and its time) and improving the familiarity between the polymer membrane, the catalyst layer, and the GDL. Therefore, it refers to the test run of the cell before the performance evaluation.

これに対して、比較材1を用いたセルのガス拡散抵抗値は107s/m、比較材2を用いたセルのガス拡散抵抗値は109s/mであり、比較材を用いたセルのガス拡散抵抗値はいずれも100s/mを超える値であった。 On the other hand, the gas diffusion resistance value of the cell using the comparative material 1 is 107 s / m, and the gas diffusion resistance value of the cell using the comparative material 2 is 109 s / m. The resistance values were all values exceeding 100 s / m.

以上の測定結果より、経糸または緯糸の一方の糸または両方の糸が実質的に無撚糸であり、燃料電池ガス拡散層用炭素繊維織物の片面において、無撚糸と交織されている他方の糸の上になる無撚糸の本数がその無撚糸と交織されている他方の糸の下になる無撚糸の本数より多い燃料電池ガス拡散層用炭素繊維織物(GDL)とすることで、前述した片面側とは反対側の面に凹条溝が形成される。 From the above measurement results, one or both of the warp and weft yarns are substantially untwisted yarns, and one side of the carbon fiber woven fabric for the fuel cell gas diffusion layer is the other yarns interwoven with the untwisted yarns. By using a carbon fiber fabric (GDL) for a fuel cell gas diffusion layer in which the number of untwisted yarns on the top is larger than the number of untwisted yarns under the other yarn interwoven with the untwisted yarn, the one-sided side described above is used. A concave groove is formed on the surface opposite to the above.

その結果、その反対側の面にセパレータを接触させることで、セル内(高分子膜や触媒層)で発生した水蒸気がGDLの凹条溝を通ってセルの外部へ速やかに排出されるので、水素ガスや空気中の酸素をより多くセル中に取り込むことができて、燃料電池のガス拡散性能を向上することができた。 As a result, by bringing the separator into contact with the surface on the opposite side, the water vapor generated in the cell (polymer membrane or catalyst layer) is quickly discharged to the outside of the cell through the concave groove of the GDL. More hydrogen gas and oxygen in the air could be taken into the cell, and the gas diffusion performance of the fuel cell could be improved.

次に、本発明材および比較材の各GDLにおける流体(水)の流れやすさを比較するために通水試験を行った。本試験に用いたGDLは実施例1で用いた本発明材2および比較材2とした(以下、本発明材3、比較材3という)。本試験において使用した試験装置の模式平面図を図12に、図12のX−X断面図を図13に示す。 Next, a water flow test was conducted to compare the flowability of the fluid (water) in each GDL of the material of the present invention and the comparative material. The GDL used in this test was the material 2 of the present invention and the comparative material 2 used in Example 1 (hereinafter, referred to as the material 3 of the present invention and the comparative material 3). A schematic plan view of the test apparatus used in this test is shown in FIG. 12, and a cross-sectional view taken along the line XX of FIG. 12 is shown in FIG.

本試験装置は、図12および図13に示すように鋼製の台座上に厚さ0.1mm×幅50mm×長さ100mmの大きさのGDLおよびその周囲にパッキンを設置した状態で上方から透明の樹脂プレートと鋼製の押さえ板でGDLを密閉する。密閉されたGDLは、図13に示すように中央部が開口された押さえ板と透明の樹脂プレートを通して、GDLの通水状況を確認できる。その後、本装置のパイプ(図面左側)から水圧0.3MPaの水道水を供給して、反対側のパイプ(図面右側)から排出される単位時間当たりの流量を測定し、水の流れ易さを比較した。 As shown in FIGS. 12 and 13, this test apparatus is transparent from above with a GDL having a thickness of 0.1 mm, a width of 50 mm, and a length of 100 mm and a packing installed around the GDL on a steel pedestal. Seal the GDL with a resin plate and a steel holding plate. As shown in FIG. 13, the sealed GDL can confirm the water flow status of the GDL through a holding plate having an open central portion and a transparent resin plate. After that, tap water with a water pressure of 0.3 MPa is supplied from the pipe of this device (left side of the drawing), and the flow rate per unit time discharged from the pipe on the opposite side (right side of the drawing) is measured to determine the ease of water flow. Compared.

水道水の流量を測定した結果、本発明材3を用いた試験装置の通水量は1分間当たり38ccであった。これに対して、比較材3を用いた試験装置の通水量は1分間当たり22ccであった。以上の測定結果より、本発明材は比較材よりも流体を通し易い構造であることがわかった。そのため、本発明のGDLはセル中でセパレータ(溝の有無に関わらず)と接触した状態であっても、セル内で発生する水蒸気をセル外へ速やかに排出できる。 As a result of measuring the flow rate of tap water, the water flow rate of the test apparatus using the material 3 of the present invention was 38 cc per minute. On the other hand, the water flow rate of the test device using the comparative material 3 was 22 cc per minute. From the above measurement results, it was found that the material of the present invention has a structure that allows more fluid to pass through than the comparative material. Therefore, the GDL of the present invention can quickly discharge the water vapor generated in the cell to the outside of the cell even when it is in contact with the separator (whether or not there is a groove) in the cell.

発明材および比較材を用いて所定の押圧下におけるたわみ量の違いを測定したので、その測定結果について説明する。また、同じ発明材および比較材を用いて実施例1と同様の発電性能の測定も行ったので、その測定結果についても合わせて説明する。 Since the difference in the amount of deflection under a predetermined pressure was measured using the invention material and the comparative material, the measurement results will be described. In addition, since the same power generation performance as in Example 1 was measured using the same invention material and comparative material, the measurement results will also be described.

本実施例のGDLのたわみ量測定および発電性能測定に用いたGDLは、発明材として実施例1で使用した本発明材1の両面に硬化処理を施したもの(以下、本発明材4とする)および比較材として実施例1で使用した比較材1の両面に熱硬化性樹脂で硬化処理を施したもの(以下、比較材4とする)の2種類とした。 The GDL used for measuring the amount of deflection and the power generation performance of the GDL of this example is obtained by subjecting both sides of the material 1 of the present invention used in Example 1 as an invention material to a curing treatment (hereinafter referred to as the material 4 of the present invention). ) And as the comparative material, both sides of the comparative material 1 used in Example 1 were cured with a thermosetting resin (hereinafter referred to as the comparative material 4).

本発明材4および比較材4の両面に施した硬化処理については、実施例1で用いた本発明材1および比較材1をレゾール型フェノール水溶液(重量比率で水:レゾール型フェノール樹脂=100:25の割合で混合したもの)に浸漬し、乾燥、200℃の雰囲気下で熱硬化させた後、さらにPTFE溶液(重量比率で水:PTFE=100:3の割合で混合したもの)を浸漬して乾燥、340℃の雰囲気下で熱処理させたものを本発明材4および比較材4とした。 Regarding the curing treatment applied to both surfaces of the material 4 of the present invention and the comparative material 4, the material 1 of the present invention and the comparative material 1 used in Example 1 were subjected to a resol-type phenol aqueous solution (water in weight ratio: resol-type phenol resin = 100:). Soaked in (mixed at a ratio of 25), dried, and thermoset in an atmosphere of 200 ° C., and then further immersed in a PTFE solution (mixed at a ratio of water: PTFE = 100: 3 by weight). The material 4 of the present invention and the comparative material 4 were dried and heat-treated in an atmosphere of 340 ° C.

次に、GDLのたわみ量の測定方法について説明する。図6に示した平坦状ブロック上に前述のGDLを設置して、溝幅(w)1mmの溝付きブロックを上方から1.7MPaの圧力(P)を押圧した状態で図7に示す浮き上がり量(溝内に侵入したGDLの寸法)δを測定した。GDLの浮き上がり量δの測定は、片面側および反対面側の両側についてそれぞれ測定した。 Next, a method for measuring the amount of deflection of GDL will be described. The above-mentioned GDL is installed on the flat block shown in FIG. 6, and the lift amount shown in FIG. 7 is pressed with a grooved block having a groove width (w) of 1 mm and a pressure (P) of 1.7 MPa from above. (Dimension of GDL that penetrated into the groove) δ was measured. The amount of lift δ of GDL was measured on both one side and the other side, respectively.

上述した測定方法に基づいて本発明材4を用いたGDLの浮き上がり量δを測定した結果、本発明材4の片面側の浮き上がり量δ1=81μmであり、反対面側の浮き上がり量δ2=43μmであった。ここで、本発明材4の片側面とは、経糸のみが実質的に無撚りであって、緯糸の上になる経糸の本数が緯糸の下になる本数より多い(1本の経糸が3本の緯糸を乗り越えた後で2本の緯糸の下をくぐる形態)面を指す。 As a result of measuring the lift amount δ of the GDL using the material 4 of the present invention based on the above-mentioned measurement method, the lift amount δ1 = 81 μm on one side of the material 4 of the present invention, and the lift amount δ2 = 43 μm on the opposite side. there were. Here, with respect to one side surface of the material 4 of the present invention, only the warp threads are substantially untwisted, and the number of warp threads above the weft threads is larger than the number of warp threads below the weft threads (three warp threads are present). Refers to the surface that passes under the two weft threads after getting over the weft threads.

つまり、本発明材4の片面側はその反対面側に比べて表出されている炭素繊維の量が多いので、GDLの浮き上がり量δ1も反対面側の浮き上がり量δ2よりも大きくなったと思われる。これに対して、その面の反対面側のGDLには前述したように凹条溝が形成されている。そのため、前述の片面側の炭素繊維が表出されている量は反対面側に比べて少なくなるので、GDLの浮き上がり量δ2は片面側の浮き上がり量δ1に比べて小さくなったと思われる。 That is, since the amount of carbon fibers exposed on one side of the material 4 of the present invention is larger than that on the opposite side, it is considered that the floating amount δ1 of GDL is also larger than the floating amount δ2 on the opposite side. .. On the other hand, a concave groove is formed in the GDL on the opposite side of the surface as described above. Therefore, since the amount of carbon fibers exposed on one side is smaller than that on the opposite side, it is considered that the floating amount δ2 of GDL is smaller than the floating amount δ1 on the one side.

これに対して、比較材4を用いたGDLの浮き上がり量δを測定した結果、両面側の浮き上がり量δ1、δ2は共に54μmで同じ値であった。これは、比較材4の織り方が両面側ともに平織りによるものであり、いずれの面も経糸、緯糸の表出形態に違いが無いためであると思われる。 On the other hand, as a result of measuring the lift amount δ of GDL using the comparative material 4, the lift amounts δ1 and δ2 on both sides were both 54 μm, which were the same values. It is considered that this is because the weaving method of the comparative material 4 is a plain weave on both sides, and there is no difference in the expression form of the warp and the weft on either side.

次に、同じ本発明材4および比較材4の各GDLを用いて、実施例1の場合と同様に発電性能の測定も行ったので、その測定結果について説明する。なお、本測定に用いたセルの構造およびガス拡散抵抗値の測定と算出根拠については、実施例1の場合と同様であるため、詳細な説明は省略する。 Next, the power generation performance was measured using the same GDLs of the material 4 of the present invention and the comparative material 4 as in the case of Example 1, and the measurement results will be described. Since the cell structure used in this measurement and the basis for measuring and calculating the gas diffusion resistance value are the same as in the case of the first embodiment, detailed description thereof will be omitted.

本発明材4のGDLを用いたセルのガス拡散抵抗値(GDR)は、53s/mであった。一方、比較材4を用いたセルのガス拡散抵抗値は、(GDR)は151s/mであり、本発明材4のGDLの抵抗値の約3倍近い測定結果となった。本発明材4のガス拡散抵抗値は、実施例1の測定で用いた本発明材1および2の測定結果(本発明材1=64s/m、本発明材2=68s/m)のいずれの結果をも上回るものであった。 The gas diffusion resistance value (GDR) of the cell using GDL of the material 4 of the present invention was 53 s / m. On the other hand, the gas diffusion resistance value of the cell using the comparative material 4 was 151 s / m in (GDR), which was almost three times the resistance value of the GDL of the material 4 of the present invention. The gas diffusion resistance value of the material 4 of the present invention is any of the measurement results of the materials 1 and 2 of the present invention (material 1 = 64 s / m, material 2 = 68 s / m) used in the measurement of Example 1. It exceeded the result.

以上のたわみ量の測定結果および発電性能(ガス拡散抵抗値)の測定結果より、発明材4のGDLの織り方の形態によって一方の面には凹条溝が形成されるので、その面に硬化処理を施すことでGDL自体の剛性を高めることができた。結果として、GDLとセパレータとが互いに接触する場合でもGDLの炭素繊維がセパレータの溝内へ侵入することを防止し、セパレータの溝を流れる水素ガスや空気の流通を妨げることを抑制できるので、燃料電池の発電効率を向上させることができる。 From the above measurement results of the amount of deflection and the measurement result of the power generation performance (gas diffusion resistance value), a concave groove is formed on one surface depending on the form of the GDL weaving of the invention material 4, and thus hardened on that surface. By applying the treatment, the rigidity of the GDL itself could be increased. As a result, even when the GDL and the separator come into contact with each other, it is possible to prevent the carbon fibers of the GDL from entering the groove of the separator and prevent the flow of hydrogen gas and air flowing through the groove of the separator. The power generation efficiency of the battery can be improved.

1、11、21、31、41 (燃料電池ガス拡散層用)炭素繊維織物
2、12、22、32 経糸
3、13、23、33 緯糸
4 凹条部
5 (溝付き)セパレータ
7 セパレータ5の溝
8 膜電極接合体
10 燃料電池セル
θ 交差角

1, 11, 21, 31, 41 (for fuel cell gas diffusion layer) Carbon fiber woven fabric 2, 12, 22, 32 Warp 3, 13, 23, 33 Weft 4 Recessed portion 5 (grooved) Separator 7 Separator 5 Groove 8 Membrane electrode assembly 10 Fuel cell cell θ Crossing angle

Claims (6)

経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物であって、前記経糸または前記緯糸の一方の糸が実質的に無撚糸であり、膜電極接合体の触媒層と接触させる前記燃料電池ガス拡散層用炭素繊維織物の一方の面は、前記無撚糸と交織されている他方の糸の上になる前記無撚糸の本数が前記他方の糸の下になる前記無撚糸の本数より多いことを特徴とする燃料電池ガス拡散層用炭素繊維織物。 A carbon fiber woven fabric for a fuel cell gas diffusion layer formed by interweaving warp threads and weft threads, wherein one of the warp threads or the weft threads is substantially untwisted and comes into contact with the catalyst layer of the membrane electrode joint. one surface of the fuel cell gas diffusion layer carbon fiber fabric make, said the other being non-twist yarns and interweaving the number of non-twist yarns made on the yarn of the non-twist yarns made under the other yarns A carbon fiber woven fabric for a fuel cell gas diffusion layer, which is characterized in that the number is larger than the number. 経糸および緯糸が交織されて形成された燃料電池ガス拡散層用炭素繊維織物であって、前記経糸および前記緯糸が共に実質的に無撚糸であり、膜電極接合体の触媒層と接触させる前記燃料電池ガス拡散層用炭素繊維織物の一方の面は、前記経糸または前記緯糸のいずれか一方の糸は、交織されている他方の糸の上になる本数が前記他方の糸の下になる本数よりも多いことを特徴とする燃料電池ガス拡散層用炭素繊維織物。 A carbon fiber woven fabric for a fuel cell gas diffusion layer formed by interweaving warp threads and weft threads, wherein both the warp threads and the weft threads are substantially untwisted threads, and the fuel is brought into contact with the catalyst layer of the membrane electrode assembly. On one side of the carbon fiber fabric for the battery gas diffusion layer, the number of threads of either the warp or the weft above the other interwoven yarn is greater than the number below the other yarn. A carbon fiber fabric for a fuel cell gas diffusion layer, which is characterized by a large number of fibers. 前記燃料電池ガス拡散層用炭素繊維織物の他方の面に凹条部が形成されている請求項1または2に記載の燃料電池ガス拡散層用炭素繊維織物。 The carbon fiber fabric for a fuel cell gas diffusion layer according to claim 1 or 2, wherein a recess is formed on the other surface of the carbon fiber fabric for the fuel cell gas diffusion layer. 前記他方の面の剛性は、前記一方の面の剛性よりも高いことを特徴とする請求項3に記載の燃料電池ガス拡散層用炭素繊維織物。 The other rigid surfaces, fuel cell gas diffusion layer for carbon fiber woven fabric according to claim 3, wherein the higher than the rigidity of said one surface. 請求項3または4に記載の燃料電池ガス拡散層用炭素繊維織物から成り前記凹条部を有するガス拡散層と、複数の溝部を有するセパレータと、を備える燃料電池セルであって、前記ガス拡散層の凹条部を有する面と、前記セパレータの溝部を有する面とが互いに接触し、かつ前記ガス拡散層の凹条部と前記セパレータの溝部との成す角度θが、10°以上35°以下の範囲であることを特徴とする燃料電池セル。 A fuel cell cell comprising the carbon fiber woven fabric for the fuel cell gas diffusion layer according to claim 3 or 4, having the gas diffusion layer having the concave portion and the separator having a plurality of grooves, and the gas diffusion. The surface having the concave portion of the layer and the surface having the groove portion of the separator are in contact with each other, and the angle θ formed by the concave portion of the gas diffusion layer and the groove portion of the separator is 10 ° or more and 35 ° or less. A fuel cell that is characterized by being in the range of. 請求項3または4に記載の前記燃料電池ガス拡散層用炭素繊維織物から成り前記凹条部を有するガス拡散層と、平面を有するセパレータと、を備える燃料電池セルであって、前記ガス拡散層の凹条部を有する面と、前記セパレータの平面と、が互いに接触していることを特徴とする燃料電池セル。
The fuel cell according to claim 3 or 4, further comprising a gas diffusion layer made of the carbon fiber woven fabric for the fuel cell gas diffusion layer and having the concave portion and a separator having a flat surface, wherein the gas diffusion layer is provided. A fuel cell in which a surface having a concave portion and a flat surface of the separator are in contact with each other.
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