JPH0963603A - Multilayer solid electrolyte for solid fuel cell - Google Patents

Multilayer solid electrolyte for solid fuel cell

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Publication number
JPH0963603A
JPH0963603A JP7239009A JP23900995A JPH0963603A JP H0963603 A JPH0963603 A JP H0963603A JP 7239009 A JP7239009 A JP 7239009A JP 23900995 A JP23900995 A JP 23900995A JP H0963603 A JPH0963603 A JP H0963603A
Authority
JP
Japan
Prior art keywords
layer
electrolyte
solid electrolyte
conductive layer
zro
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP7239009A
Other languages
Japanese (ja)
Other versions
JP3259756B2 (en
Inventor
Reiichi Chiba
玲一 千葉
Bunichi Yoshimura
文一 吉村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
NTT Inc
Original Assignee
Nippon Telegraph and Telephone Corp
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Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP23900995A priority Critical patent/JP3259756B2/en
Publication of JPH0963603A publication Critical patent/JPH0963603A/en
Application granted granted Critical
Publication of JP3259756B2 publication Critical patent/JP3259756B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M8/00Fuel cells; Manufacture thereof
    • H01M8/10Fuel cells with solid electrolytes
    • H01M8/12Fuel cells with solid electrolytes operating at high temperature, e.g. with stabilised ZrO2 electrolyte
    • H01M8/124Fuel cells with solid electrolytes operating at high temperature, e.g. with stabilised ZrO2 electrolyte characterised by the process of manufacturing or by the material of the electrolyte
    • H01M8/1246Fuel cells with solid electrolytes operating at high temperature, e.g. with stabilised ZrO2 electrolyte characterised by the process of manufacturing or by the material of the electrolyte the electrolyte consisting of oxides
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01MPROCESSES OR MEANS, e.g. BATTERIES, FOR THE DIRECT CONVERSION OF CHEMICAL ENERGY INTO ELECTRICAL ENERGY
    • H01M2300/00Electrolytes
    • H01M2300/0088Composites
    • H01M2300/0094Composites in the form of layered products, e.g. coatings
    • 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E60/00Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
    • Y02E60/30Hydrogen technology
    • Y02E60/50Fuel cells
    • 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Sustainable Development (AREA)
  • Sustainable Energy (AREA)
  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • General Chemical & Material Sciences (AREA)
  • Fuel Cell (AREA)
  • Compositions Of Oxide Ceramics (AREA)

Abstract

(57)【要約】 【課題】 機械的強度やコストの面で優れた組成の材料
を電解質の主な構成材とし、これが電極と接する表面の
みに薄くイオン伝導度の高い層を設けることにより機械
的強度の低下や材料コストの上昇をほとんど伴わずに固
体電解質内の発電損失の改善を行うことを目的とする。 【解決手段】 希土類を添加したジルコニア系固体電解
質において、イオン電導率の高いイオン伝導層とイオン
電導率の低い支持層とからなり、高イオン伝導層の層厚
が0.03ミクロンから50ミクロンで、高イオン伝導
層が電解質の燃料電極側、または空気電極側の何れか一
方もしくは、両方の表層に設けられていることを特徴と
する。 【効果】高エネルギー密度で、かつ充放電容量が大き
く、しかも安全性が確保され、サイクル寿命が長いリチ
ウム二次電池を得ることができるという優れた効果を有
する。
(57) 【Abstract】 PROBLEM TO BE SOLVED: To use a material having a composition excellent in mechanical strength and cost as a main constituent material of an electrolyte, and to form a thin layer having high ionic conductivity only on a surface in contact with an electrode. The purpose is to improve the power generation loss in the solid electrolyte with almost no decrease in the mechanical strength and increase in the material cost. In a zirconia-based solid electrolyte to which a rare earth is added, an ionic conductive layer having a high ionic conductivity and a support layer having a low ionic conductivity are provided, and the high ionic conductive layer has a layer thickness of 0.03 to 50 microns. The high ion conductive layer is provided on the surface layer of either or both of the fuel electrode side and the air electrode side of the electrolyte. [Effect] It has an excellent effect that it is possible to obtain a lithium secondary battery having a high energy density, a large charge / discharge capacity, ensuring safety, and a long cycle life.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明はイオン伝導体及び固体燃
料電池用固体電解質に関するものである。
TECHNICAL FIELD The present invention relates to an ionic conductor and a solid electrolyte for a solid fuel cell.

【0002】[0002]

【従来技術および問題点】近年、酸素イオン伝導体を用
いた固体電解質燃料電池に関心が高まりつつある。特
に、エネルギーの有効利用という観点から、固体燃料電
池はカルノー効率の制約を受けないため本質的に高いエ
ネルギー変換効率を有し、さらに良好な環境保全が期待
されるなどの優れた特徴を持っている。
2. Description of the Related Art In recent years, solid electrolyte fuel cells using oxygen ion conductors have been gaining interest. In particular, from the viewpoint of effective use of energy, solid fuel cells have inherently high energy conversion efficiency because they are not restricted by Carnot efficiency, and they also have excellent characteristics such as good environmental protection. There is.

【0003】固体電解質燃料電池の電解質は、内部をイ
オンが流れるときに直流抵抗損を低く抑える必要から、
高いイオン伝導度が求められる。このほかに、燃料電池
の運転と休止に伴う温度変化から生じる熱応力に対し、
充分な強度を保つことが必要である。このほかに、製造
コストを抑えるために、原材料に安価な材料を使用する
必要がある。
The electrolyte of a solid oxide fuel cell is required to keep DC resistance loss low when ions flow inside,
High ionic conductivity is required. In addition to this, for the thermal stress caused by the temperature change accompanying the operation and shutdown of the fuel cell,
It is necessary to maintain sufficient strength. In addition to this, it is necessary to use inexpensive materials as raw materials in order to suppress manufacturing costs.

【0004】従来最も有望視されてきた酸素イオン導伝
体には、Y23安定化ZrO2(YSZ)、Sc23
Al23安定化ZrO2(SAISZ)等がある。これ
らは、ジルコニアをベースにし、これに希土類元素等を
添加しイオン導伝性を発現させた固体電解質である。こ
れらの材料は酸素イオン輸率が100%(電子伝導性が
ない)でかつ比較的低温で焼成しても緻密なものが得ら
れるため、最も有望と考えられる。
The most promising oxygen ion conductors in the past are Y 2 O 3 -stabilized ZrO 2 (YSZ) and Sc 2 O 3 −.
There are Al 2 O 3 stabilized ZrO 2 (SAISZ) and the like. These are solid electrolytes based on zirconia, which are added with a rare earth element or the like to exhibit ion conductivity. These materials are considered to be the most promising because they have an oxygen ion transport number of 100% (no electronic conductivity) and can be dense even when fired at a relatively low temperature.

【0005】この中で最も良く検討されているものがY
23安定化ZrO2(YSZ)である。この系において
組成が0.92ZrO2−0.08Y23付近の場合、
電気伝導度が最も高い組成であることが知られている。
一方、機械的強度が最も高い組成は、0.97ZrO2
−0.03Y23であるが、伝導度は比較的劣る。ま
た、Y23の代わりにSc23を用いた場合、(1−x
−y)ZrO2−xSc23−yAl23(0.070
<x+y<0.160かつ0.000<x<0.02
0)、ジルコニア系の中で最も高いイオン伝導度を示
す。しかし、ここで添加物として用いる材料(Sc
23)は、非常に高価なため、多量に使用すると製造コ
ストを低く抑えることが難しい。このようにジルコニア
系固体電解質においても、一つの材料で全ての要求を満
足することは難しい。
The most studied among these is Y
2 O 3 stabilized ZrO 2 (YSZ). In this system, when the composition is near 0.92ZrO 2 -0.08Y 2 O 3 ,
It is known that the composition has the highest electric conductivity.
On the other hand, the composition with the highest mechanical strength is 0.97ZrO 2
Is a -0.03Y 2 O 3, the conductivity is relatively poor. When Sc 2 O 3 is used instead of Y 2 O 3 , (1-x
-Y) ZrO 2 -xSc 2 O 3 -yAl 2 O 3 (0.070
<X + y <0.160 and 0.000 <x <0.02
0), which has the highest ionic conductivity among zirconia-based materials. However, the materials (Sc
Since 2 O 3 ) is very expensive, it is difficult to keep the manufacturing cost low when used in a large amount. As described above, it is difficult to satisfy all the requirements with one material even in the zirconia-based solid electrolyte.

【0006】[0006]

【発明の目的】本発明は機械的強度やコストの面で優れ
た組成の材料を電解質の主な構成材とし、これが電極と
接する表面のみに薄くイオン伝導度の高い層を設けるこ
とにより機械的強度の低下や材料コストの上昇をほとん
ど伴わずに固体電解質内の発電損失の改善を行うことを
目的とする。
An object of the present invention is to use a material having a composition excellent in mechanical strength and cost as a main constituent material of an electrolyte, and to provide a thin layer having a high ionic conductivity only on the surface in contact with an electrode to improve mechanical properties. The purpose is to improve the power generation loss in the solid electrolyte with almost no decrease in strength and increase in material cost.

【0007】[0007]

【問題点を解決するための手段】上記問題点を解決する
ため、本発明による固体燃料電池用多層型固体電解質は
希土類を添加したジルコニア系固体電解質において、イ
オン電導率の高いイオン伝導層とイオン電導率の低い支
持層とからなり、高イオン伝導層の層厚が0.03ミク
ロンから50ミクロンで、高イオン伝導層が電解質の燃
料極側、または空気極側の何れか一方もしくは、両方の
表層に設けられていることを特徴とする。
In order to solve the above problems, a multilayer solid electrolyte for a solid fuel cell according to the present invention is a zirconia-based solid electrolyte containing a rare earth element and an ion conductive layer having a high ion conductivity and an ion. The high ionic conductive layer has a layer thickness of 0.03 μm to 50 μm, and the high ionic conductive layer has either a fuel electrode side or an air electrode side of the electrolyte, or both. It is characterized in that it is provided on the surface layer.

【0008】本発明は図1に示すごとく酸素電極1、燃
料電極2と接する面において、イオン伝導度の高い0.
92ZrO2−0.08Y23または(1−x−y)Z
rO2−xSc23−yAl23(0.070<x+y
<0.160かつ0.000<x<0.020)等の高
イオン伝導層3を設け、これ以外の部分には、イオン伝
導度は比較的低いが、機械的強度やコストの面で優れた
他の組成の支持層4を用いる。
According to the present invention, as shown in FIG. 1, in the surface which is in contact with the oxygen electrode 1 and the fuel electrode 2, a high ion conductivity of 0.
92ZrO 2 -0.08Y 2 O 3 or (1-xy) Z
rO 2 -xSc 2 O 3 -yAl 2 O 3 (0.070 <x + y
<0.160 and 0.000 <x <0.020) and other high ionic conductive layers 3 are provided. Other parts have relatively low ionic conductivity, but are excellent in mechanical strength and cost. A support layer 4 having another composition is used.

【0009】ここで、高イオン伝導層3の厚みは、これ
が接する電極1、2材の粒径と同程度かそれ以下である
が少なくとも良好な膜質を得るには0.03ミクロン以
上の膜厚を必要とする。電極材の粒径は作製プロセスに
より異なるが、通常平均粒径が、0.2から50ミクロ
ンの間であるので、高イオン伝導層の厚みも0.02ミ
クロン以上は必要である。粒径により0.02ミクロン
から50ミクロン程度となる。しかし良好な膜質を得る
ために高イオン伝導層3の膜厚の下限は、0.03ミク
ロンとなる。また、支持層4は、1から200ミクロン
程度となる。支持層、高イオン伝導層ともに、層厚が2
0から200ミクロン程度までならテープキャスティン
グ法、ドクターブレード法、ディッピング法、EVD法
で作製可能である。10ミクロン以下では、ディッピン
グ法、EVD法、そして、RFスパッタリング法等で作
製可能である。
Here, the thickness of the high ion conductive layer 3 is equal to or smaller than the particle diameter of the electrodes 1 and 2 in contact with it, but at least 0.03 micron or more is required to obtain a good film quality. Need. The particle size of the electrode material varies depending on the manufacturing process, but since the average particle size is usually between 0.2 and 50 μm, the thickness of the high ion conductive layer must be 0.02 μm or more. Depending on the particle size, it will be about 0.02 to 50 microns. However, in order to obtain good film quality, the lower limit of the film thickness of the high ion conductive layer 3 is 0.03 micron. The support layer 4 has a thickness of about 1 to 200 μm. Both the support layer and the high ion conductive layer have a layer thickness of 2
If it is about 0 to 200 μm, it can be manufactured by a tape casting method, a doctor blade method, a dipping method, or an EVD method. If it is 10 microns or less, it can be manufactured by a dipping method, an EVD method, an RF sputtering method, or the like.

【0010】[0010]

【作用】図2に示すように、燃料電池において不可欠な
電気化学反応(空気電極の場合O2→2O,2O+4e-
→2O2-)は、反応ガスと電流を供給する電極、そし
て、イオンを運ぶ電解質が同時に接する三相界面におい
て行われている。図2において、5は電極の微粒子であ
る。
As shown in FIG. 2, an electrochemical reaction (in the case of an air electrode, O 2 → 2O, 2O + 4e
→ 2O 2- ) is carried out at the three-phase interface in which the reaction gas, the electrode supplying the current, and the electrolyte carrying the ions are in contact at the same time. In FIG. 2, 5 is a fine particle of the electrode.

【0011】ここで、電解質に接する電極材料は、電極
と電解質の界面まで、反応ガスを十分に導くため多孔質
にしておく必要がある。このため電極材はある程度粒径
の大きな材料で構成されなければならない。図7に示す
ように固体電解質6の両側に直接酸素電極1および燃料
電極2を設けている場合、このようにして作られたイオ
ンは、図8に示すように電解質4の内部をイオン電流と
して流れていく。この場合イオン電流は、三相界面を源
として流れるため、この付近に集中する傾向にある。こ
の電流の集中は、電極材の粒径が大きいほど顕著にな
り、電流の集中が電解質の内部まで深く残る。そして、
この電流の集中は、導体の実質的な断面積の減少を意味
し、この部分において大きな電圧降下をもたらし、電解
質内での発電損失の大きな原因となっている。
Here, the electrode material in contact with the electrolyte needs to be porous so as to sufficiently guide the reaction gas to the interface between the electrode and the electrolyte. For this reason, the electrode material must be made of a material having a relatively large grain size. When the oxygen electrode 1 and the fuel electrode 2 are provided directly on both sides of the solid electrolyte 6 as shown in FIG. 7, the ions thus produced are converted into an ionic current inside the electrolyte 4 as shown in FIG. It flows. In this case, since the ionic current flows from the three-phase interface as a source, it tends to concentrate in this vicinity. The larger the particle size of the electrode material, the more remarkable the current concentration becomes, and the current concentration remains deep inside the electrolyte. And
This concentration of current means a substantial reduction in the cross-sectional area of the conductor, which causes a large voltage drop in this portion, which is a major cause of power generation loss in the electrolyte.

【0012】以上の理由により、界面付近のイオン伝導
度は、セル特性に大きな影響を及ぼす。特に電解質全体
の厚みが薄い場合においては、界面付近の電圧降下が電
解質内での電圧降下の主要な部分となる。
For the above reasons, the ionic conductivity near the interface has a great influence on the cell characteristics. In particular, when the thickness of the entire electrolyte is thin, the voltage drop near the interface becomes the main part of the voltage drop in the electrolyte.

【0013】もし、上記のイオン電流の集中する界面付
近をイオン導電性の高い材料3に代えた多層型固体電解
質(高イオン伝導層+支持層)にした場合、この部分に
おける電圧降下が改善される。これと同時に、高イオン
伝導層3内で電流の集中が緩和され易くなり(電流分布
が均一になりやすい)、支持層4内の電流の集中は軽減
される。これを図4に模式的に示した。このため、表面
にごく薄い高イオン伝導層を設けるだけで、電解質内で
の電圧降下を軽減することができる。また、これ以外の
電解質全体の厚みの主要な部分には、伝導度が劣るもの
の機械的強度や材料コストの面で優れたイオン伝導体を
用いる。この結果、機械的強度の低下や材料コストの上
昇をほとんど伴わずに固体電解質内の発電損失の改善を
行うことができる。
If a multilayer solid electrolyte (high ionic conduction layer + support layer) is used in which the vicinity of the interface where the ionic current is concentrated is replaced with the material 3 having high ionic conductivity, the voltage drop in this portion is improved. It At the same time, the concentration of current in the high ion conductive layer 3 is easily alleviated (current distribution is likely to be uniform), and the concentration of current in the support layer 4 is reduced. This is schematically shown in FIG. Therefore, the voltage drop in the electrolyte can be reduced only by providing a very thin high ion conductive layer on the surface. In addition, an ionic conductor having low conductivity but excellent in mechanical strength and material cost is used for the other major portion of the total thickness of the electrolyte. As a result, the power generation loss in the solid electrolyte can be improved with almost no reduction in mechanical strength and increase in material cost.

【0014】[0014]

【実施例】以下に本発明の実施例を説明する。なお、当
然のことであるが本発明は以下の実施例に限定されるも
のではない。
Embodiments of the present invention will be described below. Note that, needless to say, the present invention is not limited to the following embodiments.

【0015】[0015]

【実施例1】図5、図6は本発明の材料を用いた単セル
の固体燃料電池の構成例を示す図である。図5は平面
図、図6は断面図である。本実施例の電池構成におい
て、1は酸素電極、2は燃料電極、3は高イオン伝導
層、4は支持層、7は集電用の白金メッシュ、8は白金
ペーストの参照極、9はアルミナ管である(高イオン伝
導層3+支持層4で固体電解質が構成される)。酸素電
極としてはLa0.8Sr0.2MnO3を、燃料電極にはN
i−(0.92ZrO2−0.08Y23)を用いた。
集電用の白金メッシュは16mmφであった。セルの有
効面積は、電極の面積に等しく約2cm2である。単セ
ルの作成方法は次のとおりである。
EXAMPLE 1 FIGS. 5 and 6 are views showing a constitutional example of a single cell solid fuel cell using the material of the present invention. 5 is a plan view and FIG. 6 is a sectional view. In the battery structure of this embodiment, 1 is an oxygen electrode, 2 is a fuel electrode, 3 is a high ion conductive layer, 4 is a support layer, 7 is a platinum mesh for collecting current, 8 is a platinum paste reference electrode, and 9 is alumina. It is a tube (a solid electrolyte is composed of the high ion conductive layer 3 + the support layer 4). La 0.8 Sr 0.2 MnO 3 was used as the oxygen electrode and N was used as the fuel electrode.
i- the (0.92ZrO 2 -0.08Y 2 O 3) was used.
The platinum mesh for current collection was 16 mmφ. The effective area of the cell is equal to the area of the electrode and is about 2 cm 2 . The method for producing a single cell is as follows.

【0016】まず、組成が0.97ZrO2−0.03
23の微粉末を通常の固相反応により合成し、ドクタ
ーブレード法によりセラミックス薄膜を形成し1200
℃で焼き上げる。約100ミクロンに焼成されたこの板
は、固体電解質のうち支持層4にあたる部分である。さ
らにこの板の両面にディッピング法により組成が0.8
8ZrO2−0.115Sc23−0.005Al23
の層を積層し、1100℃で燒結させ、両面に各々5.
0ミクロンの高イオン伝導層を設けた。そして約200
ミクロン厚の燃料電極Ni−YSZおよび空気電極La
0.8Sr0.2MnO3を片面ずつ上記の固体電解質板の上
に1100℃で焼き付けた。
First, the composition is 0.97ZrO 2 -0.03.
Fine powder of Y 2 O 3 was synthesized by a usual solid phase reaction, and a ceramic thin film was formed by the doctor blade method.
Bake at ℃. This plate, which has been baked to about 100 microns, is the portion of the solid electrolyte that corresponds to the support layer 4. Furthermore, the composition is 0.8 on both sides of this plate by the dipping method.
8ZrO 2 -0.115Sc 2 O 3 -0.005Al 2 O 3
Layers were laminated and sintered at 1100 ° C., and 5.
A 0 micron high ionic conduction layer was provided. And about 200
Micron-thick fuel electrode Ni-YSZ and air electrode La
0.8 Sr 0.2 MnO 3 was baked on each side of the above solid electrolyte plate at 1100 ° C.

【0017】本実施例の効果を図7の測定例で示す。こ
れは、上記の要領で作られた”セル#1”について80
0℃で測定した単セルの電流(電流密度)−電圧特性で
ある。比較のために従来構造の電解質を用いた”セル#
0”も同じ条件で測定した。これも図7に示してある。
ここで燃料極、酸素極にはそれぞれH2、O2、ガスを用
いている。図から明らかなように、本実施例は従来例よ
り良好な電池特性すなわち電流−電圧特性が得られた。
同様にして本発明の材料を多層型固体電解質を片面だけ
に用いた場合でも、”セル#2”、”セル#3”のよう
に、その電池特性はすべて従来例より良好であった。こ
れらを表1に示す。
The effect of this embodiment is shown in the measurement example of FIG. This is 80 for "cell # 1" created as above
It is a current (current density) -voltage characteristic of a single cell measured at 0 ° C. "Cell # with conventional structure electrolyte for comparison"
0 "was also measured under the same conditions. This is also shown in FIG.
Here, H 2 , O 2 and gas are used for the fuel electrode and the oxygen electrode, respectively. As is clear from the figure, this example provided better battery characteristics, that is, current-voltage characteristics, than the conventional example.
Similarly, when the material of the present invention was used for the single-sided multi-layer solid electrolyte, the battery characteristics were all better than those of the conventional example, as in "cell # 2" and "cell # 3". These are shown in Table 1.

【0018】表1 電解質及び電極の構成が/酸素電極/”層#1”/”層
#2”/”層#3”/燃料電極/の多層となっている場
合の単セルにおける出力電流。単セルは、酸素電極(L
0.8Sr0.2MnO3)/電解質/燃料電極(Ni−Y
SZ)とした。 *セルの出力電圧が0.2Vのときの電流値(800℃において測定)。
Table 1 Output current in a single cell when the composition of the electrolyte and the electrode is a multi-layer of / oxygen electrode / "layer # 1" / "layer # 2" / "layer # 3" / fuel electrode /. The single cell has an oxygen electrode (L
a 0.8 Sr 0.2 MnO 3 ) / electrolyte / fuel electrode (Ni-Y
SZ). * Current value when the cell output voltage is 0.2V (measured at 800 ° C).

【0019】[0019]

【実施例2】実施例1と同様の構成でかつ高イオン伝導
層の厚みのみを変えたセルを作りその電流電圧特性を測
定した。表2に示すように、高イオン伝導層の層厚だけ
を0.5ミクロンまで変化させた。いずれも従来の”セ
ル#0”(表1参照)よりも良好な特性が得られた。
Example 2 A cell having the same structure as that of Example 1 except that the thickness of the high ion conductive layer was changed was prepared, and its current-voltage characteristics were measured. As shown in Table 2, only the layer thickness of the high ion conductive layer was changed to 0.5 micron. In all cases, better characteristics were obtained as compared with the conventional "cell # 0" (see Table 1).

【0020】表2 単セルにおける出力電流の高イオン伝導層厚依存性 固体電解質として”セル#1”の構成で高イオン伝導層
厚だけ変えた。 *セルの出力電圧が0.2Vのときの電流値(800℃
において測定)。
Table 2 Dependence of output current on high ionic conduction layer thickness in single cell In the constitution of "cell # 1" as the solid electrolyte, only the high ionic conduction layer thickness was changed. * Current value when cell output voltage is 0.2V (800 ℃
In).

【0021】[0021]

【実施例3】実施例1と同様の構成でかつ支持層の厚み
のみを変えたセルを作りその電流電圧特性を測定した。
表3に示すように、支持層の層厚だけを50ミクロンか
ら150ミクロンまで変化させた。いずれも従来の”セ
ル#0”(表1参照)よりも良好な特性が得られた。
Example 3 A cell having the same structure as in Example 1 except that the thickness of the support layer was changed was prepared, and the current-voltage characteristics thereof were measured.
As shown in Table 3, only the layer thickness of the support layer was changed from 50 microns to 150 microns. In all cases, better characteristics were obtained as compared with the conventional "cell # 0" (see Table 1).

【0022】表3 単セルにおける出力電流の支持層厚依存性 固体電解質として”セル#1”の構成で支持層厚だけ変
えた。 セルの出力電圧が0.2Vのときの電流値(800℃に
おいて測定)。
Table 3 Dependence of output current in single cell on support layer thickness In the constitution of "cell # 1" as the solid electrolyte, only the support layer thickness was changed. Current value when cell output voltage is 0.2 V (measured at 800 ° C.).

【0023】[0023]

【実施例4】実施例1と同様の構成でかつ高イオン伝導
層の組成のみを変えたセルを作りその電流電圧特性を測
定した。この結果を表4に示す。いずれも従来の”セル
#0”(表1参照)よりも良好な特性が得られた。
Example 4 A cell having the same structure as that of Example 1 except that only the composition of the high ion conductive layer was changed was prepared, and its current-voltage characteristics were measured. Table 4 shows the results. In all cases, better characteristics were obtained as compared with the conventional "cell # 0" (see Table 1).

【0024】表4 単セルにおける出力電流の高イオン伝導層組成依存性 固体電解質として”セル#1”の構成で高イオン伝導層
組成だけ変えた。 セルの出力電圧が0.2Vのときの電流値(800℃において測定)。
Table 4 Dependence of the output current in a single cell on the composition of the high ionic conduction layer Only the composition of the high ionic conduction layer was changed in the constitution of "cell # 1" as the solid electrolyte. Current value when cell output voltage is 0.2 V (measured at 800 ° C.).

【0025】[0025]

【実施例5】実施例1と同様の構成でかつ支持層組成の
みを変えたセルを作りその電流電圧特性を測定した。こ
の結果を表5に示す。いずれも従来の”セル#0”(表
1参照)よりも良好な特性が得られた。
Example 5 A cell having the same structure as that of Example 1 except that only the composition of the supporting layer was changed was prepared, and its current-voltage characteristics were measured. Table 5 shows the results. In all cases, better characteristics were obtained as compared with the conventional "cell # 0" (see Table 1).

【0026】表5 単セルにおける出力電流の支持層組成依存性 固体電解質として”セル#1”の構成で支持層組成だけ
変えた。 セルの出力電圧が0.2Vのときの電流値(800℃において測定)。
Table 5 Dependence of output current in single cell on support layer composition Only the support layer composition was changed in the configuration of "cell # 1" as a solid electrolyte. Current value when cell output voltage is 0.2 V (measured at 800 ° C.).

【0027】表6 単セルにおける出力電流の支持層組成依存性 固体電解質として”セル#0”の構成で支持層組成だけ
変えた。(従来型セルで高イオン伝導層がない) セルの出力電圧が0.2Vのときの電流値(800℃において測定)。
Table 6 Dependence of output current in single cell on supporting layer composition Only the supporting layer composition was changed in the constitution of "cell # 0" as the solid electrolyte. (Conventional cell without high ionic conduction layer) Current value when cell output voltage is 0.2 V (measured at 800 ° C.).

【0028】[0028]

【発明の効果】以上説明したように、機械的強度やコス
トの面で優れた組成の材料を電解質の主な構成材料と
し、これが電極と接する表面にのみ薄くイオン伝導度の
高い層を設けることにより機械的強度の低下や材料コス
トの上昇をほとんど伴わずに固体電解質内の発電損失の
改善を行うことができる。
As described above, a material having a composition excellent in mechanical strength and cost is used as a main constituent material of the electrolyte, and a thin layer having high ionic conductivity is provided only on the surface in contact with the electrode. As a result, the power generation loss in the solid electrolyte can be improved with almost no decrease in mechanical strength and increase in material cost.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の電解質の構成図。FIG. 1 is a configuration diagram of an electrolyte of the present invention.

【図2】三相界面において行われている電気化学的反応
過程の模式図。
FIG. 2 is a schematic diagram of an electrochemical reaction process performed at a three-phase interface.

【図3】高イオン伝導層を付加した場合の電解質内のイ
オン電流分布の模式図。
FIG. 3 is a schematic diagram of an ion current distribution in an electrolyte when a high ion conductive layer is added.

【図4】単セルの構成模式図。FIG. 4 is a schematic diagram of the configuration of a single cell.

【図5】単セルの構成模式図。FIG. 5 is a schematic diagram of the configuration of a single cell.

【図6】”セル#0”及び”セル#1”の電流−電圧特
性図。
FIG. 6 is a current-voltage characteristic diagram of “cell # 0” and “cell # 1”.

【図7】従来の電解質の構成図。FIG. 7 is a configuration diagram of a conventional electrolyte.

【図8】従来の電解質内のイオン電流分布の模式図。FIG. 8 is a schematic diagram of an ion current distribution in a conventional electrolyte.

【符号の説明】[Explanation of symbols]

1 酸素電極 2 燃料電極 3 高イオン伝導層 4 支持層 5 電極の微粒子 6 従来の固体電解質 7 集電用の白金メッシュ 8 参照極 9 アルミナ管 1 Oxygen Electrode 2 Fuel Electrode 3 High Ion Conductive Layer 4 Support Layer 5 Electrode Fine Particles 6 Conventional Solid Electrolyte 7 Platinum Mesh for Current Collection 8 Reference Electrode 9 Alumina Tube

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】希土類を添加したジルコニア系固体電解質
において、イオン電導率の高いイオン伝導層とイオン電
導率の低い支持層とからなり、高イオン伝導層の層厚が
0.03ミクロンから50ミクロンで、高イオン伝導層
が電解質の燃料極側、または空気極側の何れか一方もし
くは、両方の表層に設けられていることを特徴とする固
体燃料電池用多層型固体電解質。
1. A zirconia-based solid electrolyte to which a rare earth is added, which comprises an ion conductive layer having a high ionic conductivity and a supporting layer having a low ionic conductivity, and the layer thickness of the high ionic conductive layer is 0.03 to 50 μm. 2. A multi-layer solid electrolyte for a solid fuel cell, characterized in that the high ionic conductive layer is provided on the surface layer of either or both of the fuel electrode side and the air electrode side of the electrolyte.
【請求項2】請求項1の高イオン伝導層に(1−x−
y)ZrO2−xSc23−yAl23(0.070<
x+y<0.160かつ0.005<y<0.020)
なる組成を有するイオン伝導体を用い、支持層に(1−
x)ZrO2−xY23(0.025<x<0.04
0)を用いることを特徴とする固体燃料電池。
2. The high ionic conduction layer according to claim 1, wherein (1-x-
y) ZrO 2 -xSc 2 O 3 -yAl 2 O 3 (0.070 <
x + y <0.160 and 0.005 <y <0.020)
An ionic conductor having a composition of
x) ZrO 2 -xY 2 O 3 (0.025 <x <0.04
0) is used, The solid fuel cell characterized by the above-mentioned.
【請求項3】請求項1の高イオン伝導層に(1−x−
y)ZrO2−xSc23−yD23(D=Ybまたは
Luで、かつ0.070<x+y<0.220かつ0.
015<y<0.060)なる組成を有するイオン伝導
体を用い、支持層に(1−x)ZrO2−xY2
3(0.025<x<0.040)を用いることを特徴
とする固体燃料電池用多層型固体電解質。
3. The high ionic conduction layer according to claim 1, wherein (1-x-
In y) ZrO 2 -xSc 2 O 3 -yD 2 O 3 (D = Yb or Lu, and 0.070 <x + y <0.220 and 0.
An ionic conductor having a composition of 015 <y <0.060) is used, and (1-x) ZrO 2 —xY 2 O is used for the supporting layer.
3 (0.025 <x <0.040) is used, The multilayer solid electrolyte for solid fuel cells characterized by the above-mentioned.
【請求項4】請求項1の高イオン伝導層に(1−x−
y)ZrO2−xSc23(0.070<x+y<0.
160かつ0.005<y<0.020)なる組成を有
するイオン伝導体を用い、支持層に(1−x)ZrO2
−xY23(0.070<x<0.110)を用いるこ
とを特徴とする固体燃料電池用多層型固体電解質。
4. The high ion conductive layer according to claim 1, wherein (1-x-
y) ZrO 2 -xSc 2 O 3 (0.070 <x + y <0.
An ion conductor having a composition of 160 and 0.005 <y <0.020) is used, and (1-x) ZrO 2 is used for the supporting layer.
-XY 2 O 3 (0.070 <x <0.110) solid fuel cell multilayer solid electrolyte, which comprises using a.
【請求項5】請求項1の高イオン伝導層に(1−x−
y)ZrO2−xSc23−yD23(D=Ybまたは
Luで、かつ0.070<x+y<0.220かつ0.
015<y<0.060)なる組成を有するイオン伝導
体を用い、支持層に(1−x)ZrO2−xY2
3(0.070<x<0.110)を用いることを特徴
とする固体燃料電池用多層型固体電解質。
5. The high ion conductive layer according to claim 1, wherein (1-x-
In y) ZrO 2 -xSc 2 O 3 -yD 2 O 3 (D = Yb or Lu, and 0.070 <x + y <0.220 and 0.
An ionic conductor having a composition of 015 <y <0.060) is used, and (1-x) ZrO 2 —xY 2 O is used for the supporting layer.
3 (0.070 <x <0.110) is used, The multilayer solid electrolyte for solid fuel cells characterized by the above-mentioned.
【請求項6】請求項1の高イオン伝導層に(1−x)Z
rO2−xY23(0.070<x<0.110)なる
組成を有する伝導体を用い、支持層に(1−x)ZrO
2−xY23(0.025<x<0.040)を用いた
ことを特徴とする固体燃料電池用多層型固体電解質。
6. The high ion conductive layer according to claim 1, wherein (1-x) Z is added.
A conductor having a composition of rO 2 −xY 2 O 3 (0.070 <x <0.110) is used, and (1-x) ZrO is used for the support layer.
A multi-layer solid electrolyte for a solid fuel cell, characterized by using 2- xY 2 O 3 (0.025 <x <0.040).
JP23900995A 1995-08-25 1995-08-25 Multilayer solid electrolyte for solid fuel cells Expired - Fee Related JP3259756B2 (en)

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