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JP3603116B2 - High-density yttria-stabilized zirconia sintered body and method for producing the same - Google Patents
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JP3603116B2 - High-density yttria-stabilized zirconia sintered body and method for producing the same - Google Patents

High-density yttria-stabilized zirconia sintered body and method for producing the same Download PDF

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JP3603116B2
JP3603116B2 JP2001057835A JP2001057835A JP3603116B2 JP 3603116 B2 JP3603116 B2 JP 3603116B2 JP 2001057835 A JP2001057835 A JP 2001057835A JP 2001057835 A JP2001057835 A JP 2001057835A JP 3603116 B2 JP3603116 B2 JP 3603116B2
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sintered body
density
ysz
conductivity
stabilized zirconia
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JP2002255642A (en
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友成 竹内
勝裕 野村
功 近藤
信幸 玉利
博之 蔭山
繁雄 棚瀬
義憲 宮崎
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National Institute of Advanced Industrial Science and Technology AIST
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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

【0001】
【発明の属する技術分野】
本発明は、高密度イットリア安定化ジルコニア焼結体及びその製造方法に関する。高密度イットリア安定化ジルコニア焼結体は、例えば固体電解質型燃料電池の固体電解質として有用である。以下、イットリア安定化ジルコニアは、「YSZ」と記載する。
【0002】
【従来の技術】
燃料電池は現行の火力発電を超える高効率が期待される化石燃料/電力変換デバイスであり、燃料電池の中でも、特に固体酸化物を電解質に用いたもの(固体電解質型燃料電池:Solid Oxide Fuel Cell(以下、「SOFC」と略記する。))は、最も高いエネルギー変換効率を有するものとして注目されている。SOFCの電解質に用いる固体酸化物としては、例えばYSZ焼結体がよく知られている。
【0003】
しかしながら、SOFCの電解質としてYSZ焼結体を用いる場合には、SOFCの通常の作動温度である1000℃近傍で1000時間以上運転すると、YSZ焼結体の劣化により、発電効率が低下するといった問題がある。この原因としては、SOFCの高温長時間運転に起因する下記事項が考えられる;
▲1▼YSZ焼結体に亀裂が生じること、
▲2▼YSZ焼結体のイオン導電率が低下すること、
▲3▼電極材料の焼結進行により、電極反応が抑制されること、及び
▲4▼YSZ焼結体/電極界面における固相反応進行による低導電層の生成。
【0004】
このような現状に鑑みて、前記の問題を解消するために、種々の試みがなされている。例えば、YSZ焼結体の機械的強度を高めるために、その組成にAl、MgO等を添加する試みがなされている。
【0005】
しかしながら、異種元素の添加は、YSZ焼結体の機械的強度を高めるものではあるが、同時にYSZ焼結体の導電率を低下させることも報告されている(例えば、L.M.Navarro,P.Recio,J.R.Jurado,and P.Duran,J.Mater.Sci.,30,1949(1995).)。また、添加した異種元素が、SOFCの高温長時間運転に伴い、電解質粒界に析出し、結果的に抵抗を増大させ、却ってSOFCの性能低下を引き起こす可能性も示唆されている。いずれにせよ、現状の試みでは従来技術の問題点を大巾に解消するには至っていない。
【0006】
【発明が解決しようとする課題】
以上のような見地より、従来のYSZ焼結体と比較して、機械的強度が高く、高温条件下においても導電率の経時低下が抑制された高密度YSZ焼結体の開発が強く要請されているものの、そのような高密度YSZ焼結体は未だ開発されるに至っていない。
【0007】
従って、本発明は、特に機械的強度が高く、高温条件下においても導電率の経時低下が抑制された高密度YSZ焼結体を提供することを目的とする。併せて、高密度YSZ焼結体の製造方法を提供することを目的とする。
【0008】
【課題を解決するための手段】
本発明者は、従来技術の問題点を解決するために鋭意研究を重ねた結果、下記の高密度YSZ焼結体及びその製造方法が上記目的を達成することを見出し、ついに本発明を完成するに至った。
【0009】
本発明は、下記の高密度YSZ焼結体及びその製造方法に係るものである。
【0010】
1.高密度イットリア安定化ジルコニア焼結体であって;
(1)焼結体のかさ密度が理論密度の95%以上、
(2)焼結体の最大粒子径が2μm以下であり、且つ平均粒子径が1μm以下、
(3)焼結体の室温曲げ強度が300MPa以上、及び
(4)焼結体を1000℃の温度下で1000時間保持した場合において、初期の導電率σに対する1000時間経過後の導電率σ1000の割合(σ1000/σ)が0.68以上
であることを特徴とする高密度イットリア安定化ジルコニア焼結体。
【0011】
2.Yを1〜20mol%ドープしたZrO粉末(イットリア安定化ジルコニア)を10〜60MPaの圧力で加圧しつつ、500〜1500Aの直流パルス電流を用いて160〜170℃/minの昇温速度で1100〜1300℃に加熱した後、1〜30分間放電プラズマ焼結することを特徴とする高密度イットリア安定化ジルコニア焼結体の製造方法。
【0012】
3.1100〜1300℃の範囲から選択される加熱温度(℃)と1〜30分間(即ち1/60〜1/2時間)の範囲から選択される放電プラズマ焼結に係る保持時間(時間)との積(℃・時間)の値が250以下である上記項2に記載の高密度イットリア安定化ジルコニア焼結体の製造方法。
【0013】
【発明の実施の形態】
高密度YSZ焼結体
以下、本発明の高密度YSZ焼結体が満足すべき(1)〜(4)の要件について詳細に説明する。
(1)焼結体のかさ密度が理論密度の95%以上であること。
【0014】
焼結体のかさ密度が理論密度(6g/cm)の95%未満の場合は、摩擦、衝撃等の外部応力に対する焼結体の破壊エネルギーが小さくなり、機械的強度の低下が生じる。また、気孔率が増加するため、例えばSOFCの固体電解質として用いる場合には、燃料ガスと空気の混合が生じ、発電効率が著しく低下する。従って、焼結体のかさ密度は、理論密度の95%以上であることが必要であり、特に98%以上であることが好ましい。
(2)焼結体の最大粒子径が2μm以下であり、且つ平均粒子径が1μm以下であること。
【0015】
一般に焼結体の粒子径が大きくなるにつれて、粒脱離摩耗による損耗が起こりやすい傾向にあるが、本発明の焼結体においても、最大粒子径が2μmを超えると、立方晶の安定性が劣るようになる。従って、例えばこの焼結体をSOFCの固体電解質として用いる場合には、SOFCを1000℃の作動温度で1000時間以上保持すると、立方晶の存在比が低下し、導電率の低い正方晶の存在比が多くなる。
【0016】
また、セラミックスの機械的強度が平均粒子径の平方根の逆数に比例すること、及び平均粒子径が1μmを超える場合には、機械的強度に殆ど差がないことを考慮すると、平均粒子径が1μm以下であることが必要となる。
【0017】
以上より、本発明の高密度YSZ焼結体は、最大粒子径が2μm以下であり、且つ平均粒子径が1μm以下であることを要する。この中でも、特に最大粒子径が1μm以下であり、平均粒子径が0.5μm以下であるものが好ましい。
【0018】
本発明では、粒子径は、高密度YSZ焼結体を顕微鏡観察し、観察される粒子を球形近似して算出した直径のことである。平均粒子径は、上記の球形近似で算出した直径の平均値である。
(3)焼結体の室温曲げ強度が300MPa以上であること。
【0019】
本発明の高密度YSZ焼結体は、例えばSOFCの固体電解質、耐熱電極等の高温導電性材料としての用途が考えられるため、繰り返しの昇降温や温度分布等による熱応力、熱衝撃に耐え得る充分な強度を有することが必要である。従って、焼結体の室温曲げ強度が300MPa以上であることが必要であり、特に320MPa以上であることが好ましい。
【0020】
なお、本発明では、室温曲げ強度の値は、室温下で高密度YSZ焼結体の3点曲げ強度を測定した値である。具体的には、JIS R1601の基準に従って、♯1000のダイヤモンド研磨盤で四面を仕上げた3×4mm角の試験片を用い、スパン30mm及び荷重速度0.5mm/minの条件で測定した3点曲げ強度(室温下)の値である。
(4)焼結体を1000℃の温度下で1000時間保持した場合において、初期の導電率σに対する1000時間経過後の導電率σ1000の割合(σ1000/σ)が0.68以上であること。
【0021】
本発明では、導電率は、高密度YSZ焼結体を角棒の形状に削り出し、白金製電極及び電圧測定用の白金製リード線を1000℃程度で焼付け、交流四端子法により交流導電率(S/cm)を測定した値である。
【0022】
本発明の高密度YSZ焼結体のσは、通常0.1S/cmであるが、例えばこの焼結体をSOFCの固体電解質として用いた場合、SOFCを1000℃の作動温度で1000時間以上保持した際に、導電率が0.068S/cm未満であれば、発電効率が低下する。従って、本発明の高密度YSZ焼結体は、σに対するσ1000の割合(σ1000/σ)が0.68以上であることを要する。
【0023】
高密度YSZ焼結体の製造方法
以下、本発明の高密度YSZ焼結体の製造方法について詳細に説明する。
【0024】
原料粉末としては、Yを1〜20mol%ドープしたZrO粉末(YSZ粉末)であれば特に限定されず、公知のもの又は市販品を用いることができる。Yをドープする割合は、1〜20mol%の中から適宜設定することができるが、特に3〜10mol%程度が好ましい。
【0025】
YSZ粉末の調製方法としては、特に限定されず、固相反応法、加水分解法、ゾル−ゲル法、水熱法等から選択されるいずれの合成手法でも良い。YSZ粉末の粒子径は、特に限定されないが、通常サブミクロン又はそれ以下の粒子径であることが好ましい。
【0026】
本発明では、前記したYSZ粉末を特定条件下で放電プラズマ焼結することで、焼結体の粒子径成長を抑制しつつ焼結し、高密度YSZ焼結体を得る。すなわち原料であるYSZ粉末よりも高密度のYSZ焼結体を得ることができる。
【0027】
本発明では、YSZ粉末を放電プラズマ焼結するために、放電プラズマ焼結機を用いることが好ましい。放電プラズマ焼結、放電焼結及び通電焼結等のON−OFFパルス通電による焼結法を用いて、YSZ粉末を圧縮して圧粉体とし、この圧粉体にパルス電流を通電すると共に、そのピーク電流とパルス幅とを制御してYSZ粉末の温度を制御しつつ圧縮焼結することが好ましい。
【0028】
放電プラズマ焼結機としては、特に限定されず、YSZ粉末の加熱・冷却及び加圧が可能で、放電を起こすだけの電圧が印加できるものであれば良い。すなわち、加熱・冷却装置、加圧装置及び放電装置並びにYSZ粉末を収納する治具を備えた放電プラズマ焼結機を用いて、YSZ粉末を放電プラズマ焼結することが好ましい。治具としては、一般にグラファイトが好適である。放電プラズマ焼結機及びその作動原理等については、例えば特許第3007929号(公開特許公報:特開平10−251070(平成10年9月22日公開))を参照することができる。
【0029】
本発明の高密度YSZ焼結体の製造過程では、先ず、YSZ粉末を10〜60MPa、好ましくは10〜30MPaの圧力で加圧しつつ、500〜1500A、好ましくは700〜1100Aの直流パルス電流を用い、YSZ粉末を160〜170℃/minの昇温速度で1100〜1300℃、好ましくは1300℃に加熱する。その後、当該温度を保持しながら1〜30分間、好ましくは1〜10分間放電プラズマ焼結する。用いるパルス電流の周期は、特に限定されず、一般に300Hz〜30KHzの範囲から適宜選択することができる。
【0030】
本発明の高密度YSZ焼結体の製造方法は、前記した各条件を満たす製造方法であれば特に限定されないが、その中でも、特に1100〜1300℃の範囲から選択される加熱温度(℃)と1〜30分間(即ち1/60〜1/2時間)の範囲から選択される放電プラズマ焼結に係る保持時間(時間)との積(℃・時間)の値が20以上250以下であることが好ましい。積の値が20以上250以下である場合には、機械的強度が高く、且つ高温条件下においても導電率の経時的低下が抑制された高密度YSZ焼結体を短時間で安定に製造することができる。
【0031】
放電プラズマ焼結後は、パルス電流及び圧力印加を止め、焼結体を室温まで冷却した後に高密度YSZ焼結体を取り出すことが好ましい。
【0032】
なお、治具としてグラファイトを用いた場合には、得られる焼結体の表面近傍には、その成分であるグラファイトが含まれる場合がある。このような焼結体の表面近傍に含まれるグラファイトのような不純物は、焼結体表面を研磨又は加熱することにより、容易に取り除くことができる。焼結体表面を研磨する場合には、例えばダイヤモンド研磨盤を用いて研磨することが好ましい。焼結体表面を加熱する場合には、例えば通常の電気炉を用いて、空気中1000〜1300℃程度で1〜3時間程度加熱することが好ましい。
【0033】
【発明の効果】
本発明に係る高密度YSZ焼結体によれば、従来のYSZ焼結体と比較して、機械的強度が高く、且つ高温条件下(例えば、1000℃で1000時間)においても導電率の経時的低下が抑制されているので、SOFCの固体電解質をはじめ、様々な用途に使用することが可能である。
【0034】
本発明に係る高密度YSZ焼結体の製造方法によれば、機械的強度が高く、且つ高温条件下においても導電率の経時的低下が抑制された高密度YSZ焼結体を、従来法と比較して低温且つ短時間で安定に製造することが可能である。
【0035】
【実施例】
以下に実施例及び比較例を示し、本発明をより具体的に説明する。ただし、本発明はこれらの記載により限定されるものではない。
【0036】
実施例1
原料粉末としては、市販のYSZ粉末(商品名「TZ−8YS」東ソー株式会社製:Yを8mol%ドープしたZrO粉末、平均粒子径0.3μm、以下、「8YSZ」と記載する。)を用いた。放電プラズマ焼結機としては、(商品名「SPS−515S」株式会社イズミテック製)を用いた。また、治具としては、直径1.5cmの円筒形のグラファイト製治具を用いた。
【0037】
先ず、治具に8YSZ粉末1gを均一に入れ、30MPaの圧力を印加しつつ、焼結チャンバー内を7Paまで脱気した。次に、治具に1000Aの直流パルス電流を印加し、8YSZ粉末を160℃/minの昇温速度で1300℃まで加熱した。さらに、この状態で900Aの直流パルス電流を印加し、1分間放電プラズマ焼結を行った。焼結後は、電流及び圧力の印加を止め、焼結体を室温まで自然冷却し、高密度YSZ焼結体を得た。加熱温度と放電プラズマ焼結に係る保持時間との積(℃・時間)の値は21.6であった。
【0038】
得られた高密度YSZ焼結体は、X線回折より治具のグラファイトを含むことが分かった。高密度YSZ焼結体が治具のグラファイトを含むことは、エネルギー分散型X線分析(EDX)測定結果よりY、Zr、O以外にCが認められたことからも明らかであった。従って、高密度YSZ焼結体を1000℃で2時間熱処理を行い、Cを含まない高密度YSZ焼結体を得た(熱処理後の高密度YSZ焼結体は、X線回折では8YSZのピークのみが観測され、EDXよりCは測定されなかった)。以下、上記の方法で得た高密度YSZ焼結体(すなわち、1300℃で1分間放電プラズマ焼結して得た高密度YSZ焼結体)を特に「SPS焼結体」と記載した。
【0039】
得られたSPS焼結体の特性は、下記の通りであった。
【0040】
〔X線回折パターン〕
得られたSPS焼結体は、立法晶のX線回折パターンを示し、ピーク位置から求めた格子定数はa=0.51398(1)nm(0.51398±0.00001nmを表す(以下同様)。)であり、報告値a=0.5137nm(R.P.Ingel and D.LewisIII,J.Am.Ceram.Soc.,69,325(1986).)と良い一致を示した。
【0041】
〔かさ密度〕
得られたSPS焼結体のかさ密度は、図1に示した通り、5.9g/cmであった。これは理論密度(6g/cm)の98%であった。
【0042】
〔結晶組織〕
得られたSPS焼結体の結晶組織は、図2のSEM写真(b)に示した通り、サブミクロン粒子から構成されており、結晶の最大粒子径が2μm以下であり、且つ平均粒子径が1μm以下であった。顕微鏡観察で観察された粒子を球形近似することで算出した最大粒子径及び平均粒子径の値は、最大粒子径0.8μm、平均粒子径0.4μmであった。
【0043】
〔3点曲げ強度〕
得られたSPS焼結体の3点曲げ強度は、図3に示した通り、329MPaであった。この値は、報告されている8YSZ焼結体(約235MPa;O.Yamamoto,Y.Takeda,N.Imanishi,T.Kawahara,G.Q.Shen,M.Mori,and T.Abe,Proceedings of the Second International Symposium on Solid Oxide Fuel Cells,pp.437(1991).)の強度よりも高い値であった。
【0044】
〔交流導電率の経時的変化〕
得られたSPS焼結体を1000℃の温度下で1000時間保持した場合の初期の交流導電率σは0.18S/cmであり、報告されている8YSZの1000℃での初期の交流導電率(0.1S/cm;N.Q.Minh,J.Am.Ceram.Soc.,76,563(1993).)と同程度であった。交流導電率の経時的変化の結果を図4に示した。SPS焼結体は500時間以降、導電率の低下が減少し、1000時間以降は低下割合がかなり抑制された。
【0045】
比較例1
実施例1と同じYSZ粉末「8YSZ」を、従来用いられている外熱式電気炉を用いて2時間焼結(CS焼結)し、YSZ焼結体を製造した。YSZ焼結体は、焼結温度の違い(1200℃、1300℃、1400℃、1500℃及び1600℃)より、5種類を製造した。以下、当該5種類のYSZ焼結体を、特に「CS焼結体」と記載した。
【0046】
得られたCS焼結体の特性は、下記の通りであった。
【0047】
〔かさ密度〕
得られたCS焼結体のかさ密度は、図1に示した。例えば、1300℃、2時間焼結して得たCS焼結体のかさ密度は、4.1g/cm(理論密度の68%)であった。相対密度が98%以上になるのは、焼結温度が1600℃以上の場合であった。
【0048】
〔結晶組織〕
得られたCS焼結体の結晶組織は、例えば1600℃、2時間焼結したものは、図2のSEM写真(c)に示した通り、結晶の粒子径が数十μm以上に成長し、粒子界面が観察し難い組織であった。
【0049】
〔3点曲げ強度〕
得られたCS焼結体の3点曲げ強度は、例えば1600℃、2時間焼結のもので205MPaであった。3点曲げ強度の測定結果を図3に示した。
【0050】
〔交流導電率の経時的変化〕
得られたCS焼結体を1000℃の温度下で1000時間保持した場合の初期の交流導電率σは0.18S/cmであり、実施例1の値と同程度であった。交流導電率の経時的変化の結果を図4に示した。CS焼結体の交流導電率は、経時的に一定割合で低下した。
【0051】
実施例及び比較例の考察
図1(SPS焼結体及びCS焼結体のかさ密度の焼結温度依存性)によれば、本発明の製造方法では、従来の製造方法よりも、より低温且つ短時間で高密度YSZ焼結体を製造できると言える。
【0052】
図2(SPS焼結体及びCS焼結体の結晶組織)によれば、本発明の製造方法では、従来の製造方法よりも、より組織制御しながら(すなわち、粒子径成長を抑制しながら)高密度YSZ焼結体を製造できると言える。
【0053】
図3(SPS焼結体及びCS焼結体の3点曲げ強度の焼結温度依存性)によれば、本発明の製造方法では、従来の製造方法よりも、より機械的強度の高い高密度YSZ焼結体を製造できると言える。Hall−Petch式(H=H+kL−1/2;Hは強度、Lは粒子サイズ、H及びkは定数)によると、材料の強度は粒径の微細化により増大するが、本発明の製造方法においても、焼結体の結晶の粒子径成長を抑制して高密度化したために同様の強度増大が起こったものと考えられる。
【0054】
図4(SPS焼結体及びCS焼結体の交流導電率の経時的変化)によれば、SPS焼結体とCS焼結体では、1000℃における初期の導電率の値は同程度であるが、経時的な交流導電率の低下割合に違いがあることが分かる。CS焼結体の場合は、経時的に一定割合で交流導電率の低下が見られる。しかし、SPS焼結体の場合は、500時間経過後は、交流導電率の低下割合がかなり抑制されており、1000時間経過後は、CS焼結体の交流導電率を上回るようになる。導電率低下の原因として、高温・長時間の環境下、YSZ中の酸素欠損とY3+の複合体形成や酸素欠損の長周期配列による酸化物イオン導電の抑制が挙げられているが(J.Kondoh,S.Kikuchi,Y.Tomii,and Y.Ito,J.Electrochem.Soc.,145,1536(1998).)、SPS焼結体では、図2に示したように明瞭な粒界が存在するため、酸素欠損の長周期配列等がある程度抑制され、導電率の経時低下が抑制されたものと考えられる。従って、本発明の製造方法の方が、高温条件下においても、より導電率の経時低下が抑制された高密度YSZ焼結体を製造できると言える。
【0055】
(その他)
本発明の高密度YSZ焼結体の製造方法は、他の様々な電解質材料、例えばLaGaO系等にも適用可能であり、従来の電気炉等による外熱式焼結法に比べ、より低温且つ短時間で高強度且つ導電率低下の少ない高密度焼結体を作成することができる。
【図面の簡単な説明】
【図1】SPS焼結体及びCS焼結体のかさ密度の焼結温度依存性を示す図である。
【図2】(a)原料粉末、(b)SPS焼結体(1300℃、1分焼結)及びCS焼結体(1600℃、2時間焼結)の結晶組織をSEM写真によりあらわした図である。
【図3】SPS焼結体及びCS焼結体の3点曲げ強度の焼結温度依存性を示す図である。
【図4】SPS焼結体(1300℃、1分焼結)及びCS焼結体(1600℃、2時間焼結)を1000℃の温度下に保持したときの交流導電率の経時的変化を示す図である。
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a high-density yttria-stabilized zirconia sintered body and a method for producing the same. The high-density yttria-stabilized zirconia sintered body is useful, for example, as a solid electrolyte of a solid oxide fuel cell. Hereinafter, yttria-stabilized zirconia is described as “YSZ”.
[0002]
[Prior art]
A fuel cell is a fossil fuel / power conversion device expected to have higher efficiency than the existing thermal power generation, and among fuel cells, a device using a solid oxide as an electrolyte (solid oxide fuel cell: Solid Oxide Fuel Cell) (Hereinafter, abbreviated as "SOFC")) has attracted attention as having the highest energy conversion efficiency. As a solid oxide used for the electrolyte of the SOFC, for example, a YSZ sintered body is well known.
[0003]
However, when using a YSZ sintered body as the electrolyte of the SOFC, there is a problem in that when the YSZ sintered body is operated at 1000 ° C. or more for about 1000 hours or more, the power generation efficiency is reduced due to the deterioration of the YSZ sintered body. is there. The following can be considered as a cause of the high-temperature and long-time operation of the SOFC;
(1) cracking of the YSZ sintered body;
(2) that the ionic conductivity of the YSZ sintered body is reduced,
(3) The electrode reaction is suppressed by the progress of sintering of the electrode material, and (4) The formation of a low conductive layer by the progress of the solid phase reaction at the YSZ sintered body / electrode interface.
[0004]
In view of such a current situation, various attempts have been made to solve the above problem. For example, attempts have been made to add Al 2 O 3 , MgO, etc. to the composition of the YSZ sintered body in order to increase the mechanical strength.
[0005]
However, it has been reported that the addition of a different element increases the mechanical strength of the YSZ sintered body, but at the same time, lowers the conductivity of the YSZ sintered body (for example, LM Navarro, P.S. Recio, JR Jurado, and P. Duran, J. Mater. Sci., 30, 1949 (1995).). It has also been suggested that the added heterogeneous element may precipitate at the electrolyte grain boundaries as the SOFC is operated at a high temperature and for a long time, resulting in an increase in resistance and a decrease in the performance of the SOFC. In any case, current attempts have not largely solved the problems of the prior art.
[0006]
[Problems to be solved by the invention]
From the above viewpoints, there is a strong demand for the development of a high-density YSZ sintered body that has higher mechanical strength than conventional YSZ sintered bodies and that suppresses a decrease in conductivity over time even under high-temperature conditions. However, such a high-density YSZ sintered body has not yet been developed.
[0007]
Accordingly, an object of the present invention is to provide a high-density YSZ sintered body having particularly high mechanical strength and in which the decrease in conductivity over time is suppressed even under high-temperature conditions. It is another object of the present invention to provide a method for manufacturing a high-density YSZ sintered body.
[0008]
[Means for Solving the Problems]
The present inventor has conducted intensive studies to solve the problems of the prior art, and as a result, found that the following high-density YSZ sintered body and a method for producing the same achieve the above objects, and finally complete the present invention. Reached.
[0009]
The present invention relates to the following high-density YSZ sintered body and a method for producing the same.
[0010]
1. A high-density yttria-stabilized zirconia sintered body;
(1) The bulk density of the sintered body is 95% or more of the theoretical density,
(2) the maximum particle size of the sintered body is 2 μm or less, and the average particle size is 1 μm or less;
(3) When the room-temperature bending strength of the sintered body is 300 MPa or more, and (4) when the sintered body is held at a temperature of 1000 ° C. for 1000 hours, the conductivity σ after the lapse of 1000 hours with respect to the initial conductivity σ 0 A high-density yttria-stabilized zirconia sintered body, wherein the ratio of 10001000 / σ 0 ) is 0.68 or more.
[0011]
2. A ZrO 2 powder (yttria-stabilized zirconia) doped with 1 to 20 mol% of Y 2 O 3 is pressurized at a pressure of 10 to 60 MPa, and heated at a temperature of 160 to 170 ° C./min using a DC pulse current of 500 to 1500 A. A method for producing a high-density yttria-stabilized zirconia sintered body, comprising: performing heating at a rate of 1100 to 1300 ° C., followed by discharge plasma sintering for 1 to 30 minutes.
[0012]
3.1 Heating temperature (° C.) selected from 1100 to 1300 ° C. and holding time (hour) for spark plasma sintering selected from the range of 1 to 30 minutes (ie, 1/60 to 1/2 hour) 3. The method for producing a high-density yttria-stabilized zirconia sintered body according to the above item 2, wherein the product (° C. · time) of the product is 250 or less.
[0013]
BEST MODE FOR CARRYING OUT THE INVENTION
High density YSZ sintered body Hereinafter, the requirements (1) to (4) that the high density YSZ sintered body of the present invention should satisfy will be described in detail.
(1) The bulk density of the sintered body is 95% or more of the theoretical density.
[0014]
If the bulk density of the sintered body is less than 95% of the theoretical density (6 g / cm 3 ), the fracture energy of the sintered body with respect to external stress such as friction and impact becomes small, and the mechanical strength is reduced. In addition, since the porosity increases, for example, when used as a solid electrolyte of an SOFC, mixing of fuel gas and air occurs, and the power generation efficiency is significantly reduced. Therefore, the bulk density of the sintered body needs to be 95% or more of the theoretical density, and particularly preferably 98% or more.
(2) The maximum particle size of the sintered body is 2 μm or less, and the average particle size is 1 μm or less.
[0015]
Generally, as the particle size of the sintered body increases, wear due to grain detachment wear tends to occur, but also in the sintered body of the present invention, when the maximum particle size exceeds 2 μm, the stability of the cubic crystal is reduced. Become inferior. Therefore, for example, when this sintered body is used as a solid electrolyte of an SOFC, when the SOFC is maintained at an operating temperature of 1000 ° C. for 1,000 hours or more, the abundance ratio of cubic crystals decreases, and the abundance ratio of tetragonal crystals having low conductivity is reduced. Increase.
[0016]
Further, considering that the mechanical strength of ceramics is proportional to the reciprocal of the square root of the average particle diameter, and when the average particle diameter exceeds 1 μm, there is almost no difference in mechanical strength, and the average particle diameter is 1 μm. It is necessary that:
[0017]
As described above, the high-density YSZ sintered body of the present invention needs to have a maximum particle diameter of 2 μm or less and an average particle diameter of 1 μm or less. Among them, those having a maximum particle diameter of 1 μm or less and an average particle diameter of 0.5 μm or less are particularly preferred.
[0018]
In the present invention, the particle diameter refers to a diameter calculated by observing a high-density YSZ sintered body with a microscope and approximating the observed particles with a spherical shape. The average particle diameter is an average value of diameters calculated by the above-described spherical approximation.
(3) The room temperature bending strength of the sintered body is 300 MPa or more.
[0019]
Since the high-density YSZ sintered body of the present invention can be used as a high-temperature conductive material such as a solid electrolyte of a SOFC and a heat-resistant electrode, it can withstand thermal stress and thermal shock due to repeated temperature rise and fall and temperature distribution. It is necessary to have sufficient strength. Therefore, the room-temperature bending strength of the sintered body needs to be 300 MPa or more, and particularly preferably 320 MPa or more.
[0020]
In the present invention, the value of the room temperature bending strength is a value obtained by measuring the three-point bending strength of the high-density YSZ sintered body at room temperature. Specifically, according to the standard of JIS R1601, three-point bending was performed using a 3 × 4 mm square test piece whose four sides were finished with a diamond polishing machine of # 1000 under the conditions of a span of 30 mm and a load speed of 0.5 mm / min. It is a value of strength (at room temperature).
(4) In the case of holding for 1000 hours at a temperature of the sintered 1000 ° C., the ratio of the conductivity sigma 1000 after 1000 hours passed to the initial conductivity σ 0 (σ 1000 / σ 0 ) is 0.68 or more That.
[0021]
In the present invention, the conductivity is determined by shaving a high-density YSZ sintered body into a square rod shape, baking a platinum electrode and a platinum lead wire for voltage measurement at about 1000 ° C. (S / cm).
[0022]
The σ 0 of the high-density YSZ sintered body of the present invention is usually 0.1 S / cm. For example, when this sintered body is used as a solid electrolyte of an SOFC, the SOFC is operated at an operating temperature of 1000 ° C. for 1000 hours or more. If the conductivity is less than 0.068 S / cm when held, the power generation efficiency is reduced. Accordingly, high-density YSZ sintered body of the present invention requires that σ (0 σ 1000 / σ) ratio of sigma 1000 for 0 is 0.68 or more.
[0023]
Method for producing high-density YSZ sintered body Hereinafter, the method for producing a high-density YSZ sintered body of the present invention will be described in detail.
[0024]
The raw material powder is not particularly limited as long as it is a ZrO 2 powder (YSZ powder) doped with 1 to 20 mol% of Y 2 O 3, and a known or commercially available product can be used. The doping ratio of Y 2 O 3 can be appropriately set from 1 to 20 mol%, but is particularly preferably about 3 to 10 mol%.
[0025]
The method of preparing the YSZ powder is not particularly limited, and may be any synthesis method selected from a solid-phase reaction method, a hydrolysis method, a sol-gel method, a hydrothermal method, and the like. Although the particle size of the YSZ powder is not particularly limited, it is usually preferable that the particle size is submicron or smaller.
[0026]
In the present invention, the above-mentioned YSZ powder is subjected to spark plasma sintering under specific conditions, thereby sintering while suppressing the particle diameter growth of the sintered body, thereby obtaining a high-density YSZ sintered body. That is, a YSZ sintered body having a higher density than the YSZ powder as the raw material can be obtained.
[0027]
In the present invention, it is preferable to use a discharge plasma sintering machine for discharge plasma sintering of the YSZ powder. Using a sintering method based on ON-OFF pulse conduction such as discharge plasma sintering, discharge sintering, and electric sintering, the YSZ powder is compressed into a green compact, and a pulse current is applied to the green compact, It is preferable to perform compression sintering while controlling the temperature of the YSZ powder by controlling the peak current and the pulse width.
[0028]
The spark plasma sintering machine is not particularly limited as long as it can heat, cool and pressurize the YSZ powder and can apply a voltage sufficient to cause a discharge. That is, YSZ powder is preferably subjected to discharge plasma sintering using a discharge plasma sintering machine equipped with a heating / cooling device, a pressurizing device, a discharge device, and a jig for storing the YSZ powder. Generally, graphite is suitable as a jig. Regarding the spark plasma sintering machine and the operation principle thereof, for example, Japanese Patent No. 3007929 (Japanese Patent Laid-Open Publication No. Hei 10-25170 (published on September 22, 1998)) can be referred to.
[0029]
In the manufacturing process of the high-density YSZ sintered body of the present invention, first, while pressing the YSZ powder at a pressure of 10 to 60 MPa, preferably 10 to 30 MPa, a DC pulse current of 500 to 1500 A, preferably 700 to 1100 A is used. The YSZ powder is heated to 1100 to 1300 ° C., preferably 1300 ° C. at a rate of 160 to 170 ° C./min. Thereafter, discharge plasma sintering is performed for 1 to 30 minutes, preferably 1 to 10 minutes while maintaining the temperature. The period of the pulse current to be used is not particularly limited, and generally can be appropriately selected from a range of 300 Hz to 30 KHz.
[0030]
The method for producing the high-density YSZ sintered body of the present invention is not particularly limited as long as the production method satisfies the above-mentioned conditions, and among them, the heating temperature (° C.) particularly selected from the range of 1100 to 1300 ° C. The value of the product (° C. · hour) with the holding time (hour) related to spark plasma sintering selected from the range of 1 to 30 minutes (ie, 1/60 to 1/2 hour) is 20 or more and 250 or less. Is preferred. When the value of the product is 20 or more and 250 or less, a high-density YSZ sintered body having high mechanical strength and in which the decrease in conductivity over time is suppressed even under high temperature conditions is stably manufactured in a short time. be able to.
[0031]
After the discharge plasma sintering, it is preferable to stop the application of the pulse current and the pressure, cool the sintered body to room temperature, and then take out the high-density YSZ sintered body.
[0032]
When graphite is used as a jig, graphite, which is a component thereof, may be included in the vicinity of the surface of the obtained sintered body. Impurities such as graphite contained in the vicinity of the surface of such a sintered body can be easily removed by polishing or heating the surface of the sintered body. When polishing the surface of the sintered body, it is preferable to use a diamond polishing machine, for example. When the surface of the sintered body is heated, for example, it is preferable to heat it in air at about 1000 to 1300 ° C. for about 1 to 3 hours using a normal electric furnace.
[0033]
【The invention's effect】
According to the high-density YSZ sintered body of the present invention, the mechanical strength is higher than that of the conventional YSZ sintered body, and the conductivity of the YSZ sintered body under high temperature conditions (for example, 1000 hours at 1000 ° C.). Since the specific decrease is suppressed, it can be used for various applications including the solid electrolyte of the SOFC.
[0034]
According to the method for producing a high-density YSZ sintered body according to the present invention, a high-density YSZ sintered body having high mechanical strength and in which a decrease in conductivity over time is suppressed even under a high temperature condition is compared with a conventional method. It is possible to manufacture stably at a lower temperature and in a shorter time in comparison.
[0035]
【Example】
Hereinafter, the present invention will be described more specifically with reference to Examples and Comparative Examples. However, the present invention is not limited by these descriptions.
[0036]
Example 1
As the raw material powder, commercially available YSZ powder (trade name “TZ-8YS” manufactured by Tosoh Corporation: ZrO 2 powder doped with 8 mol% of Y 2 O 3 , average particle diameter 0.3 μm, hereinafter referred to as “8YSZ”) .) Was used. As the spark plasma sintering machine, (trade name "SPS-515S" manufactured by Izumi Tech Co., Ltd.) was used. As the jig, a cylindrical graphite jig having a diameter of 1.5 cm was used.
[0037]
First, 1 g of 8YSZ powder was uniformly placed in a jig, and the inside of the sintering chamber was evacuated to 7 Pa while applying a pressure of 30 MPa. Next, a DC pulse current of 1000 A was applied to the jig, and the 8YSZ powder was heated to 1300 ° C. at a rate of 160 ° C./min. Further, in this state, a DC pulse current of 900 A was applied, and discharge plasma sintering was performed for one minute. After sintering, the application of current and pressure was stopped, and the sintered body was naturally cooled to room temperature to obtain a high-density YSZ sintered body. The value of the product (° C. · hour) of the heating temperature and the holding time related to spark plasma sintering was 21.6.
[0038]
The obtained high-density YSZ sintered body was found by X-ray diffraction to contain graphite of a jig. The fact that the high-density YSZ sintered body contained the graphite of the jig was evident from the results of energy dispersive X-ray analysis (EDX) that C was recognized in addition to Y, Zr, and O. Therefore, the high-density YSZ sintered body was heat-treated at 1000 ° C. for 2 hours to obtain a high-density YSZ sintered body containing no C (the high-density YSZ sintered body after the heat treatment has a peak of 8 YSZ in X-ray diffraction). Only E was observed, and C was not measured by EDX). Hereinafter, the high-density YSZ sintered body obtained by the above method (that is, the high-density YSZ sintered body obtained by spark plasma sintering at 1300 ° C. for 1 minute) is particularly described as “SPS sintered body”.
[0039]
The characteristics of the obtained SPS sintered body were as follows.
[0040]
[X-ray diffraction pattern]
The obtained SPS sintered body shows an X-ray diffraction pattern of a cubic crystal, and the lattice constant obtained from the peak position is a = 0.51398 (1) nm (0.51398 ± 0.00001 nm (the same applies hereinafter)). ), Which is in good agreement with the reported value a = 0.5137 nm (RP Ingel and D. Lewis III, J. Am. Ceram. Soc., 69, 325 (1986).).
[0041]
[Bulk density]
The bulk density of the obtained SPS sintered body was 5.9 g / cm 3 as shown in FIG. This was 98% of the theoretical density (6 g / cm 3 ).
[0042]
(Crystal structure)
As shown in the SEM photograph (b) of FIG. 2, the crystal structure of the obtained SPS sintered body is composed of submicron particles, the maximum particle size of the crystal is 2 μm or less, and the average particle size is It was 1 μm or less. The values of the maximum particle diameter and the average particle diameter calculated by approximating the particles observed by a microscope to a sphere were a maximum particle diameter of 0.8 μm and an average particle diameter of 0.4 μm.
[0043]
[Three-point bending strength]
The three-point bending strength of the obtained SPS sintered body was 329 MPa as shown in FIG. This value is based on the reported 8YSZ sintered body (about 235 MPa; O. Yamamoto, Y. Takeda, N. Imanishi, T. Kawahara, GQ. Shen, M. Mori, and T. Abe, Proceedings of the The value was higher than the strength of Second International Symposium on Solid Oxide Fuel Cells, pp. 437 (1991).
[0044]
(Change over time in AC conductivity)
When the obtained SPS sintered body is held at a temperature of 1000 ° C. for 1000 hours, the initial AC conductivity σ 0 is 0.18 S / cm, and the reported initial AC conductivity of 8YSZ at 1000 ° C. Rate (0.1 S / cm; NQ Minh, J. Am. Ceram. Soc., 76, 563 (1993)). FIG. 4 shows the results of the change over time in the AC conductivity. After 500 hours, the decrease in conductivity of the SPS sintered body was reduced, and after 1000 hours, the rate of decrease was considerably suppressed.
[0045]
Comparative Example 1
The same YSZ powder “8YSZ” as in Example 1 was sintered (CS sintering) for 2 hours using a conventional external heating electric furnace to produce a YSZ sintered body. Five types of YSZ sintered bodies were manufactured based on differences in sintering temperatures (1200 ° C., 1300 ° C., 1400 ° C., 1500 ° C., and 1600 ° C.). Hereinafter, the five types of YSZ sintered bodies are particularly described as “CS sintered bodies”.
[0046]
The characteristics of the obtained CS sintered body were as follows.
[0047]
[Bulk density]
The bulk density of the obtained CS sintered body is shown in FIG. For example, the bulk density of a CS sintered body obtained by sintering at 1300 ° C. for 2 hours was 4.1 g / cm 3 (68% of the theoretical density). The relative density was 98% or more when the sintering temperature was 1600 ° C. or more.
[0048]
(Crystal structure)
The crystal structure of the obtained CS sintered body is, for example, sintered at 1600 ° C. for 2 hours, and as shown in the SEM photograph (c) of FIG. 2, the crystal grain size grows to several tens μm or more. The grain interface was a structure that was difficult to observe.
[0049]
[Three-point bending strength]
The three-point bending strength of the obtained CS sintered body was, for example, 205 MPa when sintered at 1600 ° C. for 2 hours. The measurement results of the three-point bending strength are shown in FIG.
[0050]
(Change over time in AC conductivity)
When the obtained CS sintered body was held at a temperature of 1000 ° C. for 1000 hours, the initial AC conductivity σ 0 was 0.18 S / cm, which was almost the same as the value of Example 1. FIG. 4 shows the results of the change over time in the AC conductivity. The AC conductivity of the CS sintered body decreased at a constant rate over time.
[0051]
Consideration of Examples and Comparative Examples According to FIG. 1 (sintering temperature dependence of bulk density of SPS sintered body and CS sintered body), the manufacturing method of the present invention is more effective than the conventional manufacturing method. It can be said that a high-density YSZ sintered body can be manufactured at a lower temperature and in a shorter time.
[0052]
According to FIG. 2 (crystal structures of the SPS sintered body and the CS sintered body), the manufacturing method of the present invention controls the structure more (that is, suppresses the particle diameter growth) than the conventional manufacturing method. It can be said that a high-density YSZ sintered body can be manufactured.
[0053]
According to FIG. 3 (the sintering temperature dependence of the three-point bending strength of the SPS sintered body and the CS sintered body), the manufacturing method of the present invention has a higher density with higher mechanical strength than the conventional manufacturing method. It can be said that a YSZ sintered body can be manufactured. According to the Hall-Petch equation (H = H 0 + kL −1/2 ; H is the strength, L is the particle size, H 0 and k are constants), the strength of the material increases with the refinement of the particle size. It is considered that the same increase in strength occurred in the production method described above because the growth of the crystal diameter of the sintered body was suppressed and the density was increased.
[0054]
According to FIG. 4 (time-dependent change in the AC conductivity of the SPS sintered body and the CS sintered body), the value of the initial conductivity at 1000 ° C. is substantially the same between the SPS sintered body and the CS sintered body. However, it can be seen that there is a difference in the rate of decrease in AC conductivity over time. In the case of a CS sintered body, a decrease in AC conductivity is observed at a constant rate over time. However, in the case of the SPS sintered body, the decrease rate of the AC conductivity is considerably suppressed after 500 hours, and exceeds the AC conductivity of the CS sintered body after 1000 hours. As the cause of the decrease in conductivity, formation of a complex of oxygen deficiency and Y 3+ in YSZ in a high-temperature and long-time environment and suppression of oxide ion conductivity due to a long-period arrangement of oxygen deficiency are mentioned (J. Kondoh, S. Kikuchi, Y. Tomii, and Y. Ito, J. Electrochem. Soc., 145, 1536 (1998)), and a clear grain boundary exists in the SPS sintered body as shown in FIG. Therefore, it is considered that the long-period arrangement and the like of oxygen deficiency were suppressed to some extent, and a decrease in conductivity over time was suppressed. Therefore, it can be said that the production method of the present invention can produce a high-density YSZ sintered body in which a decrease in conductivity over time is suppressed even under high-temperature conditions.
[0055]
(Other)
The method for producing a high-density YSZ sintered body of the present invention can be applied to various other electrolyte materials, for example, LaGaO 3 or the like, and has a lower temperature than a conventional external heat sintering method using an electric furnace or the like. In addition, a high-density sintered body having high strength and little decrease in conductivity can be produced in a short time.
[Brief description of the drawings]
FIG. 1 is a diagram showing the sintering temperature dependence of the bulk density of an SPS sintered body and a CS sintered body.
FIG. 2 is a SEM photograph showing the crystal structures of (a) raw material powder, (b) SPS sintered body (1300 ° C., 1 minute sintering) and CS sintered body (1600 ° C., 2 hour sintering). It is.
FIG. 3 is a diagram showing the sintering temperature dependence of the three-point bending strength of an SPS sintered body and a CS sintered body.
FIG. 4 shows the change over time of the AC conductivity when the SPS sintered body (1300 ° C., sintering for 1 minute) and the CS sintered body (1600 ° C., sintering for 2 hours) are maintained at a temperature of 1000 ° C. FIG.

Claims (2)

固体電解質型燃料電池の固体電解質として用いる高密度イットリア安定化ジルコニア焼結体であって;
(1)焼結体のかさ密度が理論密度の95%以上、
(2)焼結体の最大粒子径が2μm以下であり、且つ平均粒子径が1μm以下、
(3)焼結体の室温曲げ強度が300MPa以上、
(4)焼結体を1000℃の温度下で1000時間保持した場合において、初期の導電率σに対する1000時間経過後の導電率σ1000の割合(σ1000/σ)が0.68以上、及び
(5)焼結体の結晶相が立方晶
であることを特徴とする高密度イットリア安定化ジルコニア焼結体。
A high-density yttria-stabilized zirconia sintered body used as a solid electrolyte of a solid oxide fuel cell ;
(1) The bulk density of the sintered body is 95% or more of the theoretical density,
(2) the maximum particle size of the sintered body is 2 μm or less, and the average particle size is 1 μm or less;
(3) The sintered body has a room temperature bending strength of 300 MPa or more.
(4) In the case of holding for 1000 hours at a temperature of the sintered 1000 ° C., the ratio of the conductivity sigma 1000 after 1000 hours passed to the initial conductivity σ 0 (σ 1000 / σ 0 ) is 0.68 or more ,as well as
(5) A high-density yttria-stabilized zirconia sintered body characterized in that the crystal phase of the sintered body is cubic .
を1〜20mol%ドープしたZrO粉末(イットリア安定化ジルコニア)を10〜60MPaの圧力で加圧しつつ、500〜1500Aの直流パルス電流を用いて160〜170℃/minの昇温速度で1100〜1300℃に加熱した後、1〜30分間放電プラズマ焼結する高密度イットリア安定化ジルコニア焼結体の製造方法であって、1100〜1300℃の範囲から選択される加熱温度(℃)と1〜30分間(即ち1/60〜1/2時間)の範囲から選択される放電プラズマ焼結に係る保持時間(時間)との積(℃・時間)の値が20以上250以下であり、焼結体の結晶相が立方晶であり、焼結体の用途が固体電解質型燃料電池の固体電解質であることを特徴とする製造方法A ZrO 2 powder (yttria-stabilized zirconia) doped with 1 to 20 mol% of Y 2 O 3 is pressurized at a pressure of 10 to 60 MPa, and heated at a temperature of 160 to 170 ° C./min using a DC pulse current of 500 to 1500 A. This is a method for producing a high-density yttria-stabilized zirconia sintered body that is heated at a rate of 1100 to 1300 ° C. and then subjected to discharge plasma sintering for 1 to 30 minutes. ) And a holding time (hour) related to spark plasma sintering selected from the range of 1 to 30 minutes (that is, 1/60 to 1/2 hour) (° C. · hour) in the range of 20 to 250. A production method, wherein the crystal phase of the sintered body is cubic, and the use of the sintered body is a solid electrolyte of a solid oxide fuel cell .
JP2001057835A 2001-03-02 2001-03-02 High-density yttria-stabilized zirconia sintered body and method for producing the same Expired - Lifetime JP3603116B2 (en)

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