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JPS6160376B2 - - Google Patents
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JPS6160376B2 - - Google Patents

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Publication number
JPS6160376B2
JPS6160376B2 JP20393181A JP20393181A JPS6160376B2 JP S6160376 B2 JPS6160376 B2 JP S6160376B2 JP 20393181 A JP20393181 A JP 20393181A JP 20393181 A JP20393181 A JP 20393181A JP S6160376 B2 JPS6160376 B2 JP S6160376B2
Authority
JP
Japan
Prior art keywords
gas
detection element
change
resistance
temperature
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.)
Expired
Application number
JP20393181A
Other languages
Japanese (ja)
Other versions
JPS58105048A (en
Inventor
Masayuki Sakai
Taiji Kikuchi
Seiichi Nakatani
Yoshihiko Nakatani
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP56203931A priority Critical patent/JPS58105048A/en
Publication of JPS58105048A publication Critical patent/JPS58105048A/en
Publication of JPS6160376B2 publication Critical patent/JPS6160376B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/02Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance
    • G01N27/04Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance by investigating resistance
    • G01N27/12Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance by investigating resistance of a solid body in dependence upon absorption of a fluid; of a solid body in dependence upon reaction with a fluid, for detecting components in the fluid

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Electrochemistry (AREA)
  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は可燃性ガス検知素子、特に、長期間の
高温動作に対してきわめて安定な特性をもつ、半
導体式可燃性ガス検知素子およびその製造方法に
関するものである。 近年、ガス機器の普及に伴なつて、ガス漏れに
よる事故が多発し、これらの事故を防ぐ方法が
種々検討されている。従来から使用されているガ
ス検知素子の代表的なものの一つとして、n型の
金属酸化物半導体を用いたものが知られている。
半導体式ガス検知素子には通常速い応答速度を要
求されるので、ガス感応体は大気中で高温度に保
持されて用いられる。そのため、ガス感応体とし
ては酸化雰囲気に対して安定な酸化物が選ばれ
る。これまで各種の酸化物がガス感応体として用
いられてきたが、最近、酸化第二鉄のうち、これ
までガスに感じないとされていたコランダム型の
結晶構造を有するアルフア型酸化第二鉄(α―
Fe2O3)が優れた感ガス特性を示すことが見出さ
れ、これを感応体としたガス検知素子の検討が進
められている。 このα―Fe2O3を用いた場合のガスセンサは、
素子の温度が350〜450℃の範囲においてガス感応
特性が顕著であり、感度(通常空気中での抵抗値
Raと検知すべきガス濃度中での抵抗値Rgとの比
で表わされる)、および検知すべき濃度範囲にお
ける単位ガス濃度当たりの抵抗値の変化率が大き
いので、検知すべきガス濃度を定量度よく抵抗値
変化として検知できるという優れた特徴を持つて
いる。しかし、ガス検知素子のように、素子その
ものが外気に直接暴露され、過酷な条件下で使用
されるため、特に長期の課電寿命に対して不安定
になりやすく、常に精度よくガスを検知すること
が困難であつた。この理由としては、ガス感応体
は多孔質の焼結体か、あるいは基板上に形成され
た膜状の焼結体が用いられるが、常時高温度に保
持されることによる活性度の変化すなわち焼結に
よる粒成長および気孔率の低下等が考えられる。
これらは全て熱履歴による原因であると考えられ
るため、焼結防止用の添加物について種々検討を
行なつた結果、La2O3、Ce2O3、Pr2O3、Nd2O3
非常に効果的であることがわかつた。本発明はこ
の検討結果にもとづくものである。 ところで、一般にガスセンサにおいては、でき
るだけ少ない電力で感応体を効率よく加熱する必
要があるので、感応体はおのずと小さいものにな
る。セラミツク半導体式の場合も同様である。し
たがつて、特性などを改善する目的で添加した
種々の添加物が感応体に均一に含まれていない
と、素子間の特性ばらつきの原因となる。このた
め、製造法としては完全に均一な組成のものが得
られる溶液法(共沈法)が有力な方法となる。こ
れによると分散混合が優れているほかに、微粒子
粉体が得られるので、比表面積の増加すなわち高
活性化につながり、メタンなどの安定なガスに対
しても検知できる材料を得ることができるという
利点がある。また、微粒子粉体を中心に考える
と、鉄イオンを共沈させ、乾燥後にLa2O3
Ce2O3、Pr2O3、Nd2O3の少なくとも一種以上を
混合する方法も考えられる。 本発明は上述の事柄に鑑みてなされたもので、
以下その実施例について比較例と対比させて説明
する。 〔比較例 1〕 市販の塩化第二鉄(FeCl3・6H2O)30gと硫
酸第一鉄(FeSO4・7H2O)60gをそれぞれ1
の水に溶かし、80℃に保ちながら撹拌した。さら
に温度を80℃に保ちつつ、この溶液に8規定の水
酸化アンモニウム(NH4OH)溶液を60c.c./分の
割合で溶液の水素イオン濃度が7になるまで滴下
した。滴下終了後、10分間溶液の温度を60℃に保
持し、この共沈物を吸引過した。このようにし
て得られた粉体を減圧容器に入れて真空乾燥を行
なつた。得られた乾燥物をらいかい機で2時間粉
砕した後、有機バインダーを用いて100〜200μm
の大きさの粒子に整粒した。この粉体に2本の白
金線を埋め込んで、直径2mm、高さ3mmの円柱状
に加圧成型し、空気中において550℃で2時間の
焼成を行なつた。得られた多孔質の焼結体を検知
素子用ヘツダーにとりつけ、焼結体のまわりにコ
イル状のヒータを配置し、防爆用のステンレス鋼
網をかぶせて検知素子を得た。 第1図はガス検知素子の構造を示したものであ
る。図において、1は焼結体で、’2本の白金線
からなる電極3,4が埋め込まれている。2は焼
結体1を加熱するためのヒータで、ヒータ用ピン
11,12からヒータ用フレーム7,8を通じて
ヒータに電力が供給される。焼結体1の抵抗は電
極3,4からフレーム5,6を通じてピン9,1
0の間で測定されるよう構成されている。ヒータ
用ピン11,12およびピン9,10はヘツダー
13に固定され、スレンレス鋼製金網14はヘツ
ダーにとりつけられている。 以上のようにして得られた検知素子について、
ガス感応特性、通常使用温度(400℃)での課電
寿命および通常使用する温度よりもはるかに高い
温度(600℃)での過負荷課電寿命を調べた。 ガス感応特性の測定方法は、あらかじめ検知素
子のヒータ部に電流を流し、感応体の温度が400
℃になるように調整しておき、それを容積の知ら
れている測定箱内に挿入した後、柱射器でテスト
用ガスを測定箱内に注入し、焼結感応体の抵抗値
を測定した。通常課電寿命は、検知素子のヒータ
部に常に電流を流し感応体の温度を400℃に保持
し、経過時間とともに、上述の方法でガス感応特
性を測定し、CH4ガスとBガス(H265%とi―
C4H1035%との混合ガス)の抵抗経時変化率、す
なわち{初期の抵抗Rg(5000ppm)―t時間通
電後の抵抗Rg(5000ppm)}/初期の抵抗Rg
(5000ppm)の値ΔR/R(%)を求めた。過負
荷課電寿命については、感応体の温度を600℃に
保持し、経過時間とともに、上記した方法で測定
し、通常課電寿命と同じ方法で抵抗経時変化率を
求めた。初期ガス感応特性を後掲の第5表(試料
No.A)に、通常課電寿命におけるCH4に対する抵
抗変化率の推移を第2図に、またBガスに対する
それを第3図に、また過負荷課電寿命における
CH4に対する抵抗変化率の推移を第6図に、また
Bガスに対するそれを第7図にそれぞれ示した。
各図における試料No.はAである。 第5表および第2図、第3図、第6図、第7図
からわかることは、通常課電寿命および過負荷課
電寿命において、メタンガスに対しては抵抗が正
側すなわち劣化傾向に、Bガスに対しては負側す
なわち増感傾向に大幅に変化するため、このまま
では実際の警報器に取り付けて使用することは、
直接検知濃度の変化につながるので好ましくない
ことがわかる。 〔実施例 1〕 出発原料は市販の塩化第2鉄と硫酸第1鉄の配
合比を比較例1と同じように、1:2にし、焼結
酸化後に第1表〜第3表(試料No.B、C、E、
F、G、I、J、K、M、N、O、Q、R、S、
T、U、V)の組成になるように硝酸ランタン
(La(NO33・6H2O)、硝酸第1セリウム(Ce
(NO33・6H2O)、硝酸プラセオジム(Pr
(NO33・6E2O)および硝酸ネオジム(Nd
(NO33・6H2O)の配合量を変化させ、比較例1
と同様の方法で検知素子を作製し、同様の方法で
特性を評価した。 初期ガス感応特性を後掲の第5表、第6表(試
料No.C、G、K、O、R、S、T、U、V)に、
通常課電寿命におけるCH4に対する抵抗変化率の
推移を第2図(試料No.C、G、K、O)と第4図
(試料No.R、S、T、U、V)に、またBガスに
対するそれを第3図(試料No.C、G、K、O)と
第5図(試料No.R、S、T、U、V)に示した。
さらに過負荷課電寿命におけるCH4に対する抵抗
変化率の推移を第6図(試料No.C、G、K、O)
に、またBガスに対するそれを第7図(試料No.
C、G、K、O)にそれぞれ示した。 また、La(NO33・6H2O、Ce(NO33
6H2O、Pr(NO33・6H2OおよびNd(NO33
6H2O共沈量を変化させて作成した検知素子の
5000時間課電後(通常荷電寿命)の抵抗変化率を
第10〜13図に示す。 以上の結果より、焼結後のLa2O3、Ce2O3
Pr2O3およびNd2O3の形として、これより選ばれ
た少なくとも一種以上を総量で0.5〜20モル%含
ませることにより、通常使用温度からさらに高い
温度範囲において、その抵抗変化率は非常に安定
であることがわかる。 La2O3、Ce2O3、Pr2O3およびNd2O3が0.5モル
%未満のものは、図よりわかるように抵抗変化率
が大きいため、またLa2O3、Ce2O3、Pr2O3および
Nd2O3が20モル%より多くなるとメタンガス感度
が小さくなり、警報器の回路構成上実用に供せな
いのでこれ以上添加量を増加させるメリツトがな
ないので、いずれも実用的でない。これより、効
果的なLa2O3、Ce2O3、Pr2O3およびNd2O3量は焼
結後の感応体において0.5〜20モル%であること
がわかる。
The present invention relates to a combustible gas detection element, and particularly to a semiconductor type combustible gas detection element that has extremely stable characteristics against long-term high-temperature operation, and a method for manufacturing the same. In recent years, with the spread of gas appliances, accidents due to gas leaks have been occurring frequently, and various methods to prevent these accidents have been studied. 2. Description of the Related Art As one of the typical gas detection elements that have been used in the past, one using an n-type metal oxide semiconductor is known.
Since a semiconductor gas sensing element is normally required to have a fast response speed, the gas sensing element is used while being maintained at a high temperature in the atmosphere. Therefore, an oxide that is stable against an oxidizing atmosphere is selected as the gas sensitive material. Up until now, various oxides have been used as gas sensitive materials, but recently alpha-type ferric oxide (ferric oxide), which has a corundum-type crystal structure that was previously thought not to be sensitive to gases, has been introduced. α―
It has been discovered that Fe 2 O 3 ) exhibits excellent gas-sensitive properties, and studies are underway to develop gas sensing elements using this as a sensitive material. A gas sensor using this α-Fe 2 O 3 is
The gas sensitivity characteristics are remarkable when the temperature of the element is in the range of 350 to 450℃, and the sensitivity (resistance value in normal air)
Ra and the resistance value Rg in the gas concentration to be detected), and the rate of change in the resistance value per unit gas concentration in the concentration range to be detected is large, so the gas concentration to be detected can be determined with a quantitative degree. It has the excellent feature that it can be easily detected as a change in resistance value. However, like gas detection elements, the elements themselves are directly exposed to the outside air and used under harsh conditions, so they tend to become unstable, especially over long energized lifespans, making it difficult to always accurately detect gases. It was difficult. The reason for this is that the gas sensitive material is either a porous sintered material or a film-like sintered material formed on a substrate, but the activity changes due to being constantly held at a high temperature. Possible causes include grain growth and a decrease in porosity due to condensation.
All of these are thought to be caused by thermal history, and as a result of various studies on additives to prevent sintering, we found that La 2 O 3 , Ce 2 O 3 , Pr 2 O 3 , and Nd 2 O 3 It turned out to be very effective. The present invention is based on the results of this study. By the way, in general, in gas sensors, it is necessary to efficiently heat the sensitive body with as little electric power as possible, so the sensitive body naturally becomes small. The same applies to the ceramic semiconductor type. Therefore, if the various additives added for the purpose of improving characteristics etc. are not uniformly contained in the sensitive body, it will cause variations in characteristics between elements. For this reason, a solution method (co-precipitation method) is an effective manufacturing method because it provides a completely uniform composition. According to this method, in addition to excellent dispersive mixing, fine particle powder can be obtained, which leads to an increase in specific surface area, that is, high activation, and it is possible to obtain a material that can detect even stable gases such as methane. There are advantages. In addition, when focusing on fine particle powder, iron ions are co-precipitated, and after drying, La 2 O 3 ,
A method of mixing at least one of Ce 2 O 3 , Pr 2 O 3 , and Nd 2 O 3 is also considered. The present invention has been made in view of the above-mentioned matters,
Examples will be described below in comparison with comparative examples. [Comparative Example 1] 30 g of commercially available ferric chloride (FeCl 3 6H 2 O) and 60 g of ferrous sulfate (FeSO 4 7H 2 O) were each
of water and stirred while maintaining the temperature at 80°C. Further, while maintaining the temperature at 80° C., an 8N ammonium hydroxide (NH 4 OH) solution was added dropwise to this solution at a rate of 60 c.c./min until the hydrogen ion concentration of the solution reached 7. After the dropwise addition was completed, the temperature of the solution was maintained at 60° C. for 10 minutes, and the coprecipitate was filtered off by suction. The powder thus obtained was placed in a vacuum container and vacuum dried. After pulverizing the obtained dried material for 2 hours using a grinder, it is pulverized to 100 to 200 μm using an organic binder.
The particles were sized to . Two platinum wires were embedded in this powder, which was then pressure-molded into a cylindrical shape with a diameter of 2 mm and a height of 3 mm, and fired at 550° C. for 2 hours in air. The obtained porous sintered body was attached to a sensing element header, a coil-shaped heater was placed around the sintered body, and an explosion-proof stainless steel net was covered to obtain a sensing element. FIG. 1 shows the structure of the gas detection element. In the figure, 1 is a sintered body in which electrodes 3 and 4 made of two platinum wires are embedded. Reference numeral 2 denotes a heater for heating the sintered body 1, and power is supplied to the heater from heater pins 11 and 12 through heater frames 7 and 8. The resistance of the sintered body 1 is measured from the electrodes 3 and 4 through the frames 5 and 6 to the pins 9 and 1.
It is configured to be measured between 0 and 0. Heater pins 11, 12 and pins 9, 10 are fixed to a header 13, and a stainless steel wire mesh 14 is attached to the header. Regarding the sensing element obtained as above,
We investigated the gas sensitivity characteristics, the energized life at normal operating temperature (400°C), and the overload energized life at a temperature much higher than the normal operating temperature (600°C). To measure the gas sensitivity characteristics, a current is applied to the heater part of the sensing element in advance, and the temperature of the sensing element is set to 400°C.
℃, insert it into a measurement box with a known volume, and then inject test gas into the measurement box with a pillar gun to measure the resistance of the sintered sensitizer. did. Normal energization life is determined by constantly passing current through the heater part of the sensing element to maintain the temperature of the sensing element at 400°C, and measuring the gas sensitivity characteristics using the method described above over time. CH 4 gas and B gas (H 2 65% and i-
C 4 H 10 (mixed gas with 35%), the rate of change in resistance over time, that is, {initial resistance Rg (5000ppm) - resistance Rg after t hours of energization (5000ppm)}/initial resistance Rg
The value ΔR/R (%) of (5000 ppm) was determined. Regarding the overload energization life, the temperature of the sensitive body was maintained at 600° C., and the temperature was measured with the above-mentioned method over time, and the rate of change in resistance over time was determined using the same method as for the normal energization life. The initial gas sensitivity characteristics are shown in Table 5 below (sample
No. A), Figure 2 shows the change in resistance change rate for CH 4 during normal energized life, Figure 3 shows that for B gas, and overloaded energized life.
The change in resistance change rate for CH 4 is shown in FIG. 6, and that for B gas is shown in FIG. 7.
The sample number in each figure is A. What can be seen from Table 5 and Figures 2, 3, 6, and 7 is that during normal energization life and overload energization life, the resistance to methane gas is on the positive side, that is, it tends to deteriorate; For B gas, there is a significant change in the negative side, that is, a sensitization tendency, so it is impossible to use it by attaching it to an actual alarm device as it is.
It can be seen that this is not desirable because it directly leads to a change in the detected concentration. [Example 1] The starting materials were commercially available ferric chloride and ferrous sulfate with a mixing ratio of 1:2, as in Comparative Example 1, and after sintering and oxidation, the materials shown in Tables 1 to 3 (Sample No. .B, C, E,
F, G, I, J, K, M, N, O, Q, R, S,
Lanthanum nitrate (La(NO 3 ) 3・6H 2 O) and ceric nitrate (Ce
(NO 3 ) 3・6H 2 O), praseodymium nitrate (Pr
(NO 3 ) 3・6E 2 O) and neodymium nitrate (Nd
Comparative Example 1
A sensing element was prepared in the same manner as above, and its characteristics were evaluated in the same manner. The initial gas sensitivity characteristics are shown in Tables 5 and 6 (sample Nos. C, G, K, O, R, S, T, U, V) below.
The transition of the resistance change rate with respect to CH 4 during the normal energized life is shown in Figure 2 (Sample No. C, G, K, O) and Figure 4 (Sample No. R, S, T, U, V). The values for B gas are shown in Fig. 3 (Sample No. C, G, K, O) and Fig. 5 (Sample No. R, S, T, U, V).
Furthermore, Fig. 6 shows the change in resistance change rate with respect to CH 4 during the life of overload application (sample Nos. C, G, K, O).
In addition, it is shown in Fig. 7 (Sample No.
C, G, K, O) respectively. Also, La(NO 3 ) 3・6H 2 O, Ce(NO 3 ) 3
6H 2 O, Pr(NO 3 ) 3・6H 2 O and Nd(NO 3 ) 3
Detection elements created by varying the amount of 6H 2 O co-precipitation
The rate of change in resistance after 5000 hours of charging (normal charging life) is shown in Figures 10 to 13. From the above results, after sintering La 2 O 3 , Ce 2 O 3 ,
By containing 0.5 to 20 mol% of at least one selected from Pr 2 O 3 and Nd 2 O 3 in the form of Pr 2 O 3 and Nd 2 O 3, the rate of change in resistance is extremely high in the temperature range higher than the normal usage temperature. It can be seen that it is stable. As can be seen from the figure, those containing less than 0.5 mol % of La 2 O 3 , Ce 2 O 3 , Pr 2 O 3 and Nd 2 O 3 have a large rate of change in resistance; , Pr 2 O 3 and
If Nd 2 O 3 exceeds 20 mol %, the sensitivity to methane gas decreases, making it impractical due to the circuit configuration of the alarm, and there is no advantage in increasing the amount added any further, so neither is practical. From this, it can be seen that the effective amounts of La 2 O 3 , Ce 2 O 3 , Pr 2 O 3 and Nd 2 O 3 in the sintered sensitive body are 0.5 to 20 mol %.

【表】【table】

【表】【table】

【表】【table】

【表】【table】

【表】【table】

【表】【table】

〔比較例 2〕[Comparative example 2]

市販のα―Fe2O3とLa2O3、Ce2O3、Pr2O3およ
びNd2O3を第4表(試料No.X、Y、Z)に示した
ように配合し、実施例1と同様の方法で混合粉砕
から焼成まで行ない、検知素子を作製した。特性
評価も同様の方法で行なつた。初期ガス感応特性
は第6表(試料No.X)に示すように、ガス感度が
非常に小さく、実用上使用できないものであつ
た。このことから、α―Fe2O3をガス感応体とす
る場合には共沈法による微粒子化が必要であると
いうことがわかる。 なお、実施例においては成型体を焼結した検知
素子の感応体について説明したが、この焼結体原
料をペースト化して基板上に塗布し、焼きつけて
感応体を得ることも可能である。 原料塩については塩化第2鉄、硫酸第1鉄およ
び硝酸ランタン、硝酸第1セリウム、硝酸プラセ
オジム、硝酸ネオジムを用いて説明したが、これ
に限らず水に溶解する鉄、ランタン、セリウム、
プラセオジムおよびネオジムの塩であるならば全
て有効である。 また、実施例において550℃で焼成を行なつた
が、この温度に限らず実用上耐えうる焼結体強度
を持つ焼成温度であればよい。 以上詳細に述べたように、本発明の素子はα―
Fe2O3とLa2O3、Ce2O3、Pr2O3およびNd2O3の少
なくとも一種以上を含有させているので、長期間
の高温動作に対し、きわめて安定な特性を維持す
ることのできるものである。これによつて、特性
の変動が著しく小さくなり、非常に信頼性のよい
可燃性ガス検知器を実現することができる。
Commercially available α-Fe 2 O 3 and La 2 O 3 , Ce 2 O 3 , Pr 2 O 3 and Nd 2 O 3 were blended as shown in Table 4 (Sample Nos. X, Y, Z), A sensing element was produced by carrying out the steps from mixing and pulverizing to baking in the same manner as in Example 1. Characteristic evaluation was also performed in the same manner. As shown in Table 6 (Sample No. X), the initial gas sensitivity was so low that it could not be used practically. From this, it can be seen that when α-Fe 2 O 3 is used as a gas sensitive material, it is necessary to make it into fine particles by a coprecipitation method. In the embodiment, the sensitive body of the sensing element was explained by sintering the molded body, but it is also possible to obtain the sensitive body by making a paste of this sintered body raw material, applying it onto a substrate, and baking it. The raw material salts have been explained using ferric chloride, ferrous sulfate, lanthanum nitrate, ceric nitrate, praseodymium nitrate, and neodymium nitrate, but are not limited to these, but include water-soluble iron, lanthanum, cerium,
All praseodymium and neodymium salts are effective. Furthermore, although firing was performed at 550° C. in the examples, the firing temperature is not limited to this temperature, and any firing temperature that provides a strength of the sintered body that can withstand practical use may be used. As described in detail above, the element of the present invention has α-
Contains Fe 2 O 3 and at least one of La 2 O 3 , Ce 2 O 3 , Pr 2 O 3 and Nd 2 O 3 , so it maintains extremely stable characteristics even during long-term high temperature operation. It is something that can be done. As a result, variations in characteristics are significantly reduced, making it possible to realize a highly reliable combustible gas detector.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明にかかる可燃性ガス検知素子の
構造の一例を示す正面図、第2図、第4図、第8
図は通常課電寿命におけるメタンガス5000ppm
雰囲気中の本発明の一実施例のガス検知素子の抵
抗値の初期値に対する変化率の推移を示す図、第
3図、第5図、第9図は通常課電寿命におけるB
ガス雰囲気中の抵抗値の変化率を示した図、第6
図は過負荷課電寿命におけるメタンガス雰囲気中
の抵抗値の変化率を示した図、第7図は過負荷課
電寿命におけるBガス雰囲気中の抵抗値の変化率
を示す図、第10図、第11図、第12図および
第13図は本発明の実施例のガス検知素子におけ
る通常課電5000時間後のLe2O3量、Ce2O3量、
Pr2O3量およびNd2O3量と抵抗変化率との関係を
示す図である。 1…焼結体、2…ヒータ、3,4…電極、5,
6,7,8…フレーム、9,10…電極用ピン、
11,12…ヒータ用ピン、13…ベース、14
…ステンレス製金網。
FIG. 1 is a front view showing an example of the structure of a combustible gas detection element according to the present invention, FIG. 2, FIG. 4, and FIG.
The figure shows 5000ppm of methane gas during normal energized life.
Figures 3, 5, and 9 are diagrams showing changes in the rate of change of the resistance value of a gas detection element according to an embodiment of the present invention in an atmosphere with respect to its initial value.
Figure 6 showing the rate of change in resistance value in a gas atmosphere
The figure shows the rate of change in the resistance value in a methane gas atmosphere during the life of overload energization, Figure 7 shows the rate of change of the resistance value in a B gas atmosphere during the life of overload energization, and Figure 10. FIGS. 11, 12, and 13 show the amount of Le 2 O 3 , amount of Ce 2 O 3 ,
FIG. 3 is a diagram showing the relationship between the amount of Pr 2 O 3 and the amount of Nd 2 O 3 and the rate of change in resistance. 1... Sintered body, 2... Heater, 3, 4... Electrode, 5,
6, 7, 8... Frame, 9, 10... Electrode pin,
11, 12... Heater pin, 13... Base, 14
...Stainless steel wire mesh.

Claims (1)

【特許請求の範囲】 1 共沈法により作成したアルフア型酸化第2鉄
(α―Fe2O3)を99.5〜80モル%含み、かつランタ
ン(La)、セリウム(Ce)、プラセオジム(Pr)
ならびにネオジム(Nd)の4種の酸化物から選
ばれた少なくとも一種が添加総量で0.5〜20モル
%の割合で含まれていることを特徴とする可燃性
ガス検知素子。 2 鉄イオンの他に、ランタン、セリウム、プラ
セオジムならびにネオジム各イオンの少なくとも
一種以上を共沈させて、ガス感応体原料を作り、
それを焼成することによつて、検知素子を得るこ
とを特徴とする可燃性ガス検知素子の製造方法。 3 鉄イオンを共沈させて、それによつて得られ
るα―Fe2O3にランタン、セリウム、プラセオジ
ムならびにネオジムの酸化物の少なくとも一種以
上を混合し、ガス感応体原料を得、されに焼成す
ることによつて検知素子を得ることを特徴とする
可燃性ガス検知素子の製造方法。
[Claims] 1. Contains 99.5 to 80 mol% of alpha-type ferric oxide (α-Fe 2 O 3 ) prepared by a coprecipitation method, and contains lanthanum (La), cerium (Ce), and praseodymium (Pr).
and at least one selected from four types of oxides of neodymium (Nd) in a total amount of 0.5 to 20 mol%. 2. In addition to iron ions, at least one of lanthanum, cerium, praseodymium, and neodymium ions is co-precipitated to produce a gas sensitizer raw material;
A method for producing a combustible gas detection element, the method comprising obtaining a detection element by firing the combustible gas detection element. 3 Co-precipitate iron ions and mix at least one of the oxides of lanthanum, cerium, praseodymium, and neodymium with the resulting α-Fe 2 O 3 to obtain a raw material for a gas sensitizer, and then sinter it. 1. A method for producing a combustible gas detection element, characterized in that the detection element is obtained by:
JP56203931A 1981-12-17 1981-12-17 Combustible gas detection element and its manufacturing method Granted JPS58105048A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56203931A JPS58105048A (en) 1981-12-17 1981-12-17 Combustible gas detection element and its manufacturing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56203931A JPS58105048A (en) 1981-12-17 1981-12-17 Combustible gas detection element and its manufacturing method

Publications (2)

Publication Number Publication Date
JPS58105048A JPS58105048A (en) 1983-06-22
JPS6160376B2 true JPS6160376B2 (en) 1986-12-20

Family

ID=16482059

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56203931A Granted JPS58105048A (en) 1981-12-17 1981-12-17 Combustible gas detection element and its manufacturing method

Country Status (1)

Country Link
JP (1) JPS58105048A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60155957A (en) * 1984-01-26 1985-08-16 Yamatake Honeywell Co Ltd Nitrogen oxide detecting element

Also Published As

Publication number Publication date
JPS58105048A (en) 1983-06-22

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