JPS6045369B2 - Flammable gas detection element - Google Patents
Flammable gas detection elementInfo
- Publication number
- JPS6045369B2 JPS6045369B2 JP52118243A JP11824377A JPS6045369B2 JP S6045369 B2 JPS6045369 B2 JP S6045369B2 JP 52118243 A JP52118243 A JP 52118243A JP 11824377 A JP11824377 A JP 11824377A JP S6045369 B2 JPS6045369 B2 JP S6045369B2
- Authority
- JP
- Japan
- Prior art keywords
- gas
- gas detection
- detection element
- al2o3
- concentration
- 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
Links
Landscapes
- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
- Non-Adjustable Resistors (AREA)
Description
【発明の詳細な説明】
本発明は可燃性ガス検出素子にかかり、可燃性ガスすな
わち還元性ガスに感応して大きな抵抗変化比を示し、か
つ長期課電寿命特性の優れた素子を提供しようとするも
のである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a combustible gas detection element, and an object thereof is to provide an element that exhibits a large resistance change ratio in response to combustible gas, that is, a reducing gas, and has excellent long-term energized life characteristics. It is something to do.
近年、ガス機器の普及に伴つて、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各種検討されてきて
いる。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.
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
1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。しかし、これは、実用上、単位ガス濃度変
化に対する電気抵抗値の変化率が小さく、検知濃度の定
量性の欠けたり、あるいは長期の課電寿命特性が十分で
なかつたりして、必ずしも十分満足できるものでない。
一方、最近、酸化第二鉄のうち、スピネル型の結晶構造
を有するガンマ型酸化第二鉄に 八、L゛l宵」−L−
よ・・ 1杜、 f、■、−A−、L−I−1く目出
され、これを感応体としたガス検知素子の開発が進めら
れている。ところで、酸化第二鉄には種々の結晶構造の
ものがあり、化学的にも物理的にもそれぞれまつたく異
なつた性質を有しており、結晶構造を指定していない限
り、酸化第二鉄の物性を語ることができない。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. However, in practice, this is not always fully satisfactory because the rate of change in electrical resistance with respect to a unit change in gas concentration is small, the detected concentration lacks quantification, or the long-term energized life characteristics are insufficient. It's not something.
On the other hand, recently, among ferric oxides, gamma-type ferric oxide, which has a spinel-type crystal structure, has been developed.
1 Mori, f, ■, -A-, and L-I-1 have been identified, and development of gas detection elements using them as sensitive bodies is progressing. By the way, ferric oxide has various crystal structures, each with completely different chemical and physical properties, so unless the crystal structure is specified, ferric oxide cannot talk about the physical properties of
その中でも、もつともよく知られているのは、コラング
ム型の結晶構造のアルファ型酸化第二鉄(α−Fe。O
。)てある。そのほかに、本発明に用いられるγ−Fe
。O。、さらに製造法、結晶構造はあまり明らかではな
いが、ベータ型酸化第二鉄(β−Fe2O。)、デルタ
型酸化第二鉄(δ−Fe。O。)などの存在が報告され
ている。しかし、これらの各種の結晶構造をもつ酸化第
二鉄のうちで、実用可能なガス感応特性を示すのは、γ
−Fe。03のみである。Among them, the most well-known is alpha-type ferric oxide (α-Fe.O
. ). In addition, γ-Fe used in the present invention
. O. Furthermore, although the manufacturing method and crystal structure are not very clear, the existence of beta-type ferric oxide (β-Fe2O.), delta-type ferric oxide (δ-Fe.O.), etc. has been reported. However, among these ferric oxides with various crystal structures, only γ shows practical gas sensitivity characteristics.
-Fe. 03 only.
このγ−Fe。This γ-Fe.
O。を用いた場合のガス感応特性は素子の温度が300
〜4000Cの範囲にあるときに大きく、その中でも、
感度(通常空気中での抵抗値フRaと検知すべきガス濃
度中での抵抗値Rgとの比て表わされる)がもつとも大
きくなるのは、約350゜Cのときである。ところで、
ガス検知素子として実用上重要なことは、いわゆる上述
の感度よりも、検知すべき濃度範囲における、単位ガス
濃ク度当たりの抵抗値の変化率(以後これを抵抗変化比
と言う)がいかに大きいかということである。換言すれ
ば、検知すべきガス濃度範囲において、その濃度をいか
に定量度よく抵抗値変化とし検知できるかということで
ある。また、ガス検知素子のように、素子そのものが外
気に暴露され、過酪な条件下で使用されるようないわゆ
る雰囲気センサは多かれ少なかれ、製造直後、エージン
グという工程を経なければならない。これは、素子製造
上、生産面から言つてもコスト面からも、できれば省略
したい工程である。これには素子そのものが製造直後か
ら長期間にわたつて安定した特性を維持することが必要
である。本発明による素子は、基本的にはγ−Fe2O
3とγ−Al2O3とで構成されるものであつて、抵抗
変化比が大きく、したがつてガス濃度検知の定量性がよ
く、かつ製造直後から長期間にわたつてきわめて安定し
た課電寿命特性を発揮するものである。O. The gas sensitivity characteristics when using
It is large when it is in the range of ~4000C, and among them,
Sensitivity (normally expressed as the ratio of the resistance value F Ra in air to the resistance value Rg in the gas concentration to be detected) becomes large at about 350°C. by the way,
What is practically important for a gas detection element, rather than the above-mentioned sensitivity, is how large the rate of change in resistance per unit gas concentration (hereinafter referred to as resistance change ratio) is in the concentration range to be detected. That is to say. In other words, in the gas concentration range to be detected, how can the concentration be quantitatively detected as a change in resistance value? In addition, so-called atmosphere sensors such as gas detection elements, in which the elements themselves are exposed to the outside air and are used under harsh conditions, must undergo an aging process more or less immediately after manufacture. This is a step that should be omitted if possible from the standpoint of device manufacturing, production, and cost. This requires that the element itself maintain stable characteristics over a long period of time immediately after manufacture. The device according to the invention basically consists of γ-Fe2O
It is composed of 3 and γ-Al2O3, and has a large resistance change ratio, so it has good quantitative gas concentration detection, and has extremely stable energized life characteristics over a long period of time immediately after manufacture. It is something that can be demonstrated.
以下に、実施例をあげて具体的な特性について述べる。Below, specific characteristics will be described using examples.
実施例1平均粒径0.2μmの四三酸化鉄(Fe3O4
)粉末を0.7モル、およびγ−Al2O3粉末を0.
3モル秤取して、水を加えて、ステンレススチールポッ
ト内でステンレススチールボールを用いて、湿式混合す
るとともに粉砕した。Example 1 Triiron tetroxide (Fe3O4) with an average particle size of 0.2 μm
) powder and 0.7 mol of γ-Al2O3 powder.
Three moles were weighed out, water was added, and wet mixed and ground using stainless steel balls in a stainless steel pot.
この混合物を80℃の温度で真空、乾燥させ、得られた
粉体を700′Cの温度で真空中て焼成した。この焼成
分に、トリエタノールアミンを加えて、ペースト化した
。一方、ガス検知素子の基板として縦、横それぞれ5T
T0n1厚み。0.5Tr$Lのアルミナ基板を用意し
、この表面に0.5TWLの間隔に金ペーストを印加し
焼付けして櫛形電極を形成し、表面には金電極の間に市
販の酸化ルテニウムのグレーズ抵抗を印刷し、焼付けて
ヒータとした。The mixture was dried in vacuo at a temperature of 80°C and the resulting powder was calcined in vacuo at a temperature of 700'C. Triethanolamine was added to the baked ingredients to form a paste. On the other hand, the substrate for the gas detection element is 5T each in the vertical and horizontal directions.
T0n1 thickness. A 0.5Tr$L alumina substrate was prepared, and gold paste was applied to the surface at intervals of 0.5TWL and baked to form comb-shaped electrodes.A commercially available ruthenium oxide glaze resistor was placed between the gold electrodes on the surface. was printed and baked to make a heater.
次に、上述のペーストを、基板の表面約J7Oμmの厚
みに印刷し、室温で自然乾燥した後、400゜Cの温度
で1時間、通常空気中で焼付けた。この段階で主成分で
あるFe3O4は酸化されてγ−Fe2O3になり、同
時にペースト中の溶剤が蒸発して、実用上十分な機械的
強度を有する焼結膜とな・つた。このようにして得られ
たガス感応体の厚みは約50P7TLであつた。素子の
動作温度はヒータ部に電流を通じ、その電流値を調節し
て制御した。Next, the paste described above was printed on the surface of the substrate to a thickness of about J70 μm, air-dried at room temperature, and then baked at a temperature of 400° C. for 1 hour, usually in air. At this stage, the main component Fe3O4 was oxidized to γ-Fe2O3, and at the same time the solvent in the paste evaporated to form a sintered film with sufficient mechanical strength for practical use. The thickness of the gas sensitive body thus obtained was approximately 50P7TL. The operating temperature of the device was controlled by passing a current through the heater section and adjusting the current value.
空気中における抵抗値(Ra)は、乾燥した空気が乱流
を生じない程度にゆつくり攪拌されている容積50eの
測定容器中で測定し、ガス中の抵抗値(Rg)はこの容
器の中に純度99%以上のイソブタンガスを体積%にし
て10ppm/秒の割合で流入し、その濃度が0.05
%および0.5%に達したときにそれぞれ測定した。測
定するガス濃度を0.05%および0.5%としたのは
、イソブタンガスの爆発下限界(LEL)約2%の、数
1紛の1から数分の1の範囲の濃度フを検知するのが、
可燃性ガス検知素子として実用上必要であるからである
。上述のようにして得られた製造直後の素子のヒータに
通電して素子温度を350℃に保持して、ガス感応特性
を測定した。その結果、Raは780KΩ、Rg(0.
05%)は220K7Ω、Rg(0.5%)は浸区Ωで
あつた。すなわち、0.05%と0.5%のガス濃度領
域の抵抗変化比は5.79である。この値は従来の半導
体式のガス検知素子で見られなかつた大きい値である。
ところで、この検知素子ではイソブタンガスのJO.O
5〜0.5%濃度範囲において、感応体の抵抗値Rgは
、ガス濃度をCとしたとき、C−1に比例するという関
係がある。The resistance value (Ra) in air is measured in a measurement container with a volume of 50e in which dry air is stirred slowly to the extent that no turbulence occurs. Isobutane gas with a purity of 99% or more flows at a rate of 10 ppm/sec by volume, and its concentration is 0.05
% and 0.5%, respectively. The gas concentrations to be measured were set to 0.05% and 0.5% to detect concentrations ranging from 1 to a fraction of the lower explosive limit (LEL) of isobutane gas, which is approximately 2%. What you do is
This is because it is practically necessary as a combustible gas detection element. Gas sensitivity characteristics were measured by energizing the heater of the element obtained as described above immediately after manufacture to maintain the element temperature at 350°C. As a result, Ra was 780KΩ, Rg(0.
05%) was 220K7Ω, and Rg (0.5%) was the immersion area Ω. That is, the resistance change ratio between the gas concentration regions of 0.05% and 0.5% is 5.79. This value is a large value that has not been seen in conventional semiconductor gas sensing elements.
By the way, this sensing element detects the JO. of isobutane gas. O
In the concentration range of 5% to 0.5%, the resistance value Rg of the sensitive body is proportional to C-1, where C is the gas concentration.
したがつて、上述の抵抗変化比は定数n(以下濃度係数
と言う)で評価することができる。ちなみに抵抗変化比
5.79はn=0.763に相当する。次に、この素子
のヒータに通電して素子温度を350゜Cに保持し、さ
らに素子側電極間に10■の直流電圧を印加して、頷時
間放置した。Therefore, the above-mentioned resistance change ratio can be evaluated using a constant n (hereinafter referred to as concentration coefficient). Incidentally, the resistance change ratio of 5.79 corresponds to n=0.763. Next, the heater of this element was energized to maintain the element temperature at 350°C, and a DC voltage of 10 μm was applied between the electrodes on the element side, and the element was left for a nodding period.
その後先述と同じ方法でガス感応特性を測定した結果、
Ra=772KΩ、Rg(0.05%)=218KΩ、
Rg(0.5%)=37KΩ、抵抗変化比=5.89(
n=0.770)であつた。さらに、この素子を同様の
方法で200Vf間放置した後、ガス感応特性を測定し
た結果、Ra=786KΩ、Rg(0.05%)=22
9KΩ、Rg(0.5%)=40KΩ、抵抗変化比=5
.73.n=0.758てあつた。以上の実験結果から
れかるように、本発明にかかる素子は、実用検知濃度範
囲における抵抗変化比がきわめて大きく、その定量性が
非常に良好である。After that, we measured the gas sensitivity characteristics using the same method as described above, and found that
Ra=772KΩ, Rg(0.05%)=218KΩ,
Rg (0.5%) = 37KΩ, resistance change ratio = 5.89 (
n=0.770). Furthermore, after leaving this element for 200Vf in the same manner, the gas sensitivity characteristics were measured. As a result, Ra = 786KΩ, Rg (0.05%) = 22
9KΩ, Rg (0.5%) = 40KΩ, resistance change ratio = 5
.. 73. n=0.758. As can be seen from the above experimental results, the element according to the present invention has an extremely large resistance change ratio in the practically detectable concentration range, and its quantitative properties are very good.
また、製造直後から長期間にわたつてそのガス感応特性
が安定してり、エージング工程を必要としないという、
製造上の大きな利点も有している。実施例2
n−Fe2O3とγ−Al。In addition, its gas sensitivity characteristics are stable over a long period of time immediately after production, and no aging process is required.
It also has significant manufacturing advantages. Example 2 n-Fe2O3 and γ-Al.
O3との組成比率を種々変えて、実施例1と同じ方法で
素子を作製し、それぞれについてガス感応特性測定した
。また、酸化アルミニウムの代表的な結晶相であるコラ
ンダム型結晶構造を有するアルファ型アルミナ(α−A
l2O3:ー般に、結晶構造を指定しない酸化アルミニ
ウムと称する場合には、このアルファ型の酸化アルミニ
ウムを意味する)を、γ−Al。O3に代えて使用した
場合についてもあわせて実験し、種々の組成比率の素子
を実施例1と同じ条件て素子を作り、それぞれについて
ガス感応特性を測定した。第1図に濃度係数(Rgcc
C−1のnで表現)、第2図に素子作製直後から20時
間後の課電寿命特性、第3図に同じく200叫間後の課
電寿命特性とγ−Al2O3、α−AI2O3量との関
係を比較して示す。第1図から明らかなように、濃度係
数nは、γ一/Vl2O3の組成比率が増大するに従つ
て大きくなり、それが10〜30モル%で極大となる。Elements were fabricated in the same manner as in Example 1 with various composition ratios with O3, and gas sensitivity characteristics were measured for each element. In addition, alpha-type alumina (α-A
12O3: Generally speaking, when referring to aluminum oxide without specifying the crystal structure, it means this alpha-type aluminum oxide), γ-Al. Experiments were also carried out using O3 in place of O3, and devices with various composition ratios were fabricated under the same conditions as in Example 1, and the gas sensitivity characteristics of each were measured. Figure 1 shows the concentration coefficient (Rgcc
(expressed by n in C-1), Fig. 2 shows the energized life characteristics 20 hours after the element fabrication, and Fig. 3 shows the energized life characteristics and the amounts of γ-Al2O3 and α-AI2O3 after 200 hours. Compare and show the relationship between. As is clear from FIG. 1, the concentration coefficient n increases as the composition ratio of γ-/Vl2O3 increases, and reaches a maximum at 10 to 30 mol%.
一方、α−Al2O3を使用した場合には、なんらそれ
による効果が認められなかつた。また、第2図、第3図
からも、γ−Al2O3を使用することによつて、素子
作製直後から長期間にわたつて、安定した課電寿命特性
を示すことがわかる。一方、α−Al2O3を使用した
場合、素子作製直後から約加時間ほどの間は抵抗値が変
化するが、それ以後は安定した特性を示す。ここで、第
2図および第3図は、イソブタンガス濃度0.5%にお
ける抵抗値Rg(0.5%)の、初期値に対する変化率
で示している。実施例3平均粒径0.5prrLのFe
3O4粉末を0.8モル、およびγ−Al2O3粉末を
0.2モル秤取し、実施例1と同様にして湿式混合し、
かつ粉砕した。On the other hand, when α-Al2O3 was used, no effect was observed. Furthermore, from FIGS. 2 and 3, it can be seen that by using γ-Al2O3, stable charging life characteristics are exhibited over a long period of time immediately after the device is fabricated. On the other hand, when α-Al2O3 is used, the resistance value changes for about an additional time immediately after the device is fabricated, but after that, stable characteristics are exhibited. Here, FIGS. 2 and 3 show the rate of change of the resistance value Rg (0.5%) with respect to the initial value at an isobutane gas concentration of 0.5%. Example 3 Fe with average particle size of 0.5 prrL
Weighed out 0.8 mol of 3O4 powder and 0.2 mol of γ-Al2O3 powder, wet-mixed them in the same manner as in Example 1,
And crushed.
この混合物を80゜Cの温度で真空中において乾燥させ
た。このようにして得られた粉体を直方体形状に加圧成
形し、窒素気流中において、温度800゜Cで焼結した
。その後、常温で冷却しでから、通常空気中で除々に昇
温し、400゜Cの温度に1時間保持して、γ−Fe2
O3を主成分とする焼結体を得た。このようにして作製
した焼結体の表面に金を蒸着して、一対の櫛形電極を形
成した。裏面には白金発熱体を無機接着剤で貼りつけて
ヒータとし、このガス検知素子した。この発熱体に電流
を通じ、その電流値を調節して素子の動作温度を制御し
た。素体温度を350℃に保持して実施例1と同様の方
法でガ又感応特性を測定した。その結果を下表にまとめ
て示す。素子を焼結体として用いても、抵抗値の絶対値
の絶対値そのものは、実施例1、2て示した焼結膜のそ
れと異なるものの、初期特性、課電寿命特性いずれも優
れた特性を有していることがわかる。このようにして、
本発明による素子において、その形状が焼結膜であれ、
焼結体であれ、γ−Al2O3を使用したことによる効
果が十分発揮されるものてある。以上述べたように、ガ
ンマ型酸化第二鉄(γ−Fe2O3)を99.5〜30
モル%、およびガンマ酸化アルミニウム(γ−Al2O
3)を0.5〜50モル%の割合で含有するガス検知素
子は、実用検知濃度範囲で抵抗変化比、すなわち濃度係
数が大きく、濃度検知の定量度がきわめて大きくて、素
子作製直後から長期にわたつて優れた課電寿命特性を有
するものである。The mixture was dried in vacuo at a temperature of 80°C. The powder thus obtained was press-molded into a rectangular parallelepiped shape and sintered at a temperature of 800°C in a nitrogen stream. Then, after cooling to room temperature, the temperature was gradually raised in normal air and maintained at a temperature of 400°C for 1 hour to produce γ-Fe2.
A sintered body containing O3 as a main component was obtained. Gold was deposited on the surface of the sintered body thus produced to form a pair of comb-shaped electrodes. A platinum heating element was attached to the back side with an inorganic adhesive to serve as a heater, and this gas detection element was made. A current was passed through this heating element, and the current value was adjusted to control the operating temperature of the element. The gas sensitivity characteristics were measured in the same manner as in Example 1 while maintaining the element temperature at 350°C. The results are summarized in the table below. Even if the element is used as a sintered body, although the absolute value of the resistance value itself is different from that of the sintered film shown in Examples 1 and 2, it has excellent initial characteristics and energized life characteristics. I know what you're doing. In this way,
In the element according to the present invention, even if its shape is a sintered film,
Even if it is a sintered body, the effects of using γ-Al2O3 can be fully exhibited. As mentioned above, gamma type ferric oxide (γ-Fe2O3) is
mole%, and gamma aluminum oxide (γ-Al2O
Gas sensing elements containing 0.5 to 50 mol % of It has excellent charging life characteristics over a long period of time.
本発明による素子において、γ−Al2O3量をγ−F
e2O3との合計量に対して0.5〜70%としたのは
、それが0.5モル%未満ではγ一AI2O3による効
果が見られず、また、70モル%を越えると、素子の抵
抗値が異常に高くなり、さらノには焼結膜、焼結体いず
れかの場合も実用素子として十分な機械的強度が得られ
ないことがあり、ガス検知素子として実用に供し得ない
ものとなるためてある。また実施例においては、出発原
料を四三酸化鉄(Fe3O4)としたものについて記載
し・たが、最終的な素子の状態で主成分がγ−Fe2O
3となるものてあればよく原材料を特に限定するもので
はない。また酸化アルミニウム(Al2O3)結晶相の
中でスピネル型構造のγ−Al2O3を選んだのは、そ
の結晶相のうちもつとも代表的なα−7/Vl2O3を
用いても、201寺間程度のエージング後の長期課電寿
命特性は優れているものの、抵抗変化比、すなわち濃度
係数の増大に効果が見られないのに対して、γ−Al2
O3については長期間にわたつて、優れた特性を保持し
得るからである。以上、本発明にかかるガス検知素子は
、ガス濃度を定量度よく検知する素子として実用上きわ
めて重要な要素てある抵抗変化比、すなわち濃度係数の
大なる素子を実現するものであり、かつ長期にわたつて
その特性が維持するという長期安定性の優れた素子を提
供するものである。また、特性をさらに向上させるため
、あるいは目的に応じて、より適した特性を得るために
他の成分を添加含有させることも勿論可能てある。実施
例では検知対象ガスをイソブタンガスに限つて説明した
が、エタンや、プロパン、水素などの一般の可念性ガス
に対しても本発明の効果は有効であることはいうまでも
ない。In the device according to the present invention, the amount of γ-Al2O3 is
The reason why it is set at 0.5 to 70% with respect to the total amount of e2O3 is that if it is less than 0.5 mol%, the effect of γ-AI2O3 will not be seen, and if it exceeds 70 mol%, the resistance of the element will decrease. The value becomes abnormally high, and either the sintered film or the sintered body may not have sufficient mechanical strength as a practical element, making it impossible to use it as a practical gas sensing element. I have saved up. Furthermore, in the examples, the starting material was described as triiron tetroxide (Fe3O4), but in the state of the final device, the main component was γ-Fe2O.
There are no particular restrictions on the raw materials, as long as they have a rating of 3. In addition, among the aluminum oxide (Al2O3) crystal phases, γ-Al2O3 with a spinel structure was selected because even if α-7/Vl2O3, which is the most representative of the crystal phases, was used, after aging of about 201 Terama, Although γ-Al2 has excellent long-term energized life characteristics, it has no effect on increasing the resistance change ratio, that is, the concentration coefficient.
This is because O3 can maintain excellent properties for a long period of time. As described above, the gas detection element according to the present invention realizes an element with a large resistance change ratio, that is, a concentration coefficient, which is an extremely important element in practical use as an element that detects gas concentration with good quantitative accuracy, and is capable of long-term use. This provides an element with excellent long-term stability that maintains its characteristics over time. Moreover, it is of course possible to add and contain other components in order to further improve the properties or to obtain more suitable properties depending on the purpose. In the embodiments, the gas to be detected is limited to isobutane gas, but it goes without saying that the effects of the present invention are also effective for general flammable gases such as ethane, propane, and hydrogen.
第1図は本発明にかかる可燃性ガス検知素子においてγ
−Al2O3量と濃度係数との関係を、γ一Al2O3
に代えてα−Al2O3を使用したときの関係と対比し
て示す図、第2図および第3図は同じく課電寿命特性を
対比して示す図である。FIG. 1 shows γ in the combustible gas detection element according to the present invention.
-The relationship between the amount of Al2O3 and the concentration coefficient is expressed as γ-Al2O3
Figures 2 and 3 are diagrams that compare the relationship when α-Al2O3 is used instead of , and Figures 2 and 3 are diagrams that also compare and compare the energized life characteristics.
Claims (1)
.5〜30%モル、およびガンマ型酸化アルミニウム(
γ−Al_2O_3)を0.5〜70モル%の割合で含
有している焼結膜または焼結体をガス感応体とし、この
ガス感応体に1対の電極を設け、可燃性ガスの存在を前
記ガス感応体の電気抵抗値の減少として検出することを
特徴とする可燃性ガス検出素子。1 Gamma type ferric oxide (γ-Fe_2O_3) at 99
.. 5-30% mol, and gamma-type aluminum oxide (
A sintered film or a sintered body containing 0.5 to 70 mol% of γ-Al_2O_3) is used as a gas sensitive body, and a pair of electrodes is provided on this gas sensitive body to detect the presence of combustible gas. A combustible gas detection element characterized by detecting a decrease in the electrical resistance value of a gas sensitive body.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52118243A JPS6045369B2 (en) | 1977-09-30 | 1977-09-30 | Flammable gas detection element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52118243A JPS6045369B2 (en) | 1977-09-30 | 1977-09-30 | Flammable gas detection element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5451896A JPS5451896A (en) | 1979-04-24 |
| JPS6045369B2 true JPS6045369B2 (en) | 1985-10-09 |
Family
ID=14731771
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52118243A Expired JPS6045369B2 (en) | 1977-09-30 | 1977-09-30 | Flammable gas detection element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6045369B2 (en) |
-
1977
- 1977-09-30 JP JP52118243A patent/JPS6045369B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5451896A (en) | 1979-04-24 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JPS5853862B2 (en) | Flammable gas detection element | |
| JPS6054259B2 (en) | Moisture sensitive ceramic | |
| JPS6045369B2 (en) | Flammable gas detection element | |
| EP0023216B1 (en) | An oxygen-sensitive element and a method of detecting oxygen concentration | |
| KR0158561B1 (en) | Method of manufacturing thick-film for one-fired inflammability gas sensor | |
| JPH01291151A (en) | Oxygen sensor | |
| JPS608459B2 (en) | gas detection element | |
| JPS5957153A (en) | Gas detecting element | |
| JPS58200153A (en) | gas detection element | |
| JPS6026458B2 (en) | gas detection element | |
| JPS63194307A (en) | Humidity sensitive ceramics | |
| KR840000260B1 (en) | Temperature-responsive element | |
| JPS6222414B2 (en) | ||
| JPS6222417B2 (en) | ||
| US4232441A (en) | Method for preparing rare earth or yttrium, transition metal oxide thermistors | |
| JPS6223252B2 (en) | ||
| JPS5957154A (en) | Gas detecting element | |
| JPS58201054A (en) | gas detection element | |
| JPS6129661B2 (en) | ||
| JPS6153658B2 (en) | ||
| JPS6222420B2 (en) | ||
| JPS6252921B2 (en) | ||
| JPH01158339A (en) | Humidity sensor | |
| JPH04329348A (en) | Moisture-sensitive ceramic composition material | |
| JPS587041B2 (en) | Moisture sensitive resistance element for relative humidity |