JPH06103285B2 - Semiconductor gas detector - Google Patents

Semiconductor gas detector

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Publication number
JPH06103285B2
JPH06103285B2 JP4024382A JP2438292A JPH06103285B2 JP H06103285 B2 JPH06103285 B2 JP H06103285B2 JP 4024382 A JP4024382 A JP 4024382A JP 2438292 A JP2438292 A JP 2438292A JP H06103285 B2 JPH06103285 B2 JP H06103285B2
Authority
JP
Japan
Prior art keywords
metal wire
gas
resistance
wire coil
resistance value
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 - Lifetime
Application number
JP4024382A
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Japanese (ja)
Other versions
JPH0580012A (en
Inventor
洋 貝野
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.)
New Cosmos Electric Co Ltd
Original Assignee
New Cosmos Electric Co Ltd
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Filing date
Publication date
Application filed by New Cosmos Electric Co Ltd filed Critical New Cosmos Electric Co Ltd
Priority to JP4024382A priority Critical patent/JPH06103285B2/en
Publication of JPH0580012A publication Critical patent/JPH0580012A/en
Publication of JPH06103285B2 publication Critical patent/JPH06103285B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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、SnO2 やZnOなど
を主成分とするガス感応半導体の燒結体で、単一の金属
線コイルを包み込んでビード状にし、前記金属線コイル
を加熱用ヒータ兼燒結体の電気抵抗値変化検出用電極と
して用いる半導体ガス検出素子に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a sintered body of a gas sensitive semiconductor containing SnO 2 , ZnO or the like as a main component and enclosing a single metal wire coil into a bead shape, and heating the metal wire coil. The present invention relates to a semiconductor gas detection element used as an electrode for detecting a change in electric resistance of a sintered body.

【0002】[0002]

【従来の技術】ガス感応半導体は、被検ガス雰囲気中に
おかれると、電気抵抗値変化(多くの場合減少)をひき
起す。その際、ガス吸脱着速度や抵抗値変化を実用的な
大きさで行わせるために、通常は室温よりもかなり高温
(300℃以上の場合が多い)で用いる。したがって、
半導体を用いた実用的なガス検出素子は、半導体を高温
にするための何らかの加熱手段を備えている。
2. Description of the Related Art A gas-sensitive semiconductor causes a change (in many cases, a decrease) in electric resistance value when placed in a test gas atmosphere. At that time, in order to change the gas adsorption / desorption rate and the resistance value with a practical size, it is usually used at a temperature considerably higher than room temperature (often 300 ° C. or higher). Therefore,
A practical gas detection element using a semiconductor includes some heating means for raising the temperature of the semiconductor.

【0003】さらに、当然のことながら、半導体の抵抗
値変化を検出するために何らかの電極を備えているのは
いうまでもない。このように、半導体ガス検出素子は、
一般に加熱用ヒータと抵抗変化検出用電極を共に具備
している。
Furthermore, it goes without saying that some kind of electrode is provided to detect a change in the resistance value of the semiconductor. Thus, semiconductors gas detecting element,
Generally they are both equipped with a heater resistance value change detecting electrodes.

【0004】このような二つの機能を単一の金属線コイ
ルで行わせる半導体ガス検出素子として、図4に示すタ
イプのものがある。
As a semiconductor gas detecting element that performs such two functions by a single metal wire coil, there is a type shown in FIG.

【0005】図4において、1は金属線コイル、2はガ
ス感応半導体の燒結体、3は金属ピンである。以下、こ
の半導体ガス検出素子の動作について説明する。
In FIG. 4, 1 is a metal wire coil, 2 is a sintered body of a gas sensitive semiconductor, and 3 is a metal pin. The operation of this semiconductor gas detecting element will be described below.

【0006】半導体ガス検出素子の加熱は、金属線コイ
ル1に適当な電流を流すことによってなされる。また、
燒結体2の抵抗値変化は、金属線コイル1の両端の抵抗
値、すなわち金属線コイル1と燒結体2の組み合わさっ
た合成的な抵抗値の変化として検出される。以下、この
合成的な抵抗値をセンサ抵抗値Rと呼ぶことにする。
The semiconductor gas detecting element is heated by passing an appropriate current through the metal wire coil 1. Also,
The change in the resistance value of the sintered body 2 is detected as a resistance value at both ends of the metal wire coil 1, that is, a combined change in the resistance value of the combination of the metal wire coil 1 and the sintered body 2. Hereinafter, this combined resistance value will be referred to as a sensor resistance value R.

【0007】今、金属線コイル1のみの抵抗値をRC
燒結体2の部分を実効的に金属線コイル1の抵抗値RC
の並列抵抗とみなしたときの抵抗値をRS とすれば、セ
ンサ抵抗値Rは、
Now, the resistance value of only the metal wire coil 1 is R C ,
The resistance value R C of the metal wire coil 1 is effectively applied to the portion of the sintered body 2.
Assuming that the resistance value of the parallel resistance of R is R S , the sensor resistance value R is

【0008】[0008]

【数1】 となる。これを図示すると、図5のようになる。被検ガ
スの存在は、被検ガスによる燒結体2の抵抗値RS の変
化が第(1)式に従うセンサ抵抗値Rの変化として検出
される。
[Equation 1] Becomes This is illustrated in FIG. The presence of the test gas is detected as a change in the resistance value R S of the sintered body 2 due to the test gas as a change in the sensor resistance value R according to the equation (1).

【0009】[0009]

【発明が解決しようとする課題】上述のようなヒータ兼
電極としての金属線コイル1に用いられる線材として
は、耐熱性,耐食性および燒結体2との電気的接触が良
好であるなどの点から、従来はPt線が用いられてい
る。しかし、Pt線は比抵抗が十分に大きくなく、その
ため検出感度が不十分であるという問題点があった。
The wire used for the metal wire coil 1 as the heater and electrode as described above is excellent in heat resistance, corrosion resistance and electrical contact with the sintered body 2. Conventionally, Pt wire is used. However, the Pt wire has a problem that the specific resistance is not sufficiently large and therefore the detection sensitivity is insufficient.

【0010】本発明は、Pt線と比べて耐食性などを余
り変えずに検出感度が大きく出来るPt合金線を用いた
半導体ガス検出素子を提供することを目的とする。
It is an object of the present invention to provide a semiconductor gas detection element using a Pt alloy wire which can have a higher detection sensitivity without significantly changing the corrosion resistance and the like as compared with the Pt wire.

【0011】[0011]

【課題を解決するための手段】本発明に係る半導体ガス
検出素子は、単一の金属線コイルをガス感応半導体の燒
結体で包み込んでビード状とした構造を有し、かつ金属
線コイルを加熱用ヒータ兼電気抵抗値変化検出用電極と
して用いるガス検出素子において、金属線コイルを、R
h,Ir,Niのいずれか1つを5〜30%の範囲で含
有したPt合金線で構成したものである。
A semiconductor gas detecting element according to the present invention has a bead-like structure in which a single metal wire coil is wrapped with a sintered body of a gas sensitive semiconductor, and the metal wire coil is heated. In the gas detection element used as the heater for the heater and the electrode for detecting the change in the electric resistance value, the metal wire coil is
It is composed of a Pt alloy wire containing any one of h, Ir and Ni in the range of 5 to 30%.

【0012】[0012]

【作用】本発明においては、金属線コイルとしてRh,
Ir,Niのいずれか1つの含有量が5〜30%である
Pt合金線を用いたので、Pt線単体に比べて耐食性な
どを余り変えずに比抵抗を大きくとれ、ガス検出感度が
向上する。
In the present invention, as the metal wire coil, Rh,
Since the Pt alloy wire in which the content of one of Ir and Ni is 5 to 30% is used, the specific resistance can be increased and the gas detection sensitivity can be improved as compared with the Pt wire alone without significantly changing the corrosion resistance. .

【0013】[0013]

【実施例】本発明の半導体ガス検出素子は、金属線コイ
ルにRh,Ir,Niのいずれか1つの含有量が5〜3
0%であるPt合金線を用いたものである。以下、金属
線材の比抵抗と抵抗温度係数に分けて本発明の実施例を
説明する。
EXAMPLE A semiconductor gas detecting element of the present invention has a metal wire coil containing 5 to 3 of any one of Rh, Ir and Ni.
The Pt alloy wire is 0%. Hereinafter, examples of the present invention will be described by dividing the specific resistance and the temperature coefficient of resistance of the metal wire.

【0014】(a) 金属線材の比抵抗 被検ガスによるRS の変化をセンサ抵抗値Rの変化とし
て、できるだけ大きく取り出すためには、RS はRC
比べて小さいほうが望ましい。しかし、燒結体2の抵抗
値を小さくすることはあまり容易ではないため、RC
S のかね合いを適当にするには、RC をできるだけ大
きくする必要がある。そのために、金属線コイル1の線
径を細くしたり巻数を多くすればよいが、それには限度
がある。
(A) Specific resistance of the metal wire rod In order to extract the change in R S due to the test gas as the change in the sensor resistance value R as large as possible, it is desirable that R S be smaller than R C. However, since it is not so easy to reduce the resistance value of the sintered body 2, it is necessary to make R C as large as possible in order to properly balance R C and R S. Therefore, the wire diameter of the metal wire coil 1 may be reduced or the number of turns may be increased, but there is a limit to that.

【0015】そこで、本発明では純Pt線の代わりに、
例えばRhを含むPt合金線を用いれば、図1にあるよ
うに、400℃では線材の比抵抗ρC (400℃)はR
h含有量が5〜30%では純Ptの25%以上、10〜
20%では40%近く増加することが分る。したがっ
て、適当なRh含有量のPt−h合金線を用いれば、
被検ガスの存在をセンサ出力として、より効率よく取り
出す利点を有する。
Therefore, in the present invention, instead of pure Pt wire,
For example, if a Pt alloy wire containing Rh is used, as shown in FIG. 1, at 400 ° C., the specific resistance ρ C (400 ° C.) of the wire is R
When the h content is 5 to 30%, it is 25% or more of pure Pt,
It can be seen that at 20%, it increases by nearly 40%. Thus, by using the Pt-R h alloy wire suitable Rh content,
There is an advantage that the existence of the test gas is used as a sensor output and is taken out more efficiently.

【0016】上記はPt−h合金線の場合であった
が、この他、Pt−Ir,Pt−Niなどの合金線を用
いることもできる。下記表1にこの発明で用いるPt合
金線の20℃での比抵抗ρC (20℃)をまとめて示
す。
[0016] The above Pt- although a was the case of R h alloy wire, this addition may be used alloy wire, such as Pt-Ir, Pt-Ni. Table 1 below summarizes the specific resistance ρ C (20 ° C.) at 20 ° C. of the Pt alloy wire used in the present invention.

【0017】[0017]

【表1】 (10-5Ωcm) (b) 金属線材の抵抗温度係数 センサ抵抗値Rの変化を一般にガス検出素子に定電圧を
かけて、または定電流を流して検出する場合、センサ抵
抗値Rの変化に対応して、ガス検出素子における消費電
力が変化してガス検出素子の温度の変化を引き起す。こ
の温度変化を押さえるため、消費電力変化を小さくする
には、RS に比べてRCを小さくすればよいが、あまり
小さくすると先の考察で明らかなように被検ガスによる
S 変化に基づくRの変化が小さくなるため、いわゆる
ガス検出素子の感度が低くなってしまう。したがって、
C は単純に小さくするわけにはいかない。また、RC
が適当に大きいときは、RC の抵抗温度係数が大きけれ
ば大きい程、ガス検出素子の消費電力の大きさに影響を
与える。したがって、金属線コイル1には小さな温度係
数を持つ線材を用いるのが望ましい。
[Table 1] (10 -5 Ωcm) (b) Temperature coefficient of resistance of metal wire When a change in the sensor resistance value R is detected by applying a constant voltage or a constant current to the gas detection element, the change in the sensor resistance value R Correspondingly, the power consumption of the gas detection element changes, causing the temperature of the gas detection element to change. Order to suppress this temperature change, in order to reduce the power consumption changes may be made smaller to R C compared to R S but based on R S changes due to the test gas as evidenced by the previous discussion when too small Since the change in R becomes small, the sensitivity of the so-called gas detection element becomes low. Therefore,
R C cannot be simply reduced. Also, R C
Is appropriately large, the larger the resistance temperature coefficient of R C , the more the power consumption of the gas detection element is affected. Therefore, it is desirable to use a wire rod having a small temperature coefficient for the metal wire coil 1.

【0018】ところが、Ptの抵抗温度係数は、ニクロ
ム線などの発熱線に比べると非常に大きい(ニクロム線
などの卑金属線は耐食性などの点で使えない)。そこ
で、耐食性などをあまり変えずに、抵抗温度係数αを小
さくするため、合金線コイルの線材として、例えばRh
を含有するPt−h合金線を用いることが有効であ
る。
However, the temperature coefficient of resistance of Pt is much larger than that of a heating wire such as a nichrome wire (a base metal wire such as a nichrome wire cannot be used in terms of corrosion resistance). Therefore, in order to reduce the temperature coefficient of resistance α without significantly changing the corrosion resistance and the like, as a wire material of the alloy wire coil, for example, Rh is used.
It is effective to use a Pt-R h alloy wire containing.

【0019】図2にあるように、Ptに対するhの含
有量の増加とともに、抵抗温度係数α(0〜100℃)
は最初減少し、再び増加する。含有量5〜70%で、α
の値は純Pt線の55%程度であり、含有量10〜60
%では純Pt線の50%以下となる。もし、ガス検出素
子の温度が400℃で用いられていて、被検ガスによっ
て100℃低下したとすると(すなわち300℃になっ
たとすると)、金属線コイル1の抵抗値RC は、図3に
あるように減少する(図にはRC (300℃)/RC
(400℃)で表した)。Pt線なら15.4%の減少
であるが、Rh含有量が5〜65%のPt−h線では
11.5%程度であり、含有量10〜15%では、ほぼ
10%以内におさえられている。したがって、適当なR
h含有量のPt−Rh線を用いれば、被検ガスの存在に
よるガス検出素子の温度の変化を抑えることができる。
なお、ZrO2 ,TiO2 などの適当な酸化物が小量
(例えば0.1%)分散添加されたものにおいても、合
金にしたことの効果は同等である。
As shown in FIG. 2, the temperature coefficient of resistance α (0 to 100 ° C.) increases as the content of R h with respect to Pt increases.
Decreases first and then increases again. Content of 5 to 70%, α
Value is about 55% of pure Pt wire, and the content is 10-60
% Is 50% or less of the pure Pt wire. If the temperature of the gas detection element is 400 ° C. and the gas to be detected lowers the temperature by 100 ° C. (that is, reaches 300 ° C.), the resistance value R C of the metal wire coil 1 is shown in FIG. Decrease as there is (R C (300 ° C) / R C in the figure)
(Expressed at 400 ° C.). Is a 15.4% reduction if Pt wire is about 11.5% in the Rh content of 5 to 65% of the Pt-R h line, the content of 10-15%, suppressed within approximately 10% Has been. Therefore, a suitable R
If the h content Pt-Rh line is used, it is possible to suppress a change in the temperature of the gas detection element due to the presence of the test gas.
Even when a small amount (for example, 0.1%) of a suitable oxide such as ZrO 2 or TiO 2 is dispersed and added, the effect of alloying is the same.

【0020】上記はPt−Rh合金線の場合であった
が、この他、Pt−Ir,Pt−Niなどの合金線を用
いることもできる。下記表2に、この発明で用いるPt
合金線の抵抗温度係数αをまとめて示す。
Although the above is the case of the Pt-Rh alloy wire, other alloy wires such as Pt-Ir and Pt-Ni can also be used. Table 2 below shows Pt used in the present invention.
The temperature coefficient of resistance α of the alloy wire is shown together.

【0021】[0021]

【表2】 (×10-4/℃) 前記(1),(2)に述べた利点およびRh含有量が3
0%を超えた場合に加工性が悪くなる点から考えて、R
h含有量の実用的な範囲としては5〜30%と思われ
る。また、Ir,Niのいずれか1つを5〜30%含有
させたPt合金線でもほぼ同様な効果が得られた。
[Table 2] (× 10 −4 / ° C.) Advantages described in (1) and (2) above and Rh content of 3
Considering from the point that workability deteriorates when it exceeds 0%, R
It seems that the practical range of the h content is 5 to 30%. In addition , a similar effect was obtained with a Pt alloy wire containing 5 to 30% of either Ir or Ni .

【0022】[0022]

【発明の効果】以上詳細に説明したように、本発明は単
一の金属線コイルをガス感応半導体の燒結体で包み込ん
で、ビード状とした構造の半導体ガス検出素子におい
て、加熱用ヒータ兼電極として純Pt線を用いる代わり
に、Rh,Ir,Niのいずれか1つを5〜30%含有
するPt合金線を用いたので、金属線コイルの耐熱性,
耐食性などはあまり変えずに、被検ガスの存在をセン
サ出力としてより敏感に取り出すことができる利点と、
ガス雰囲気でのガス検出素子の消費電力の変化を抑制
できる利点を有する。
As described in detail above, according to the present invention, in a semiconductor gas detecting element having a bead-like structure in which a single metal wire coil is wrapped with a sintered body of a gas sensitive semiconductor, a heater / electrode for heating is also used. Since a Pt alloy wire containing any one of Rh, Ir, and Ni in an amount of 5 to 30% was used instead of the pure Pt wire as described above, the heat resistance of the metal wire coil
With the advantage that the existence of the test gas can be more sensitively taken out as the sensor output without changing the corrosion resistance etc.
It has an advantage that a change in power consumption of the gas detection element in a gas atmosphere can be suppressed.

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

【図1】本発明を説明するためのPtに対するRh含有
量と比抵抗との関係を示す図である。
FIG. 1 is a diagram showing the relationship between Rh content and specific resistance with respect to Pt for explaining the present invention.

【図2】Rhの含有量と抵抗温度係数αの関係を示す特
性図である。
FIG. 2 is a characteristic diagram showing the relationship between the content of Rh and the temperature coefficient of resistance α.

【図3】Rh含有量と金属線コイルの抵抗値の300℃
と400℃における比との関係を示す図である。
FIG. 3 Rh content and resistance of metal wire coil of 300 ° C.
It is a figure which shows the relationship between and the ratio in 400 degreeC.

【図4】従来の半導体ガス検出素子の一例を示す要部の
構成略図である。
FIG. 4 is a schematic configuration diagram of a main part showing an example of a conventional semiconductor gas detection element.

【図5】図4の等価回路図である。FIG. 5 is an equivalent circuit diagram of FIG.

【符号の説明】[Explanation of symbols]

1 金属線コイル 2 燒結体 3 金属ピン 1 Metal wire coil 2 Sintered body 3 Metal pin

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 単一の金属線コイルをガス感応半導体の
燒結体で包み込んでビード状とした構造を有し、かつ前
記金属線コイルを加熱用ヒータ兼電気抵抗値変化検出用
電極として用いるガス検出素子において、前記金属線コ
イルを、Rh,Ir,Niのいずれか1つを5〜30%
の範囲で含有したPt合金線で構成したことを特徴とす
る半導体ガス検出素子。
1. A gas having a structure in which a single metal wire coil is wrapped in a sintered body of a gas sensitive semiconductor to form a bead, and the metal wire coil is used as a heater for heating and an electrode for detecting electric resistance value change. In the detection element, the metal wire coil is made of any one of Rh, Ir and Ni in an amount of 5 to 30%.
2. A semiconductor gas detecting element, characterized in that it is composed of a Pt alloy wire contained in the range of.
JP4024382A 1992-01-16 1992-01-16 Semiconductor gas detector Expired - Lifetime JPH06103285B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4024382A JPH06103285B2 (en) 1992-01-16 1992-01-16 Semiconductor gas detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4024382A JPH06103285B2 (en) 1992-01-16 1992-01-16 Semiconductor gas detector

Publications (2)

Publication Number Publication Date
JPH0580012A JPH0580012A (en) 1993-03-30
JPH06103285B2 true JPH06103285B2 (en) 1994-12-14

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP4024382A Expired - Lifetime JPH06103285B2 (en) 1992-01-16 1992-01-16 Semiconductor gas detector

Country Status (1)

Country Link
JP (1) JPH06103285B2 (en)

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