JPH032654A - Carbon monoxide sensor - Google Patents
Carbon monoxide sensorInfo
- Publication number
- JPH032654A JPH032654A JP13837889A JP13837889A JPH032654A JP H032654 A JPH032654 A JP H032654A JP 13837889 A JP13837889 A JP 13837889A JP 13837889 A JP13837889 A JP 13837889A JP H032654 A JPH032654 A JP H032654A
- Authority
- JP
- Japan
- Prior art keywords
- sensitivity
- gas
- semiconductor
- resistance value
- active part
- 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.)
- Pending
Links
- UGFAIRIUMAVXCW-UHFFFAOYSA-N Carbon monoxide Chemical compound [O+]#[C-] UGFAIRIUMAVXCW-UHFFFAOYSA-N 0.000 title claims description 6
- 229910002091 carbon monoxide Inorganic materials 0.000 title claims description 5
- 239000004065 semiconductor Substances 0.000 claims abstract description 41
- 230000035945 sensitivity Effects 0.000 claims abstract description 41
- 238000010438 heat treatment Methods 0.000 claims description 7
- 239000000203 mixture Substances 0.000 claims description 7
- 239000000919 ceramic Substances 0.000 claims description 6
- 238000005245 sintering Methods 0.000 claims description 6
- 239000003795 chemical substances by application Substances 0.000 claims description 5
- 229910052697 platinum Inorganic materials 0.000 claims description 5
- 229910052763 palladium Inorganic materials 0.000 claims description 4
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 abstract description 22
- 239000007789 gas Substances 0.000 description 36
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Substances [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 21
- 238000010586 diagram Methods 0.000 description 5
- 238000000034 method Methods 0.000 description 5
- 239000007787 solid Substances 0.000 description 5
- 239000000843 powder Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000003973 paint Substances 0.000 description 2
- 238000004804 winding Methods 0.000 description 2
- 229910018487 Ni—Cr Inorganic materials 0.000 description 1
- 229910001260 Pt alloy Inorganic materials 0.000 description 1
- 229910002845 Pt–Ni Inorganic materials 0.000 description 1
- 230000032683 aging Effects 0.000 description 1
- 229910002090 carbon oxide Inorganic materials 0.000 description 1
- 238000007084 catalytic combustion reaction Methods 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 230000017525 heat dissipation Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000001179 sorption measurement Methods 0.000 description 1
Landscapes
- Investigating Or Analyzing Materials By The Use Of Fluid Adsorption Or Reactions (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、活性部及び補償部に夫々組成の異なるSnO
□系半導体を組み込んで形成されるブリフジ回路方式の
一酸化炭素センサに関する。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention provides an active part and a compensation part containing SnO with different compositions.
□Relates to a carbon monoxide sensor of the Brifuji circuit type formed by incorporating a system semiconductor.
一般に、SnO,系半導体センサに限らず、半導体セン
サは、低濃度のガスに極めて高い感度を有するものであ
るが、反面、
a、ガスの選択性がない。即ち、各種のガスが混在する
場合における特定ガスの感度がよくない。In general, semiconductor sensors, including SnO-based semiconductor sensors, have extremely high sensitivity to low concentration gases, but on the other hand, a) they lack gas selectivity. That is, when various gases are mixed, the sensitivity of a specific gas is not good.
b、雰囲気で敏感で、特にノーガス時の特性(例えば、
ゼロポイント)が不安定かつ不確実である。b. Sensitive in the atmosphere, especially characteristics when there is no gas (e.g.
zero point) is unstable and uncertain.
C1再現性がよくない。C1 reproducibility is poor.
d、環境の変化即ち温湿度の変化等によりその特性に変
動が認められる。d. Changes in the characteristics are observed due to changes in the environment, ie, changes in temperature and humidity.
等の欠点があり、LPG用のガス洩れ警報器であっても
、1ctH+oの警報濃度が500〜3000pPta
の間で変動し、C,H50H等では誤報が屡々発生する
のが実状であった。このため、COに対する感度が良好
なSnO□系半導体であっても、従来のSnO□系半導
体を警報器に適用することは、不安定でありときには危
険でさえあった。Even with gas leak alarms for LPG, the alarm concentration for 1 ctH+o is 500 to 3000 pPta.
The actual situation is that false alarms often occur with C, H50H, etc. For this reason, even though SnO□-based semiconductors have good sensitivity to CO, applying conventional SnO□-based semiconductors to alarm devices has been unstable and sometimes even dangerous.
本発明はかかる実状に鑑み、SnO□系半導体の組成と
温度との関係並びに該センサの各種ガスの感度特性につ
いて種々研究を重ねた結果、2種類の特長のあるSnO
□半導体を使用して他ガスの感度を相殺し、CO感度の
みを取り出しうろことを知得し、更に組成を中心に種々
検討した結果、SnO□系半導体センサの精度を高める
に至りたるものである。In view of these circumstances, the present invention has been made through various studies on the relationship between the composition and temperature of SnO□-based semiconductors and the sensitivity characteristics of various gases of the sensor.
□Using a semiconductor to offset the sensitivity of other gases, extracting only the CO sensitivity and learning about the scales, and further considering various aspects with a focus on composition, we were able to improve the accuracy of the SnO□-based semiconductor sensor. be.
本発明は、
(i)直列に配置されてノーガス時概ね同一の抵抗値を
有する活性部1と補償部2とを有し、その対辺に並列し
て所定のブリッジ抵抗rl+rZ+r、を直列に配置し
、活性部1と補償部2との中間点3とブリッジ抵抗r2
との間にCOガス感十
が電圧値で表示される感度計会を設け、また、上記活性
部、補償部及び各ブリッジ抵抗に直流電圧を印加するブ
リッジ電源弁を配置するブリフジ回路をもって形成され
る一酸化炭素センサであって、
(ii)活性部1には、CO感度のみ増感された5nO
z/Pd、Pt半導体が使用され、
(iii )また、補償部2にはCO感度が増感されて
いないSnO2/Sn半導体が使用されて、(iv)
Co雰囲気中で活性部1と補償部2と間に生じる抵抗値
差に基づいてCO感度を求める(v)−酸化炭素センサ
にその要旨を存するものである。The present invention has the following features: (i) The active part 1 and the compensation part 2 are arranged in series and have approximately the same resistance value during no gas, and a predetermined bridge resistance rl+rZ+r is arranged in series in parallel on the opposite side thereof. , the intermediate point 3 between the active part 1 and the compensation part 2 and the bridge resistance r2
A sensitivity meter for displaying the CO gas sensitivity as a voltage value is installed between the bridge circuit and the bridge circuit, which is equipped with a bridge power supply valve that applies a DC voltage to the active section, compensation section, and each bridge resistor. (ii) The active part 1 contains 5nO sensitized only to the CO sensitivity.
z/Pd, Pt semiconductors are used, (iii) and a SnO2/Sn semiconductor whose CO sensitivity is not sensitized is used for the compensator 2, (iv)
The gist of this is a (v)-carbon oxide sensor that determines the CO sensitivity based on the resistance value difference that occurs between the active part 1 and the compensating part 2 in a Co atmosphere.
以下、図面を参照し実施例に基づいて本発明を説明する
。Hereinafter, the present invention will be described based on examples with reference to the drawings.
第1図は、本発明に係るセンサの回路図である。FIG. 1 is a circuit diagram of a sensor according to the present invention.
まず、直列に配置される活性部1と補償部2とは、ノー
ガス時概ね同一の抵抗値を有するコイルからなり、その
対辺に並列してブリッジ抵抗rI+ r2゜r3が直列
に配置されている。活性部1と補償部2との中間点とブ
リッジ抵抗r2との間には、COガス怒度が相等する電
圧値で表示される感度計4を設け、また活性部1及び補
償部2に直流電圧を印加するブリッジ電源5を配してブ
リッジ回路が形成される。First, the active part 1 and the compensation part 2 arranged in series are composed of coils having approximately the same resistance value when no gas is present, and a bridge resistor rI+r2°r3 is arranged in series in parallel on the opposite side thereof. A sensitivity meter 4 is provided between the midpoint between the active part 1 and the compensation part 2 and the bridge resistor r2, and the sensitivity meter 4 displays the CO gas anger level with an equivalent voltage value. A bridge circuit is formed by arranging a bridge power supply 5 that applies voltage.
活性部1及び補償部2を形成するコイルは、共に線径1
5〜20μmの白金(Pt)線又は白金系合金(Pt−
報、 Pt−Ni、 Pt−Rt等)線をセラミック管
りにコイル状に巻付けて作成される。The coils forming the active part 1 and the compensation part 2 both have a wire diameter of 1.
Platinum (Pt) wire or platinum alloy (Pt-
It is made by winding a wire (Pt-Ni, Pt-Rt, etc.) into a coil around a ceramic tube.
活性部1に使用される5nu2n半2体は、SnO□に
Pd、 Ptを夫々1重量%添加して約600℃で1.
5時間焼成しCO感度を増感したものが使用され、また
補償部2には、感度が増感されてない般用のSnO□/
Snが使用される。The 5nu2n halves used in the active part 1 were prepared by adding 1% by weight each of Pd and Pt to SnO□ and heating them at about 600°C for 1.
The one used is one whose CO sensitivity has been sensitized by firing for 5 hours, and the general-purpose SnO□/ whose sensitivity has not been sensitized is used in the compensation section 2.
Sn is used.
夫々の組成の半導体粉末を微粉砕し、SiO□コロイダ
ル溶液等の焼結剤を加えて塗料化したものを、第2図に
示す如く、セラミック(例えばアルミナ)管6の上面に
ノーガス時概ね同一抵抗になるようPt線を巻いて形成
され信号取出ロア、7を有するコイル8のうえに、塗装
し、650″〜700℃で1〜1.5時間焼結し、その
後、該セラミック管の中空部に内蔵されるNi−Cr線
の如き発熱体9を装着する。できたSnO,系半導体セ
ンサは焼結後、十分な通電エージングが行なわれる。発
熱体9に印加される電圧により、センサの温度が定めら
れる。即ち印加電圧がDCIOVでは220’〜240
℃、12Vでは300’〜320℃となる。Semiconductor powder of each composition is finely ground, a sintering agent such as SiO□ colloidal solution is added to form a paint, and as shown in FIG. Coil 8, which is formed by winding a Pt wire to form a resistor and has a signal extraction lower 7, is coated and sintered at 650'' to 700°C for 1 to 1.5 hours, and then the hollow of the ceramic tube is A heating element 9 such as a Ni-Cr wire built into the part is attached.After the SnO-based semiconductor sensor is sintered, it is subjected to sufficient electrical aging.The voltage applied to the heating element 9 causes the sensor to heat up. The temperature is determined, i.e. the applied voltage is between 220' and 240' at DCIOV.
℃ and 12V, it becomes 300' to 320℃.
かくして構成されたセンサを使用して、ノーガス時にお
ける上記センサの感度A(kΩ)及びCO500ppr
a雰囲気中におけるセンサの感度B(kΩ)が測定され
た。結果は第1表のとおり。Using the sensor configured in this way, the sensitivity A (kΩ) of the above sensor and CO500 ppr in no gas state.
The sensitivity B (kΩ) of the sensor in a atmosphere was measured. The results are shown in Table 1.
上表から、ヒータに印加される電圧即ちセンサ温度によ
り、
10Vでは 活性部の変化率(平均)61.7%補償部
# 24.3%
変化率(平均)の差 37.4%
12Vでは 活性部の変化率(平均)62.7%補償部
〃 45.7%
変化率(平均)の差 17.0%
となるが、活性部と補償部との差は、同一濃度でほぼ同
じようにあられれるので、CO500ppmでは、37
%に対応する感度(kΩ)が生じる。従って他の濃度値
例えば、11000ppでは74%の変化値が測定され
ることとなる。From the above table, depending on the voltage applied to the heater, that is, the sensor temperature, at 10V the rate of change (average) of the active part is 61.7% Compensation part #24.3% Difference in the rate of change (average) 37.4% At 12V the active part The rate of change in the active part (average) is 62.7%, the compensation part is 45.7%, the difference in the rate of change (average) is 17.0%, but the difference between the active part and the compensation part is almost the same at the same concentration. Because it is hail, at 500 ppm of CO, 37
A sensitivity (kΩ) corresponding to % occurs. Therefore, at other concentration values, for example, 11000 pp, a change value of 74% will be measured.
次に本発明はノーガス時の抵抗値が比較的安定しない半
導体センサについて下記の如き手段により安定性を高め
ようとするものである。いま、従来の5nOz半導体セ
ンサのノーガス時の特性(Ro)を、発熱体10■につ
いて調べてみると、第2表のとおりとなる。Next, the present invention attempts to improve the stability of a semiconductor sensor whose resistance value is relatively unstable in the absence of gas by the following means. Now, when we examine the characteristics (Ro) of the conventional 5nOz semiconductor sensor when no gas is present for the heating element 10, the results are as shown in Table 2.
上表の如く、活性部と補償部との関係は、必ずh
しも常に別記の変化値が顕著に現われない場合がかなり
多く、活性部及び補償部の夫々におけるRO特性もかな
り変動があることを免れない。As shown in the table above, the relationship between the active part and the compensation part is always h.In many cases, the change values listed separately do not appear significantly, and the RO characteristics of the active part and the compensation part vary considerably. I can't escape it.
本発明ではこの問題を解決するため、下記の如き傍熱型
固体熱伝導式を採用した。In order to solve this problem, the present invention employs an indirect heating type solid heat conduction method as described below.
第2図には、その方式により製作された活性部及び補償
部の半導体センサが示されている。まず、外径1.2〜
1.6φで、内径0.8〜1.2φ、長さ4〜6n程度
のセラミック管上に等間隔に20〜25μmのPt線を
ほぼ等間隔に抵抗が100〜150Ω(20℃)になる
ように巻いてなるコイル上に、活性部及び補傷部に使用
する前述の半導体粉末をSiO□コロイダル溶液で塗料
化したものを夫々20〜30μm程度の厚さに、できる
だけ平滑に塗装し、乾燥後650〜700℃で1〜16
5時間で焼結させた。FIG. 2 shows a semiconductor sensor with an active part and a compensation part manufactured by this method. First, the outer diameter is 1.2~
1.6φ, inner diameter 0.8 to 1.2φ, length about 4 to 6n, Pt wires of 20 to 25μm are placed at equal intervals on a ceramic tube with a resistance of 100 to 150Ω (at 20℃). On the coil wound like this, a SiO□ colloidal solution of the semiconductor powder used for the active part and the repair part is applied as a paint to a thickness of about 20 to 30 μm, as smooth as possible, and dried. 1-16 at 650-700℃
It was sintered in 5 hours.
ついで、磁性管の内側に加熱用のNi−Cr線のヒータ
を入れ、これを第3図に示す如く、組合わせて、保持体
(ステム)に固定する。図中符号7゜7′は夫々活性部
、補償部における信号取出口を符号9.9′はヒータの
端末を示している。Next, a Ni--Cr wire heater is placed inside the magnetic tube, and as shown in FIG. 3, the tubes are assembled and fixed to a holder (stem). In the figure, reference numerals 7° and 7' indicate signal output ports in the active section and compensation section, respectively, and 9 and 9' indicate terminals of the heater.
このような構成でセンサがヒータで加熱されると、CO
感度の適温である1506〜200℃となり、Pt線の
抵抗が、例えば常温(20°C)の約1.5〜1.6倍
に上昇する。この方式を本発明に係るブリッジ回路に適
用する場合にはPtコイルに自己加熱がないようにPt
線の抵抗を比較的大きくとるとさらに安定性が良くなる
。When the sensor is heated with a heater in this configuration, CO
The temperature becomes 1506 to 200°C, which is the optimum temperature for sensitivity, and the resistance of the Pt wire increases to, for example, about 1.5 to 1.6 times that of room temperature (20°C). When this method is applied to the bridge circuit according to the present invention, the Pt coil is
If the resistance of the wire is relatively high, the stability will be further improved.
このようにした傍熱型の構造により、ノーガス時の抵抗
は主としてPtコイルの抵抗に依存されることとなり感
度v0が安定化される。また。固体熱伝導タイプである
から、可燃性ガスがセンサの表面に触れて吸着されると
表面の放熱がよくなり、内部が冷却される。With this indirectly heated structure, the resistance when no gas is present depends mainly on the resistance of the Pt coil, and the sensitivity v0 is stabilized. Also. Since it is a solid heat conduction type, when flammable gas touches the surface of the sensor and is absorbed, heat dissipation from the surface improves and the interior is cooled.
従って、PtBの抵抗はガス濃度に比例して△Rだけ低
下し、単体の時より変動率は幾分小となるが、CO以外
の他ガス例えばH2等の感度を相殺するため有利である
。Therefore, the resistance of PtB decreases by ΔR in proportion to the gas concentration, and the fluctuation rate is somewhat smaller than when using PtB alone, but it is advantageous because it offsets the sensitivity of other gases than CO, such as H2.
次に、本センサにおける活性部と補償部とにおけるCO
感度差を、より大にするために本発明は下記の如き工夫
がなされた。Next, the CO in the active part and the compensation part in this sensor is
In order to further increase the difference in sensitivity, the invention has been devised as follows.
これは上記の固体熱伝導センサにおけるSnO,系半導
体の抵抗値及びPtコイルの抵抗値の範囲を定めてCO
感度を大にするものである。This is determined by determining the range of the resistance value of SnO, the system semiconductor, and the resistance value of the Pt coil in the solid-state thermal conductivity sensor mentioned above.
This increases sensitivity.
いま、固定熱伝導センサの抵抗値RはSnO2系半導体
の抵抗値r、とPtコイルの抵抗値rtとの合成値と考
えられ、両者は第4図に示す如(並列の関係にあるので
、
る抵抗値でαは恒数である
であられされ、各使用温度により一定値となる。Now, the resistance value R of the fixed heat conduction sensor is considered to be a composite value of the resistance value r of the SnO2-based semiconductor and the resistance value rt of the Pt coil, and the two are in a parallel relationship as shown in Figure 4 (since they are in a parallel relationship, α is a constant value, and it becomes a constant value depending on the operating temperature.
ここで、半導体の抵抗値r1が比較的小なる場合と比較
的大なる場合の夫々について、ガスの有無により抵抗値
がどのように変るかについて検討すると、
a、r、が比較的小なる場合例えばr、=lkΩ。Now, when we consider how the resistance value changes depending on the presence or absence of gas in cases where the resistance value r1 of the semiconductor is relatively small and relatively large, we find that when a and r are relatively small, For example, r, = lkΩ.
rz=150Ωであればノーガス時の合成抵抗R1は、 r、+r。If rz=150Ω, the combined resistance R1 at no gas time is r, +r.
の関係にある。There is a relationship between
また、SnO2系半導体の抵抗値r1は、焼結時のSn
O2粉末と焼結剤(例えば5iOzコロイダル液)の組
成に大きく変化することがわかり、特に焼結剤の量を増
すと抵抗値は大きくなる。In addition, the resistance value r1 of the SnO2-based semiconductor is the SnO2-based semiconductor during sintering.
It was found that the composition of the O2 powder and the sintering agent (for example, 5iOz colloidal liquid) changes greatly, and in particular, as the amount of the sintering agent increases, the resistance value increases.
さらに、Ptコイルの抵抗値は、
Rt =R,(1+αt) ・ ・ ・ ・ (
2)但しR,、R,は夫々温度t’c、0℃におけとな
るが、半導体がCOガスに触れてr、が50Ωに変化し
たとなると、r+’=50Ω。Furthermore, the resistance value of the Pt coil is Rt = R, (1+αt) ・ ・ ・ ・ (
2) However, R, and R are respectively at the temperature t'c and 0°C, but if the semiconductor comes into contact with CO gas and r changes to 50Ω, then r+'=50Ω.
rz=150Ω(変らず)となり、その合成抵抗R2は
、
となって、R,とR,”との差値△R3は、92.9Ω
と大きく変化する。rz=150Ω (unchanged), and the combined resistance R2 is as follows, and the difference value △R3 between R and R is 92.9Ω.
changes greatly.
b、一方、r、が比較的大なる場合例えばr。b.On the other hand, if r is relatively large, e.g.
=500にΩ、rz=150Ωであると、まず、ノーガ
ス時の合成抵抗Rhは、
となるが、半導体がCOガスに触れてrlが前記と同じ
割合で抵抗が下ったとすると、1000 : 50
= 500000 : x x=2500(Ω)即
ち、r、は500にΩから2.5にΩに下ったこととな
り、
となり、R1とR5″ との差値△R1は、8.4Ωし
かない。= 500 Ω and rz = 150 Ω, first, the combined resistance Rh when there is no gas is as follows. However, if the semiconductor comes into contact with CO gas and the resistance of rl decreases at the same rate as above, then it becomes 1000:50.
= 500000: x
このことから、aの如く、活性部にあっては、目的とす
るCoWl度(例えば500 ppm)において、半導
体の抵抗値がPtコイルの抵抗値より小さくなるように
rlを選ぶと、センサのCO感度が格段に大きくなる。From this, as shown in a, in the active region, if rl is selected so that the resistance value of the semiconductor is smaller than the resistance value of the Pt coil at the target CoWl level (for example, 500 ppm), the CO of the sensor will be reduced. Sensitivity is greatly increased.
なお、補償部にあっては、COに対する抵抗の変化は殆
んどないものが選ばれるので左程問題はないが、−名目
的とするCO濃度でもPtコイル抵抗より小さくならな
いようなr2を有するものが選択されることが望ましい
。For the compensation section, a component with almost no change in resistance due to CO is selected, so there is no problem as shown on the left; It is desirable that something is selected.
以下、具体例について述べると、本発明に係るSnO□
半導体のcOガスによる抵抗の変化率は、c。Hereinafter, specific examples will be described. SnO□ according to the present invention
The rate of change in resistance of a semiconductor due to cO gas is c.
500ppmで、
活性部 SnO2/Pd、 Pt 60%
補償部 Snug/Sn 20%あり
、20℃では、約100ΩのPtコイルは、使用温度(
220’〜240℃)では、その抵抗が150〜160
Ωとなるので、活性部の方は、c。At 500ppm, active part SnO2/Pd, Pt 60%
Compensation section Snug/Sn 20%, at 20°C, a Pt coil of approximately 100Ω will exceed the operating temperature (
220'~240℃), its resistance is 150~160
Ω, so the active part is c.
500ppmで150Ω以下になるためには、ノーガス
時に375Ω程度の抵抗値を有するものにすればよく、
この抵抗値を保持するように焼結剤の配合を決めればよ
い。In order to have a resistance of 150Ω or less at 500ppm, it is sufficient to have a resistance value of about 375Ω when there is no gas.
The combination of the sintering agent may be determined so as to maintain this resistance value.
また、補償部の方は、CO500ppmでは上述の如く
20%程度抵抗値が変化するので、ノーガス時375Ω
位になるように配合してもせいぜい300Ωにしか変化
せず、問題がないことがわかる。In addition, the resistance value of the compensation section changes by about 20% at 500 ppm of CO as mentioned above, so it is 375 Ω when no gas is present.
It can be seen that even if the resistance is mixed so that the resistance is about 300Ω, the resistance changes to 300Ω at most, and there is no problem.
実機にあっては、ノーガス時、
のセンサが、CO500ppn+の雰囲気中では、とな
り、合成抵抗の差値△Rは、
△R=R,°−R,’=100−75=25 (Ω)と
なる。In the actual machine, when there is no gas, the sensor becomes as follows in an atmosphere of 500 ppn+ CO, and the difference value △R of the combined resistance is △R=R,°-R,'=100-75=25 (Ω). Become.
この活性部及び補償部を第1図のブリフジ回路に適用し
て、ブリッジ電圧6Vとすると、ガス感度△■は、
の弐に、△R=25(Ω)、R=375(Ω)、V、=
6 (V)の代入することにより、△■ズ
x 6 = 0.1 (V) =100(
mV)X375
の出力が得られる。When this active part and compensation part are applied to the bridge circuit shown in Fig. 1 and the bridge voltage is 6V, the gas sensitivity △■ is as follows: △R=25 (Ω), R=375 (Ω), V ,=
6 By substituting (V), △■ Z
x 6 = 0.1 (V) = 100(
An output of mV)X375 is obtained.
なお、COガスの吸着によりPtコイルの抵抗が夫々1
50−△RI°、150Ω−△R2’となり、また、△
R,’>△R2゛であるから、さらに、大きな出力が得
られる場合がある。In addition, due to the adsorption of CO gas, the resistance of the Pt coil increases by 1
50-△RI°, 150Ω-△R2', and △
Since R,'>ΔR2', an even larger output may be obtained.
以上の如く、本発明にあっては、SnO□半導体の抵抗
値に関し、ノーガス時と一定濃度OCO中とを夫々測定
してその変化率を求めることにより、100〜200p
pmの如き低濃度のガスに対しても、零点が安定して1
00mV以上の出力を取り出すセンサが製作できるもの
である。As described above, in the present invention, the resistance value of the SnO
Even for gases with low concentrations such as pm, the zero point remains stable at 1.
It is possible to manufacture a sensor that outputs an output of 00 mV or more.
本発明にあっては、2種類の組成の異なる、SnO2半
導体を組合わせCOセンサを構成するものであって、H
z + C2)ISOHI icJ+o等の他ガスの感
度が活性部と補償部との関係において相殺されCO感度
のみを取出すことが可能である。In the present invention, a CO sensor is constructed by combining two types of SnO2 semiconductors with different compositions, and H
The sensitivity of other gases such as z + C2) ISOHI icJ+o is canceled out in the relationship between the active part and the compensation part, and it is possible to extract only the CO sensitivity.
ただし、半導体センサの組合わせによりつくられるCO
センサではノーガス時の抵抗値を同一にすることがかな
り困難であることから、歩留りが悪いことは避けられな
い。However, the CO produced by the combination of semiconductor sensors
In sensors, it is quite difficult to make the resistance value the same when there is no gas, so it is inevitable that the yield will be poor.
これを解決する手段として、前述の固体熱伝導式が導入
される。ノーガス時のセンサの抵抗は実質的にPtコイ
ルの抵抗に依存するため、零点調整が容易で使用し易い
。特に、半導体の抵抗値がCOガスの一定値でPtコイ
ルの抵抗値以下になるよう製作することにより、そのC
O?M度で少なくとも100mV以上の出力が得られて
いる。丁寧に調整して製作するのが煩瑣であるときには
、C0100ppIIl、1OOIIlv用、200p
pm、100mV用等仕分する方法もとられる。As a means to solve this problem, the above-mentioned solid heat conduction method is introduced. Since the resistance of the sensor during no gas substantially depends on the resistance of the Pt coil, zero point adjustment is easy and it is easy to use. In particular, by manufacturing the semiconductor so that the resistance value is less than the resistance value of the Pt coil at a constant value of CO gas, the C
O? An output of at least 100 mV or more was obtained at M degrees. If it is too troublesome to make careful adjustments, use C0100ppIIl, 1OOIIlv, 200p.
A method of sorting for pm, 100 mV, etc. is also used.
半導体センサは、接触燃焼式センサ等と異なりガス濃度
と感度出力との間に直線比例関係が求められない通常で
あるが、本発明に係る低濃度における高感度特性を利用
すれば、COの選択性が改善され、警報器用として十分
役立つものとなりうる。Semiconductor sensors, unlike catalytic combustion type sensors, do not normally require a linear proportional relationship between gas concentration and sensitivity output, but if the high sensitivity characteristics at low concentrations according to the present invention are used, CO selection This improves the performance and can make it useful as an alarm device.
本発明は以上の構成に基づくもので、半導体センサにお
けるCO感度を格段に向上させ、従来センサにおける選
択性がない欠点が大幅に改善されたものであって、特に
固体熱伝導式を採用することにより警報器用として十分
使用できることとなり極めて有用な発明である。The present invention is based on the above-described configuration, and significantly improves the CO sensitivity of a semiconductor sensor, and greatly improves the lack of selectivity in conventional sensors. In particular, it adopts a solid heat conduction type. This makes it possible to fully use it as an alarm device, making it an extremely useful invention.
第1図は、本発明に係るブリッジ回路の説明図、第2図
は本発明に係るセンサの活性部の説明図、第3図は活性
部と補償部との連結状態を示す説明図、第4図は、固体
熱伝導式におけるPtコイル抵抗とSnO□半導体抵抗
の配列を示す説明図である。
1・・・活性部、2・・・補償部、rl、r2.r3・
・・ブリッジ抵抗、4・・・感度計、5・・・ブリッジ
電源、6・・・セラミック管、8・・・Ptコイル、9
・・・発熱体。FIG. 1 is an explanatory diagram of the bridge circuit according to the present invention, FIG. 2 is an explanatory diagram of the active part of the sensor according to the present invention, FIG. 3 is an explanatory diagram showing the connection state of the active part and the compensation part, FIG. 4 is an explanatory diagram showing the arrangement of the Pt coil resistance and the SnO□ semiconductor resistance in the solid heat conduction type. 1... Active part, 2... Compensation part, rl, r2. r3・
...Bridge resistance, 4...Sensitivity meter, 5...Bridge power supply, 6...Ceramic tube, 8...Pt coil, 9
...heating element.
Claims (1)
有する活性部1と補償部2とを設け、その対辺に並列し
て所定のブリッジ抵抗にr_1、r_2、r_3を直列
に配置し、活性部1と補償部2との中間点3とブリッジ
抵抗r_2との間にCOガス感度が相等する電圧値で表
示される感度計4を設け、また、上記活性部1及び補償
部2に直流電圧を印加するブリッジ電源5を配置するブ
リッジ回路をもって形成される一酸化炭素センサであっ
て、活性部1にはCO感度のみ増感されたSnO_2/
Pd、Pt半導体が使用され、また、補償部2にはCO
感度が増感されてないSnO_2/Sn半導体が使用さ
れて、CO雰囲気中で活性部1及び補償部2との間に生
じる抵抗値差に基づいてCO感度を求めることを特徴と
する一酸化炭素センサ。 2、セラミック管上に同一抵抗のPt線コイルを固定し
てなる活性部及び補償部に各半導体成分を焼結せしめる
とともに該セラミック管に発熱体を内蔵せしめる請求項
1に記載の一酸化炭素センサ。 3、活性部におけるノーガス時のPtコイルと半導体の
合成抵抗値が使用時のPtコイルの抵抗値より大である
とともに、COガス中では半導体の抵抗値がPtコイル
の抵抗値より小なる如くし、また、補償部におけるノー
ガス時の抵抗値を上記活性部におけるノーガス時の抵抗
値と同一にするとともに、上記COガス中では活性部に
おけるPtコイルの抵抗値より大ならしめる如く各Sn
O_2系半導体及び焼結剤の組成が定められる請求項1
に記載の一酸化炭素センサ。[Claims] 1. An active part 1 and a compensation part 2 are provided which are arranged in series and have approximately the same resistance value when no gas is present, and r_1, r_2, r_3 are connected to predetermined bridge resistances in parallel on the opposite side. A sensitivity meter 4 is arranged in series between the intermediate point 3 between the active part 1 and the compensation part 2 and the bridge resistor r_2, and the sensitivity meter 4 displays the CO gas sensitivity with an equal voltage value. This is a carbon monoxide sensor formed with a bridge circuit in which a bridge power supply 5 is arranged to apply a DC voltage to a compensating part 2, and the active part 1 is equipped with SnO_2/2, which has only the CO sensitivity sensitized.
Pd, Pt semiconductors are used, and the compensation section 2 is made of CO.
Carbon monoxide, characterized in that a SnO_2/Sn semiconductor whose sensitivity has not been sensitized is used, and the CO sensitivity is determined based on the resistance difference generated between the active part 1 and the compensation part 2 in a CO atmosphere. sensor. 2. The carbon monoxide sensor according to claim 1, wherein each semiconductor component is sintered in the active part and the compensation part, which are formed by fixing a Pt wire coil of the same resistance on a ceramic tube, and the ceramic tube has a built-in heating element. . 3. The combined resistance value of the Pt coil and semiconductor in the active region when no gas is present is greater than the resistance value of the Pt coil during use, and the resistance value of the semiconductor is smaller than the resistance value of the Pt coil in CO gas. In addition, each Sn
Claim 1, wherein the composition of the O_2-based semiconductor and the sintering agent is determined.
Carbon monoxide sensor as described in .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13837889A JPH032654A (en) | 1989-05-31 | 1989-05-31 | Carbon monoxide sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP13837889A JPH032654A (en) | 1989-05-31 | 1989-05-31 | Carbon monoxide sensor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH032654A true JPH032654A (en) | 1991-01-09 |
Family
ID=15220535
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP13837889A Pending JPH032654A (en) | 1989-05-31 | 1989-05-31 | Carbon monoxide sensor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH032654A (en) |
-
1989
- 1989-05-31 JP JP13837889A patent/JPH032654A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US3607084A (en) | Combustible gas measurement | |
| US4396899A (en) | Platinum thin film resistance element and production method therefor | |
| US3699803A (en) | Semiconductor element for detecting gases and meter for measuring component concentration of a gas mixture | |
| KR940002635B1 (en) | Humidity sensor | |
| US4587104A (en) | Semiconductor oxide gas combustibles sensor | |
| US4036592A (en) | Detection of carbon monoxide | |
| JPH0517650Y2 (en) | ||
| JPH032654A (en) | Carbon monoxide sensor | |
| US5681111A (en) | High-temperature thermistor device and method | |
| EP0038078B1 (en) | Gas sensor | |
| JP2615138B2 (en) | Composite gas sensor | |
| KR930000541B1 (en) | Thick type element for detecting gas | |
| KR102773775B1 (en) | Gas sensor detecting module using wheatstone bridge circuit, and gas sensor having it | |
| Ramalingam et al. | Study of robust thin film PT-1000 temperature sensors for cryogenic process control applications | |
| Tew | Calibration of cryogenic resistance thermometers between 0.65 K and 165 K on the international temperature scale of 1990 | |
| JPH053974Y2 (en) | ||
| KR900003928B1 (en) | Gas detector | |
| JPS6138820B2 (en) | ||
| KR900003929B1 (en) | Gas detector | |
| JPH053973Y2 (en) | ||
| KR900003930B1 (en) | Gas detector | |
| JPH0447658Y2 (en) | ||
| KR20250028332A (en) | Gas sensor detecting module using wheatstone bridge circuit, and gas sensor having it | |
| Gillette | Measurement of static strain at 2,000° F: Work is being done at Hughes Aircraft Company using capacitance strain gages to measure static strains at temperatures up to and including 2,000° F | |
| JPS5848615Y2 (en) | Gas Kenchiki |