JP2945315B2 - Method and apparatus for detecting insulator fouling - Google Patents
Method and apparatus for detecting insulator foulingInfo
- Publication number
- JP2945315B2 JP2945315B2 JP32427795A JP32427795A JP2945315B2 JP 2945315 B2 JP2945315 B2 JP 2945315B2 JP 32427795 A JP32427795 A JP 32427795A JP 32427795 A JP32427795 A JP 32427795A JP 2945315 B2 JP2945315 B2 JP 2945315B2
- Authority
- JP
- Japan
- Prior art keywords
- insulator
- measuring section
- amount
- fouling
- contamination
- 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 - Fee Related
Links
Landscapes
- Testing Relating To Insulation (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Insulators (AREA)
Description
【0001】[0001]
【発明の属する技術分野】本発明は、碍子表面の汚損量
を正確に求めるための碍子の汚損検出方法及び装置に関
するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and an apparatus for detecting contamination of an insulator for accurately determining the amount of contamination on the surface of the insulator.
【0002】[0002]
【従来の技術】碍子表面に設けられた電極間に電圧を印
加し、漏洩電流の値から碍子表面の汚損量を測定する方
法は従来から知られている。ところが、漏洩電流の値は
碍子表面の汚損量の他に、湿潤状態(湿度)によっても
大きく変化するので、湿潤状態の影響をキャンセルする
ため、碍子表面を十分に湿潤させた状態で測定を行う必
要があった。しかしこのためには表面を湿潤させるため
の蒸気室等の湿潤装置が不可欠となるうえ、湿潤前の状
態における現実の碍子の汚損量を正確に求めることがで
きないという問題があった。2. Description of the Related Art A method of measuring the amount of contamination on an insulator surface from a value of a leakage current by applying a voltage between electrodes provided on the surface of the insulator is conventionally known. However, since the value of the leakage current varies greatly depending on the wet state (humidity) in addition to the amount of contamination on the insulator surface, the measurement is performed with the insulator surface sufficiently wetted to cancel the influence of the wet state. Needed. However, for this purpose, a wetting device such as a steam chamber for wetting the surface is indispensable, and there is a problem that the actual amount of contamination of the insulator before wetting cannot be accurately obtained.
【0003】[0003]
【発明が解決しようとする課題】本発明は上記した従来
の問題点を解決し、湿潤装置を必要とせず、湿潤されな
い現実の碍子の汚損量を正確に求めることができる碍子
の汚損検出方法及び装置を提供するためになされたもの
である。SUMMARY OF THE INVENTION The present invention solves the above-mentioned conventional problems, and does not require a wetting device, and a method for detecting contamination of an insulator which can accurately determine the amount of contamination of an actual insulator which is not wetted. It was made to provide a device.
【0004】[0004]
【課題を解決するための手段】上記の課題を解決するた
めになされた本発明の碍子の汚損検出方法は、碍子の表
面に、表面抵抗の小さい第1の測定部と、これより表面
抵抗の大きい第2の測定部とを設けておき、これらの測
定部に電圧を印加したときの漏洩電流I1 、I2 を比較
演算して碍子の汚損量を求めることを特徴とするもので
ある。なおこの比較演算は、漏洩電流I1 、I2 に対応
する両方の測定部の湿度及び汚損量が同一であることを
利用して比較演算を繰り返し、汚損量の収束値を求める
方法によって行うことが好ましい。また上記の課題を解
決するためになされた本発明の碍子の汚損検出装置は、
碍子の表面に設けられた表面抵抗の小さい第1の測定部
と、前記碍子と同一または近傍の碍子の表面に設けられ
た表面抵抗の大きい第2の測定部と、これらの測定部に
電圧を印加する電圧印加手段と、各測定部に流れる漏洩
電流I1 、I2 の検出手段と、これらの漏洩電流I1 、
I2 を比較演算することにより碍子の汚損量を求める演
算手段とを備えたことを特徴とするものである。SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, a method for detecting contamination of an insulator according to the present invention comprises: a first measuring section having a small surface resistance on a surface of the insulator; A large second measuring section is provided, and leakage currents I 1 and I 2 when a voltage is applied to these measuring sections are compared to calculate the amount of contamination of the insulator. Note that this comparison operation is performed by a method in which the comparison operation is repeated by using the fact that the humidity and the contamination amount of both measurement units corresponding to the leakage currents I 1 and I 2 are the same, and a convergence value of the contamination amount is obtained. Is preferred. Further, an insulator fouling detection device of the present invention made in order to solve the above problems,
A first measuring section having a small surface resistance provided on the surface of the insulator, a second measuring section having a large surface resistance provided on the surface of the insulator at or near the insulator, and applying a voltage to these measuring sections. voltage applying means for applying a detecting means of the leakage current I 1, I 2 flowing through each measurement section, these leakage currents I 1,
It is characterized in that a calculation means for calculating a fouling of the insulator by comparing calculating the I 2.
【0005】なお、表面抵抗の異なる第1及び第2の測
定部は、導電率の異なる2種類の半導体釉薬を碍子表面
に施釉することにより構成してもよく、あるいは表面抵
抗の異なる第1の測定部を半導体釉薬により構成し、こ
れよりも表面抵抗の大きい第2の測定部を通常の釉薬に
より構成してもよい。The first and second measuring units having different surface resistances may be constituted by glazing the insulator surface with two kinds of semiconductor glazes having different electric conductivity, or the first and second measuring units having different surface resistances. The measurement unit may be formed of a semiconductor glaze, and the second measurement unit having a larger surface resistance may be formed of a normal glaze.
【0006】[0006]
【発明の実施の形態】以下に本発明の実施の形態を、図
面を参照しつつ詳細に説明する。図1は本発明の装置の
概略図であり、1は半導体釉薬が施釉された碍子、2は
通常の釉薬が施釉された測定対象となる碍子、3、3は
その上下に配置されたダミー碍子である。ここで用いら
れる半導体釉薬自体は公知のものであり、例えば酸化
錫、酸化鉄のような半導電性の酸化金属粉末を釉薬中に
混入させたものであって、その混入量を変えることによ
り導電率を異ならせることができる。碍子1と碍子2と
は湿潤状態(湿度)及び汚損状態が同一となるよう、近
傍に配置しておくものとするが、同一の碍子であっても
差し支えない。Embodiments of the present invention will be described below in detail with reference to the drawings. FIG. 1 is a schematic view of an apparatus of the present invention, wherein 1 is an insulator glazed with a semiconductor glaze, 2 is an insulator to be measured which is glazed with a normal glaze, and 3 and 3 are dummy insulators arranged above and below the insulator. It is. The semiconductor glaze itself used here is a known one. For example, a semiconductive metal oxide powder such as tin oxide or iron oxide is mixed in the glaze, and the conductive amount is changed by changing the mixing amount. The rates can be different. The insulator 1 and the insulator 2 are arranged close to each other so that the wet state (humidity) and the soiled state are the same, but the same insulator may be used.
【0007】半導体釉薬が施釉された碍子1及び通常の
釉薬が施釉された碍子2の表面には、適宜の電極によっ
て第1の測定部4と第2の測定部5とが設けられてい
る。この例では第1の測定部4の表面抵抗値は乾燥状態
においてはほぼ10MΩのレベルにあり、第2の測定部5
の表面抵抗値は乾燥状態においては1000MΩのレベルに
ある。6はこれらの第1の測定部4と第2の測定部5と
に電圧を印加する電圧印加手段である。また各測定部
4、5には、電圧を印加されたときに流れる漏洩電流を
検出するための検出手段7、8が接続されている。A first measuring unit 4 and a second measuring unit 5 are provided on the surfaces of the insulator 1 glazed with the semiconductor glaze and the insulator 2 glazed with the usual glaze by appropriate electrodes. In this example, the surface resistance value of the first measuring unit 4 is at a level of approximately 10 MΩ in the dry state, and the second measuring unit 5
Has a level of 1000 MΩ in a dry state. Reference numeral 6 denotes voltage applying means for applying a voltage to the first measuring unit 4 and the second measuring unit 5. Further, the measuring units 4 and 5 are connected to detecting means 7 and 8 for detecting a leakage current flowing when a voltage is applied.
【0008】図2はこの測定装置の等価回路を示すもの
であり、R1 は半導体釉薬による抵抗、R2 は汚損量に
対応する碍子表面の抵抗である。電圧印加手段6により
電圧Vを印加した場合、第1の測定部4にはI1 =V/
(1/ R1 +1/R2)の漏洩電流が流れ、第2の測定部5に
はI2 =V/R2 の漏洩電流が流れることとなるから、
I1>I2 となる。そしてこれらの漏洩電流I1 、I2 は
検出手段7、8により測定され、演算手段9により次の
とおり比較演算される。FIG. 2 shows an equivalent circuit of this measuring device, where R 1 is the resistance of the semiconductor glaze, and R 2 is the resistance of the insulator surface corresponding to the amount of contamination. When the voltage V is applied by the voltage applying means 6, the first measuring unit 4 applies I 1 = V /
Since a leakage current of (1 / R 1 + 1 / R 2 ) flows and a leakage current of I 2 = V / R 2 flows in the second measuring section 5,
I 1 > I 2 . Then, these leakage currents I 1 and I 2 are measured by the detecting means 7 and 8 and are compared and calculated by the calculating means 9 as follows.
【0009】図3と図4は本発明の比較演算の方法を説
明するグラフである。まず図3には、碍子表面の湿潤状
態と表面漏洩電流との関係が示されている。前記したと
おり、碍子1の測定部4と碍子2の測定部5の湿度(湿
潤状態)及び汚損量は同一であるが、前式から明らかな
ように漏洩電流I1 、I2 はI1>I2 となる。また図3
には右拡がりの2本ずつの曲線が実線で示されている
が、下側が汚損量ゼロの場合、上側が汚損量最大の場合
を示している。下側の曲線は実験により正確に決定され
るが、上側の曲線は正確には決定できず便宜的に図示し
たものである。図3の汚損量ゼロの曲線は、データとし
て予め演算手段9に記憶させておく。FIGS. 3 and 4 are graphs for explaining a comparison operation method according to the present invention. First, FIG. 3 shows the relationship between the wet state of the insulator surface and the surface leakage current. As described above, the humidity (wet state) and the amount of contamination of the measuring unit 4 of the insulator 1 and the measuring unit 5 of the insulator 2 are the same, but as is clear from the above expression, the leakage currents I 1 and I 2 are I 1 > the I 2. FIG.
, Two curves each extending to the right are shown by solid lines. The lower side shows the case where the amount of contamination is zero, and the upper side shows the case where the amount of contamination is maximum. The lower curve is determined accurately by experiment, while the upper curve is not accurately determined and is shown for convenience. The curve with zero contamination amount shown in FIG. 3 is stored in advance in the arithmetic means 9 as data.
【0010】本発明においては、上記のように測定され
た漏洩電流I1 、I2 の値が、図3のI01、I02である
場合にはデータを取り込まない。これは碍子表面が全く
湿潤しておらず有効な測定が不可能なためである。ま
た、測定された漏洩電流I1 、I2 の値が汚損量ゼロの
曲線X1 、X2 と交わる点P1 、P2 の湿度A1 、A2
を求め、A1 =A2 の場合には汚損量がゼロと判断す
る。しかし多くの場合にはA1 <A2 であるので、次の
ように比較演算を行う。In the present invention, no data is taken in when the values of the leakage currents I 1 and I 2 measured as described above are I 01 and I 02 in FIG. This is because the insulator surface is not wet at all and effective measurement is impossible. Further, the humidity A 1 , A 2 at the points P 1 , P 2 where the measured values of the leakage currents I 1 , I 2 intersect the curves X 1 , X 2 with zero contamination amount, respectively.
Is determined, and when A 1 = A 2 , the amount of contamination is determined to be zero. However, in many cases, A 1 <A 2 , so the comparison operation is performed as follows.
【0011】まず漏洩電流I1 の値が汚損量ゼロの曲線
X1 と交わる点P1 と、漏洩電流I2 の値が汚損量ゼロ
の曲線X2 と交わる点P2 とを対比する。ここで両者の
湿度は同一のはずであるから、点P1 から下ろした垂線
P1 A1 と水平線I2 P2 との交点P3 よりも右側部
分、即ちP3 からP2 までの部分については無視するこ
とができる。換言すれば、この範囲内には汚損量の正解
値は存在しないのである。[0011] First the value of the leakage current I 1 and P 1 point of intersection with the curve X 1 fouling amount zero, comparing the point P 2 value of the leakage current I 2 intersects the curve X 2 fouling zero amount. Here, since both humidity should be the same, the right side of the intersection P 3 of the perpendicular P 1 A 1 and the horizontal I 2 P 2 lowered from the point P 1 , that is, the portion from P 3 to P 2 Can be ignored. In other words, there is no correct value of the amount of contamination within this range.
【0012】そこでこの点P3 を通る曲線X3 (図3に
鎖線で表示)を引くと、それに対応する測定対象となる
碍子2の汚損量が仮に求められる。碍子2の汚損量と碍
子1の汚損量とは等しいはずであるから、この汚損量を
碍子1側に投影し、その汚損量に対応する曲線X4 を引
く。そして水平線I1 P1 と曲線X4 との交点をP4 と
する。この一連の比較演算によって、点P1 と点P4 と
の間の範囲内には汚損量の正解値は存在しないことが分
かる。Therefore, when a curve X 3 (indicated by a chain line in FIG. 3) passing through this point P 3 is drawn, the corresponding amount of contamination of the insulator 2 to be measured is temporarily obtained. Since it should be equal to the fouling of fouling amount and insulator 1 of the insulator 2, and projecting this fouling amount insulator 1 side, pulling the curve X 4 corresponding to the fouling amount. The intersection of the horizontal line I 1 P 1 and the curve X 4 is defined as P 4 . This series of comparison operation in the range between the point P 1 and point P 4 it can be seen that absent correct value of fouling amount.
【0013】次に、点P4 を出発点として同様の比較演
算を繰り返せば、図4のグラフに示されるように汚損量
−湿度のグラフ上で演算結果は次第に収束し、正しい汚
損量が求められることとなる。この演算は図4のグラフ
に示される碍子1、碍子2に対応する2本の曲線の交点
を求めることと同じである。従って、このような2本の
曲線が容易に得られる場合には、必ずしも上記したよう
な収束値を求める演算を繰り返す必要はない。Next, when the same comparison operation is repeated starting from the point P 4 , the calculation results gradually converge on the graph of the amount of contamination-humidity as shown in the graph of FIG. Will be done. This calculation is the same as finding the intersection of two curves corresponding to the insulator 1 and the insulator 2 shown in the graph of FIG. Therefore, when such two curves are easily obtained, it is not always necessary to repeat the calculation for obtaining the convergence value as described above.
【0014】上記したように、本発明によれば従来のよ
うに蒸気室等により測定部を完全に湿潤させる必要がな
く、湿潤されない現実の碍子の汚損量を正確に求めるこ
とができる利点がある。しかし、測定部4、5に冷却素
子を組み込んでおき、測定不能なほどに碍子が乾燥して
いる場合には、冷却素子により測定部4、5を結露させ
て湿潤させつつ測定を行うことは可能である。As described above, according to the present invention, it is not necessary to completely wet the measuring section by the steam chamber or the like as in the prior art, and there is an advantage that the amount of contamination of the actual insulator that is not wet can be accurately obtained. . However, if a cooling element is incorporated in the measuring units 4 and 5 and the insulator is too dry to be measured, it is not possible to perform measurement while dewing and moistening the measuring units 4 and 5 with the cooling element. It is possible.
【0015】なお、本発明による汚損量の測定において
は、電圧の印加を間欠的に行い、例えば30分に1回程度
の時間間隔で測定を行うことが好ましい。これは常時電
圧を印加すると漏洩電流のジュール熱で測定部4、5が
乾燥してしまうためである。また所定の時間間隔で測定
を行えば汚損量の経時的な変化の傾向が把握できるの
で、前回の測定により得られた汚損量の値を参照しつつ
汚損量を求めることができる。この結果、明らかな異常
値をデータから外すことが可能となり、信頼性の高い測
定が可能となる。In the measurement of the amount of fouling according to the present invention, it is preferable that the voltage is applied intermittently, for example, at a time interval of about once every 30 minutes. This is because, when a voltage is constantly applied, the measuring units 4 and 5 are dried by the Joule heat of the leakage current. Further, if the measurement is performed at predetermined time intervals, the tendency of the change in the amount of contamination over time can be grasped, so that the amount of contamination can be obtained while referring to the value of the amount of contamination obtained by the previous measurement. As a result, apparent abnormal values can be excluded from the data, and highly reliable measurement can be performed.
【0016】[0016]
【発明の効果】以上に説明したように、本発明は表面抵
抗の小さい第1の測定部と、これより表面抵抗の大きい
第2の測定部とを設け、これらの測定部から得られた漏
洩電流を比較演算して汚損量を求めるようにしたので、
従来のように測定部を完全に湿潤させて測定を行う必要
がなく、湿潤されない現実の碍子の汚損量を正確に求め
ることができる利点がある。またこれにより蒸気室等の
湿潤装置を無くすることもできるので、装置の小型化を
図ることができる利点もある。As described above, according to the present invention, the first measuring section having a small surface resistance and the second measuring section having a larger surface resistance are provided, and the leakage obtained from these measuring sections is provided. Since the amount of contamination was calculated by comparing the current,
It is not necessary to perform the measurement by completely wetting the measuring unit as in the related art, and there is an advantage that the actual amount of contamination of the non-wetted insulator can be accurately obtained. This also eliminates the need for a wetting device such as a steam chamber, and has the advantage that the size of the device can be reduced.
【図1】本発明の汚損検出装置の概略図である。FIG. 1 is a schematic diagram of a fouling detection device of the present invention.
【図2】図1の等価回路図である。FIG. 2 is an equivalent circuit diagram of FIG.
【図3】湿度と表面漏洩電流との関係を示すグラフであ
る。FIG. 3 is a graph showing a relationship between humidity and surface leakage current.
【図4】湿度と汚損量との関係を示すグラフである。FIG. 4 is a graph showing the relationship between humidity and the amount of fouling.
1 半導体釉薬が施釉された碍子、2 測定対象となる
碍子、3 ダミー碍子、4 第1の測定部、5 第2の
測定部、6 電圧印加手段、7 漏洩電流の検出手段、
8 漏洩電流の検出手段、9 演算手段1 insulator glazed with a semiconductor glaze, 2 insulators to be measured, 3 dummy insulators, 1st measuring section, 5th measuring section, 6 voltage applying means, 7 leakage current detecting means,
8 Leakage current detection means, 9 Operation means
Claims (8)
定部と、これより表面抵抗の大きい第2の測定部とを設
けておき、これらの測定部に電圧を印加したときの漏洩
電流I1 、I2 を比較演算して碍子の汚損量を求めるこ
とを特徴とする碍子の汚損検出方法。1. A first measuring section having a small surface resistance and a second measuring section having a higher surface resistance are provided on the surface of an insulator, and leakage occurs when a voltage is applied to these measuring sections. A method for detecting contamination of an insulator, comprising calculating an amount of contamination of the insulator by comparing the currents I 1 and I 2 .
定部と、これより表面抵抗の大きい第2の測定部とを設
けておき、これらの測定部に電圧を印加したときの漏洩
電流I1 、I2 に対応する両方の測定部の湿度及び汚損
量が同一であることを利用して比較演算を繰り返し、汚
損量の収束値を求めることを特徴とする碍子の汚損検出
方法。2. A first measuring section having a small surface resistance and a second measuring section having a higher surface resistance are provided on the surface of the insulator, and leakage occurs when a voltage is applied to these measuring sections. A method for detecting fouling of an insulator, wherein a comparison operation is repeated by using the fact that the humidity and the fouling amount of both measurement units corresponding to the currents I 1 and I 2 are the same, and a convergence value of the fouling amount is obtained.
隔で測定を行う請求項1又は2に記載の碍子の汚損検出
方法。3. The method for detecting contamination of an insulator according to claim 1, wherein the voltage is applied intermittently and the measurement is performed at predetermined time intervals.
照しつつ汚損量を求める請求項2に記載の碍子の汚損検
出方法。4. The method for detecting fouling of an insulator according to claim 2, wherein the fouling amount is obtained by referring to the value of the fouling amount obtained by the previous measurement.
測定部を湿潤させつつ測定を行う請求項1〜4のいずれ
かに記載の碍子の汚損検出方法。5. The method for detecting contamination of an insulator according to claim 1, wherein a cooling element is incorporated in the measuring section, and the measurement is performed while the measuring section is moistened by dew condensation.
第1の測定部と、前記碍子と同一または近傍の碍子の表
面に設けられた表面抵抗の大きい第2の測定部と、これ
らの測定部に電圧を印加する電圧印加手段と、各測定部
に流れる漏洩電流I1 、I2 の検出手段と、これらの漏
洩電流I1 、I2 を比較演算することにより碍子の汚損
量を求める演算手段とを備えたことを特徴とする碍子の
汚損検出装置。6. A first measuring section provided on the surface of the insulator and having a small surface resistance, a second measuring section provided on the surface of the insulator at or near the insulator and having a large surface resistance, and Voltage application means for applying a voltage to the measuring section, means for detecting leakage currents I 1 and I 2 flowing through each measuring section, and the amount of contamination of the insulator is determined by comparing and calculating these leakage currents I 1 and I 2. A detector for detecting fouling of an insulator, comprising a calculating means.
が、2種類の半導体釉薬により構成されたものである請
求項6に記載の碍子の汚損検出装置。7. The insulator fouling detecting device according to claim 6, wherein the first and second measuring units having different surface resistances are constituted by two kinds of semiconductor glazes.
薬により構成され、表面抵抗の大きい第2の測定部が通
常の釉薬により構成されたものである請求項6に記載の
碍子の汚損検出装置。8. The insulator according to claim 6, wherein the first measuring section having a different surface resistance is made of a semiconductor glaze, and the second measuring section having a large surface resistance is made of a normal glaze. Detection device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32427795A JP2945315B2 (en) | 1995-12-13 | 1995-12-13 | Method and apparatus for detecting insulator fouling |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP32427795A JP2945315B2 (en) | 1995-12-13 | 1995-12-13 | Method and apparatus for detecting insulator fouling |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH09166565A JPH09166565A (en) | 1997-06-24 |
| JP2945315B2 true JP2945315B2 (en) | 1999-09-06 |
Family
ID=18164017
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP32427795A Expired - Fee Related JP2945315B2 (en) | 1995-12-13 | 1995-12-13 | Method and apparatus for detecting insulator fouling |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2945315B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP6536602B2 (en) * | 2017-02-28 | 2019-07-03 | 日新電機株式会社 | Pollution detection device |
| CN119881563B (en) * | 2025-03-28 | 2025-06-06 | 南京工程学院 | A composite insulator state prediction method based on improved physical model of surface resistance and leakage current |
-
1995
- 1995-12-13 JP JP32427795A patent/JP2945315B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH09166565A (en) | 1997-06-24 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN111537561A (en) | Method and system for measuring interface thermal resistance | |
| JP2945315B2 (en) | Method and apparatus for detecting insulator fouling | |
| JPH02249251A (en) | Method of measuring physical characteristic of buried channel | |
| JP2001508880A (en) | Operating method of gas sensor | |
| JP3103449B2 (en) | Soil detection method | |
| JPH0353184Y2 (en) | ||
| JP2731685B2 (en) | Soil detection sensor | |
| JPH0631536A (en) | Measurement of temperature of wire on wire electric discharge machine | |
| EP0086415B1 (en) | Humidity sensitive device | |
| JP3067921B2 (en) | Soil detection sensor | |
| JP3103450B2 (en) | Soil detection method | |
| JP3106660B2 (en) | Humidity detector | |
| JP3638067B2 (en) | A method for determining the position of a nail punched into a hot water pipe of a floor heating system | |
| JPS5888645A (en) | Measuring sensor for content of oxygen in gas | |
| JP3067922B2 (en) | Soil detection sensor | |
| US6784012B2 (en) | Method for measuring temperature in a wide range using a tunnel junction | |
| JPS6227956A (en) | Method for measuring skin impedance | |
| JPS56153745A (en) | Method for defect evaluation on insulative thin film | |
| JPH0552789A (en) | Moisture content sensor | |
| JPH0712769A (en) | Hygrometer | |
| JP3519977B2 (en) | Estimation method of resistive film pressure sensitive digitizer circuit constant | |
| JPH0674804A (en) | Thermal flow sensor | |
| JP2946708B2 (en) | Moisture sensitive element | |
| JPH09159633A (en) | Gas sensor | |
| JPH0353168Y2 (en) |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A01 | Written decision to grant a patent or to grant a registration (utility model) |
Free format text: JAPANESE INTERMEDIATE CODE: A01 Effective date: 19990611 |
|
| LAPS | Cancellation because of no payment of annual fees |