JPS5814031A - Sensor for amount of steam - Google Patents
Sensor for amount of steamInfo
- Publication number
- JPS5814031A JPS5814031A JP11263081A JP11263081A JPS5814031A JP S5814031 A JPS5814031 A JP S5814031A JP 11263081 A JP11263081 A JP 11263081A JP 11263081 A JP11263081 A JP 11263081A JP S5814031 A JPS5814031 A JP S5814031A
- Authority
- JP
- Japan
- Prior art keywords
- water vapor
- amount sensor
- sensor
- vapor amount
- gold electrodes
- 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
- 239000013078 crystal Substances 0.000 claims abstract description 18
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 claims abstract description 15
- 239000010931 gold Substances 0.000 claims abstract description 15
- 229910052737 gold Inorganic materials 0.000 claims abstract description 15
- 238000005260 corrosion Methods 0.000 claims abstract description 5
- 230000007797 corrosion Effects 0.000 claims abstract description 5
- 229910052751 metal Inorganic materials 0.000 claims abstract description 4
- 239000002184 metal Substances 0.000 claims abstract description 4
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 33
- 239000000919 ceramic Substances 0.000 claims description 2
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 claims description 2
- 239000011521 glass Substances 0.000 abstract description 2
- 229910052703 rhodium Inorganic materials 0.000 abstract description 2
- 239000010948 rhodium Substances 0.000 abstract description 2
- MHOVAHRLVXNVSD-UHFFFAOYSA-N rhodium atom Chemical compound [Rh] MHOVAHRLVXNVSD-UHFFFAOYSA-N 0.000 abstract description 2
- 229910001220 stainless steel Inorganic materials 0.000 abstract description 2
- 239000010935 stainless steel Substances 0.000 abstract description 2
- 230000004044 response Effects 0.000 description 11
- 238000005259 measurement Methods 0.000 description 10
- 239000007789 gas Substances 0.000 description 8
- 239000011347 resin Substances 0.000 description 5
- 229920005989 resin Polymers 0.000 description 5
- 230000004043 responsiveness Effects 0.000 description 5
- 238000002474 experimental method Methods 0.000 description 4
- 239000010409 thin film Substances 0.000 description 4
- 239000000428 dust Substances 0.000 description 3
- 239000000126 substance Substances 0.000 description 3
- 230000007704 transition Effects 0.000 description 3
- KWGKDLIKAYFUFQ-UHFFFAOYSA-M lithium chloride Chemical compound [Li+].[Cl-] KWGKDLIKAYFUFQ-UHFFFAOYSA-M 0.000 description 2
- 238000012423 maintenance Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000004088 simulation Methods 0.000 description 2
- 239000000243 solution Substances 0.000 description 2
- 238000001179 sorption measurement Methods 0.000 description 2
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 230000001934 delay Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000003487 electrochemical reaction Methods 0.000 description 1
- 239000003792 electrolyte Substances 0.000 description 1
- 239000011888 foil Substances 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000012528 membrane Substances 0.000 description 1
- 229910044991 metal oxide Inorganic materials 0.000 description 1
- 150000004706 metal oxides Chemical class 0.000 description 1
- TWNQGVIAIRXVLR-UHFFFAOYSA-N oxo(oxoalumanyloxy)alumane Chemical compound O=[Al]O[Al]=O TWNQGVIAIRXVLR-UHFFFAOYSA-N 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 150000003839 salts Chemical class 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N5/00—Analysing materials by weighing, e.g. weighing small particles separated from a gas or liquid
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- General Physics & Mathematics (AREA)
- Immunology (AREA)
- Pathology (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は、応答性、再現性に優れ、特に湿度の連続的制
御を目的とする計測にも適した気体中の水蒸気量のセン
サーに関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a sensor for measuring the amount of water vapor in a gas that has excellent responsiveness and reproducibility and is particularly suitable for measurements aimed at continuous control of humidity.
従来より空気中の水蒸気量を測定する手段として種々の
ものが用いられてきたが、何れも応答性。Various methods have been used to measure the amount of water vapor in the air, but all of them are responsive.
再現性、信頼性、保守の容易性及び経時変化等の緒特性
の全てについて満足できるものがなかった。None of them were satisfactory in terms of all characteristics such as reproducibility, reliability, ease of maintenance, and changes over time.
例えば、従来の乾湿球温度計は保守が十分になされてい
れば性能の経時変化は少なく比較的容易に正確に湿度の
測定を行ない得るが、この湿度計は被測定気体に大きな
影響を与えるために、狭い空間内の湿度測定には適さな
い。またこれは応答も遅く、小形化も容易にはできず、
指示値を電気信号に変換することも容易にはできない必
・ら、湿度の制御を目的とする計測には全く不向きであ
る。For example, if a conventional wet and dry bulb thermometer is well maintained, there is little change in performance over time and it is possible to measure humidity relatively easily and accurately. Therefore, it is not suitable for measuring humidity in a small space. In addition, it has a slow response and cannot be easily miniaturized.
Since the indicated value cannot be easily converted into an electrical signal, it is completely unsuitable for measurement aimed at controlling humidity.
この点最近の金属酸化物(酸化アルミニウム等)または
電解質(塩化リチウム等)等を用いた静電容量式または
電気抵抗式湿度センサーは小形軽量で取扱いも容易であ
り、かつ測定値が電気信号として得られるさころから開
発に力が注がれている。In this regard, recent capacitive or electrical resistance humidity sensors that use metal oxides (aluminum oxide, etc.) or electrolytes (lithium chloride, etc.) are small, lightweight, and easy to handle, and the measured values are converted into electrical signals. Efforts are being put into development from the souls that can be obtained.
しかしながら、これらのセンサーは抵抗体の吸着現象に
よって再現性が不十分であり、経時変化も大きいため、
信頼性の面で実用化の域に達していない。さらに最近に
なって、厚みすべり振動する圧電共振子(水晶振動子)
の少なくとも一方の表面に吸湿性物質の薄膜を形成し、
湿度変化に伴うこの圧電共振子の共振周波数の変化から
湿度を検出する湿度センサーも公表されている(特開昭
52−55580号公報)。しかしながらこの湿度セン
サーは、これより以前のセンサーに比較すれば応答連関
かやや速いが、しかし、内燃機関の特性改善のために機
関の吸入気中の水蒸気量を計測して連続的に制御しよう
とする場合のように極めて速い応答性が要求される場合
に適用するには、前記公開公報に開示された程度の応答
特性では列置不十分である。また互換性のある製品を得
ることが実際には困難である。However, these sensors have insufficient reproducibility due to the adsorption phenomenon of the resistor and also have large changes over time.
In terms of reliability, it has not reached the level of practical use. More recently, piezoelectric resonators (crystal resonators) that vibrate through thickness shear
forming a thin film of a hygroscopic substance on at least one surface of the
A humidity sensor that detects humidity from a change in the resonant frequency of the piezoelectric resonator due to a change in humidity has also been published (Japanese Patent Application Laid-Open No. 52-55580). However, this humidity sensor has a slightly faster response than previous sensors, but attempts to measure and continuously control the amount of water vapor in the engine's intake air in order to improve the characteristics of the internal combustion engine. The response characteristics disclosed in the above-mentioned publication are insufficient for application to cases where extremely fast response is required, such as in cases where extremely fast response is required. Also, it is difficult in practice to obtain compatible products.
本発明はこれらの点に鑑みなされたものであり、応答性
及び再現性に優れ特に速やかな応答性が要求される湿度
の連続的制御を目的とする計測にも適した水蒸気量セン
サーを提供しようとするものである。本発明者は上述の
目的を満足する水蒸気量センサーを得べく種々実験を行
なった。従来は湿度センサーには吸湿物質を塗着又は貼
付せねばならないと考えられていたが、種々実験の結果
当該分野における技術者にとって従来全く予想し得なか
った意外な実験データが得られた。本発明はこの実験デ
ータに基づいて完成に導かれ、所期の(目的を達成した
ものである。以下図面を用いて本発明の実施例について
詳述することにより本発明を明らかにする。The present invention has been made in view of these points, and it is an object of the present invention to provide a water vapor amount sensor that has excellent responsiveness and reproducibility and is suitable for measurements aimed at continuous control of humidity, which particularly requires quick responsiveness. That is. The present inventor conducted various experiments in order to obtain a water vapor amount sensor that satisfies the above-mentioned objectives. Conventionally, it was thought that a moisture-absorbing substance must be applied or pasted to a humidity sensor, but as a result of various experiments, unexpected experimental data that could not have been predicted by engineers in the field was obtained. The present invention was completed on the basis of this experimental data and has achieved its intended purpose.The present invention will be clarified by describing embodiments of the present invention in detail below with reference to the drawings.
第1図は本発明の一実施例としての水蒸気量センサーの
正面図、第2図は第1図の水蒸気量センサーの平面図で
ある。第1図及び第2図において対応部にはそれぞれ同
一符号を付しである。図において1は圧電気現象を生じ
る圧電体としての水晶片であり、該水晶片lの表面及び
裏面の中央部には、それぞれこの圧電体としての水晶片
1に振動電圧を印加するための箔状の金電極2.2/が
対向する対をなして配され、これら金電極2,2′の前
記水晶片1に接していない側の面はそれぞれ直接外気に
接触するように露出されている。従って前記水晶片1及
び一対の金電極2,2′は公知の水晶振動子における水
晶片及び電極と同様の形状をなしている。前記金電極2
,2′からはそれぞれ耐蝕性金属(例えばステンレス鋼
、ロジウム等)製のリード線8.8′が導出され、これ
らのリード線8.8′は絶縁ガラス等よりなるベース4
によりそれらの相対位置が固定されている。なお前記各
リード線8,8′は、各対応する金電極2,2′に接触
する部分が小径のコイルスプリング状となされ、それぞ
れ金電極2,2′とともに水晶片1を挾んで支持するよ
うになされている。FIG. 1 is a front view of a water vapor amount sensor as an embodiment of the present invention, and FIG. 2 is a plan view of the water vapor amount sensor of FIG. 1. Corresponding parts in FIG. 1 and FIG. 2 are given the same reference numerals. In the figure, reference numeral 1 denotes a crystal piece as a piezoelectric body that generates a piezoelectric phenomenon, and foils for applying an oscillating voltage to the crystal piece 1 as a piezoelectric body are respectively placed at the center of the front and back surfaces of the crystal piece l. Gold electrodes 2 and 2/ are arranged in opposing pairs, and the surfaces of these gold electrodes 2 and 2' that are not in contact with the crystal piece 1 are exposed so as to be in direct contact with the outside air. . Therefore, the crystal blank 1 and the pair of gold electrodes 2, 2' have the same shape as the crystal blank and electrodes in a known crystal resonator. The gold electrode 2
, 2' lead out lead wires 8.8' made of a corrosion-resistant metal (for example, stainless steel, rhodium, etc.), and these lead wires 8.8' are connected to the base 4 made of insulating glass or the like.
Their relative positions are fixed by Each of the lead wires 8, 8' has a coil spring shape with a small diameter at the part that contacts the corresponding gold electrode 2, 2', and is designed to sandwich and support the crystal piece 1 together with the gold electrode 2, 2'. is being done.
上述のような構成の本発明の水蒸気量センサーは以下の
ように作用する。発明者は本発明の水蒸気量センサーを
被測定気体中に置き、外部から前記リード線8,8/を
通して振動電圧を与え、そのときの水蒸気量センサーの
共振周波数を測定する実験を行った。この実験の結果、
被測定気体中の水蒸気量の変化と水蒸気量センサーの共
振周波数の遷移値との間には応答性及び再現性の極めて
よい一定の対応関係が存在することが明らかとなった。The water vapor amount sensor of the present invention configured as described above operates as follows. The inventor placed the water vapor amount sensor of the present invention in a gas to be measured, applied an oscillating voltage from the outside through the lead wires 8, 8/, and conducted an experiment in which the resonance frequency of the water vapor amount sensor at that time was measured. As a result of this experiment,
It has become clear that there is a certain correspondence relationship with extremely good response and reproducibility between the change in the amount of water vapor in the gas to be measured and the transition value of the resonance frequency of the water vapor amount sensor.
このように応答性及び再現性の極めてよい一定の対応関
係があるのは、本発明のセンサーは吸湿物質を全く有し
ないために応答を遅らせる程多量の水蒸気を吸収しまた
は放出する作用がなく、共振周波数の遷移は同相である
センサーの電極及び水晶片の外表面と気相である被測定
気体との界面における吸着現象によってこの界面の水蒸
気がセンサーに影響を与えるためであると考えられる。The reason why there is such a constant relationship between responsiveness and reproducibility is that the sensor of the present invention does not contain any hygroscopic substances, so it does not absorb or release water vapor in such a large amount that it delays the response. It is thought that the transition of the resonance frequency is caused by an adsorption phenomenon at the interface between the sensor's electrode and the outer surface of the crystal piece, which are in the same phase, and the gas to be measured, which is in the gas phase, and water vapor at this interface affects the sensor.
従って本発明の水蒸気量センサーの共振周波数から被測
定気体中の水蒸気m(例えば相対湿度)を正確に知るこ
とができる。このように何等の吸湿性物質も特設されて
いないセンサーによって水蒸気量の測定が正確に行ない
得ることは、従来当該分野においては全く予想されなか
ったことであり、画期的な結果である。本発明の水蒸気
量センサーの特性を、本発明と同様の形状を有し、金電
極にかえて銀電極とした装置(水晶片としてはl Q
MHz仕様のATカットの水晶片を適用したもの)を用
いてシミュレーションを行なった結果を第8図のグラフ
に示す。第8図のグラフにおいて、縦軸は共振周波数の
遷移量−Δf (:Hz )、横軸は相対湿度〔%〕で
あり、測定点としてはJI8 に規定された湿度の定
点(塩類の飽和水溶液と共存して平衡にある気体の相対
湿度)等を選んでいる。なおこの特性は気温25℃にお
ける測定結果である。本発明の水蒸気量センサーは前述
の公開公報所載の従来のセンサーに比し格段に優れた応
答性(従来100%応答に約20秒ないし数分要し7て
いたのに対し、本発明では約0.5秒以下)及び再現性
(±1%)を有している。これは次のような理由による
ものと考えられる。すなわち、上記従来のセンサーは、
吸湿性樹脂を小さな圧電共振子上に均一な薄膜を形成す
るように(実際には製品にばらつきが生じないようにこ
のような薄膜を形成するのけ困難であるが)配している
ので、吸湿性樹脂が水蒸気を吸収し、まだは放出するの
に時間がかかるので応答が遅れ、また高湿分囲気中では
吸湿性樹脂が多量に水分を含んで粘着性をもちはじめ、
塵埃等がセンサーに付着しやすくなるので、この付着し
た塵埃等の影響で特に高湿度領域の測定時にヒステリシ
スが増大してくる。また物性上の制約から使用温度範囲
も0〜50℃程度に限定される。これに対し本発明の装
置は上述の応答遅れやヒステリシスの原因となる吸湿性
樹脂を有しないので、極めて応答が速く、高湿度高温度
領域においてもヒステリシスをほとんど生じない。また
本発明の装置は画一的に量産することが困難な吸湿性樹
脂の薄膜を有しないので、品質にばらつきのない製品が
容易に量産でき、互換性に富んでいる。Therefore, the water vapor m (for example, relative humidity) in the gas to be measured can be accurately determined from the resonance frequency of the water vapor amount sensor of the present invention. The ability to accurately measure the amount of water vapor using a sensor that does not contain any hygroscopic material was something that had never been expected in this field, and is an epoch-making result. The characteristics of the water vapor amount sensor of the present invention are as follows: A device having the same shape as the present invention, and using a silver electrode instead of a gold electrode (as a crystal piece:
The graph in FIG. 8 shows the results of a simulation using an AT-cut crystal piece with MHz specifications. In the graph of Figure 8, the vertical axis is the amount of transition of the resonant frequency -Δf (:Hz), the horizontal axis is the relative humidity [%], and the measurement point is a fixed humidity point specified by JI8 (a saturated aqueous solution of salts). relative humidity of a gas that coexists with and is in equilibrium). Note that this characteristic is a measurement result at an air temperature of 25°C. The water vapor amount sensor of the present invention has much better response than the conventional sensor described in the above-mentioned publication (conventionally, it took about 20 seconds to several minutes for 100% response7, but the present invention (approximately 0.5 seconds or less) and reproducibility (±1%). This is considered to be due to the following reasons. In other words, the conventional sensor described above is
The hygroscopic resin is placed on a small piezoelectric resonator to form a uniform thin film (although it is difficult to form such a thin film in order to prevent variations in the product). The hygroscopic resin absorbs water vapor and it takes time to release it, so the response is delayed, and in a high humidity environment, the hygroscopic resin contains a large amount of water and becomes sticky.
Since dust and the like tend to adhere to the sensor, hysteresis increases especially when measuring in high humidity areas due to the influence of the attached dust and the like. Further, due to restrictions on physical properties, the operating temperature range is also limited to approximately 0 to 50°C. On the other hand, since the device of the present invention does not have a hygroscopic resin that causes the above-mentioned response delay and hysteresis, it has an extremely fast response and hardly causes hysteresis even in a high humidity and high temperature region. Furthermore, since the apparatus of the present invention does not have a thin film of hygroscopic resin that is difficult to uniformly mass-produce, products with consistent quality can be easily mass-produced and are highly compatible.
このことは苛酷な条件下で使用されるセンサーさして極
めて重要な利点である。また一般に従来の電気式湿度セ
ンサーは高湿領域における測定では湿度が一定でも時間
の経過とともに指示値が増大する傾向を呈していた。こ
の現象はまだ十分に解析されていないが、水分を多く吸
着したセンサーにおいて電極近傍等で何等かの電気化学
的反応がひき起こされていることによるものであると推
定される。従来はこの対策としてセンサーを周囲温度よ
り高温を保つよう加熱して吸着した水分を迅速に離脱さ
せる方法(特開昭54−94090号公報)が考案され
ていたが、このような方法をとればセンサー近傍の湿度
が本来測定の対象となる湿度と差異を生じてしまう。本
発明の装置によれば上述のように高湿領域においても迅
速確実に測定ができこのような問題は全くない。また本
発明の装置は金電極と耐蝕性金属リード線を用いている
ので腐食性ガス分囲気中での連続使用も可能であり、ま
た塵埃等が付着しても洗滌することができ経年変化も極
めて少ない。また使用温度範囲も一80〜+250℃で
実用的な測定が可能である。This is a very important advantage for sensors used under harsh conditions. Furthermore, in general, conventional electric humidity sensors have a tendency for the indicated value to increase over time even when the humidity is constant when measuring in a high humidity region. Although this phenomenon has not yet been fully analyzed, it is presumed that it is caused by some kind of electrochemical reaction occurring near the electrodes in the sensor that has adsorbed a large amount of water. Conventionally, as a countermeasure to this problem, a method was devised to quickly remove the adsorbed moisture by heating the sensor to keep it higher than the ambient temperature (Japanese Patent Application Laid-open No. 54-94090). The humidity near the sensor will differ from the humidity that is originally the target of measurement. According to the apparatus of the present invention, measurements can be made quickly and reliably even in high humidity areas, as described above, and there is no such problem. Furthermore, since the device of the present invention uses gold electrodes and corrosion-resistant metal lead wires, it can be used continuously in an atmosphere surrounded by corrosive gases, and even if dust or the like adheres to it, it can be washed and will not deteriorate over time. Very few. Practical measurement is also possible within the operating temperature range of -80 to +250°C.
以上を要するに、本発明の水蒸気量センサーは、応答性
、再現性、信頼性、保守の容易性及び経時変化等の緒特
性について、湿度の連続的制御を目的とする計測に適用
するにも十分満足できる性能を有するものである。In summary, the water vapor amount sensor of the present invention has sufficient characteristics such as responsiveness, reproducibility, reliability, ease of maintenance, and changes over time to be applied to measurements aimed at continuous control of humidity. It has satisfactory performance.
また本発明の特殊な用途として、相対湿度100%以上
の領域、すなわち湯気が存在する分囲気において、その
水分量を推定するためのセンサーとして用いたり、本発
明の装置を特殊な半透膜で密閉して被測定溶液中に沈め
、その溶液中の水分量を測定するだめのセンサーとして
も応用することができる。In addition, as a special application of the present invention, the device of the present invention may be used as a sensor for estimating the moisture content in an area with a relative humidity of 100% or more, that is, in an ambient atmosphere where steam is present, and the device of the present invention may be used with a special semipermeable membrane. It can also be used as a sensor that is sealed and submerged in a solution to be measured to measure the amount of water in the solution.
なお、上述においては圧電体として水晶片を用いた場合
の実施例について説明したが、圧電体としては、水晶片
にかえて、圧電セラミック片、圧電音叉、または超音波
共振体等を適用することも可能である。これらの圧電体
の選択は価格、共振周波数等を測定の目的や表示回路部
の仕様等に合わせて勘案し、任意に行なえばよい。In addition, in the above, an example in which a crystal piece is used as the piezoelectric body has been described, but instead of the crystal piece, a piezoelectric ceramic piece, a piezoelectric tuning fork, an ultrasonic resonator, etc. can be applied as the piezoelectric body. is also possible. The selection of these piezoelectric bodies may be made arbitrarily, taking into consideration the price, resonance frequency, etc., in accordance with the purpose of measurement, the specifications of the display circuit section, etc.
第1図は本発明の水蒸気量センサーの実施例を示す正面
図、第2図は第1図の水蒸気量センサーの平面図、第8
図は本発明の水蒸気量センサーの特性をシミュレーショ
ンにより求めた結果としてのグラフである。
1・・・圧電体(水晶片)
2.2′・・・金電極
8.8′・・リード線
4・・・ベース
代理人 弁理士 東島隆治FIG. 1 is a front view showing an embodiment of the water vapor amount sensor of the present invention, FIG. 2 is a plan view of the water vapor amount sensor of FIG.
The figure is a graph showing the results obtained by simulation of the characteristics of the water vapor amount sensor of the present invention. 1...Piezoelectric body (crystal piece) 2.2'...Gold electrode 8.8'...Lead wire 4...Base agent Patent attorney Ryuji Higashijima
Claims (1)
の所定位置に一方の面が直接外気に接触するようにして
それぞれ配された箔状の金電極、及び前記各金電極から
それぞれ導出されたリード線を有する水蒸気量センサー
。 (2)前記圧電体は水晶片である特許請求の範囲第1項
記載の水蒸気量センサー。 (3)前記圧電体は圧電セラミック片である特許請求の
範囲第1項記載の水蒸気量センサー。 (41前記圧電体は圧電音叉である特許請求の範囲第1
項記載の水蒸気量センサー。 (6)前記圧電体は超音波共振体である特許請求の範囲
第1項記載の水蒸気量センサー。 (6)前記リード線は耐蝕性金属である特許請求の範囲
第1項ないし第5項記戦の水蒸気量センサー。[Scope of Claims] (A piezoelectric body, a pair of foil-shaped gold electrodes each disposed at a predetermined position so as to apply an oscillating voltage to the piezoelectric body, one surface of which is in direct contact with the outside air, and A water vapor amount sensor having lead wires respectively led out from each of the gold electrodes. (2) The water vapor amount sensor according to claim 1, wherein the piezoelectric body is a crystal piece. (3) The piezoelectric body is a piezoelectric ceramic. The water vapor amount sensor according to claim 1, which is a piezoelectric member.
Water vapor amount sensor as described in section. (6) The water vapor amount sensor according to claim 1, wherein the piezoelectric body is an ultrasonic resonator. (6) The water vapor amount sensor according to any one of claims 1 to 5, wherein the lead wire is made of a corrosion-resistant metal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11263081A JPS5814031A (en) | 1981-07-17 | 1981-07-17 | Sensor for amount of steam |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11263081A JPS5814031A (en) | 1981-07-17 | 1981-07-17 | Sensor for amount of steam |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS5814031A true JPS5814031A (en) | 1983-01-26 |
Family
ID=14591533
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11263081A Pending JPS5814031A (en) | 1981-07-17 | 1981-07-17 | Sensor for amount of steam |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5814031A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6453130A (en) * | 1987-06-02 | 1989-03-01 | Esu Deijiyoratsupu Robaato | Constant temperature operation type hygrometer |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5160584A (en) * | 1974-11-25 | 1976-05-26 | Matsushita Electric Industrial Co Ltd | Shimokenchi sochi |
-
1981
- 1981-07-17 JP JP11263081A patent/JPS5814031A/en active Pending
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5160584A (en) * | 1974-11-25 | 1976-05-26 | Matsushita Electric Industrial Co Ltd | Shimokenchi sochi |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6453130A (en) * | 1987-06-02 | 1989-03-01 | Esu Deijiyoratsupu Robaato | Constant temperature operation type hygrometer |
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