JPH059657Y2 - - Google Patents

Info

Publication number
JPH059657Y2
JPH059657Y2 JP16351786U JP16351786U JPH059657Y2 JP H059657 Y2 JPH059657 Y2 JP H059657Y2 JP 16351786 U JP16351786 U JP 16351786U JP 16351786 U JP16351786 U JP 16351786U JP H059657 Y2 JPH059657 Y2 JP H059657Y2
Authority
JP
Japan
Prior art keywords
light
voltage
optical fiber
side optical
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.)
Expired - Lifetime
Application number
JP16351786U
Other languages
Japanese (ja)
Other versions
JPS6370084U (en
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP16351786U priority Critical patent/JPH059657Y2/ja
Publication of JPS6370084U publication Critical patent/JPS6370084U/ja
Application granted granted Critical
Publication of JPH059657Y2 publication Critical patent/JPH059657Y2/ja
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Measurement Of Current Or Voltage (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Description

【考案の詳細な説明】 A 産業上の利用分野 本考案は、電気泳動現象を利用してコロイド溶
液中を透過する光の透過量の変化を測定すること
により電圧を測定する光コロイド電圧センサに関
する。
[Detailed description of the invention] A. Industrial application field The present invention relates to an optical colloid voltage sensor that measures voltage by measuring changes in the amount of light transmitted through a colloid solution using electrophoresis. .

B 考案の概要 本考案は、コロイド溶液内に配置した一対の電
極に電圧を印加すると、コロイド溶液内のコロイ
ド粒子が一方の電極の方へ移動する現象、即ち電
気泳動を応用したものである。つまり、一方の電
極の方へ移動するコロイド粒子のコロイド溶液と
の境界面移動速度は、電極に印加される電圧に比
例して増加する。また、コロイド溶液中に光を透
過させた際に透過する光の透過量も、コロイド粒
子の移動と共に増加するので、コロイド溶液中を
透過する光の透過量は、電極に印加される電圧に
比例して増加する。
B. Overview of the Invention This invention applies the phenomenon that when a voltage is applied to a pair of electrodes placed in a colloidal solution, colloidal particles in the colloidal solution move toward one of the electrodes, i.e., electrophoresis. In other words, the speed at which colloidal particles move toward one of the electrodes at the interface with the colloidal solution increases in proportion to the voltage applied to the electrodes. In addition, the amount of light transmitted when light is transmitted through the colloidal solution also increases with the movement of the colloidal particles, so the amount of light transmitted through the colloidal solution increases in proportion to the voltage applied to the electrodes.

従つて、予め、電極に印加される電圧と、コロ
イド溶液中を透過する光の透過量との関係を測定
して記憶しておくことにより、コロイド溶液中を
透過する光の透過量から、電極に印加される電圧
(測定電圧)を求めることができる。
Therefore, by measuring and storing the relationship between the voltage applied to the electrode and the amount of light transmitted through the colloidal solution in advance, it is possible to determine the relationship between the electrode and the amount of light transmitted through the colloidal solution. The voltage applied to (measured voltage) can be determined.

C 従来の技術 従来より電圧測定を行う測定器には、可動コイ
ル形等の各種タイプが用いられている。
C. Prior Art Conventionally, various types of measuring instruments, such as a moving coil type, have been used for measuring voltage.

しかしながら、従来の電圧測定器はいずれも電
磁ノイズの影響を受けやすいので、電磁ノイズが
多い環境下での電圧測定は測定値に誤差が生じる
不都合があつた。
However, all conventional voltage measuring instruments are easily affected by electromagnetic noise, so voltage measurements in environments with a lot of electromagnetic noise have the disadvantage of causing errors in measured values.

D 考案が解決しようとする問題点 本考案は上記した電磁ノイズによつて測定値に
誤差が生じる問題点を解決する目的でなされ、電
気泳動現象を利用してコロイド溶液中を透過する
光の透過量の変化を測定することにより、電磁ノ
イズの影響を受けることなく電圧を測定できる新
規の光コロイド電圧センサを提供しようとするも
のである。
D. Problems to be solved by the invention The invention was made to solve the above-mentioned problem in which errors occur in measured values due to electromagnetic noise, and uses electrophoresis to transmit light through a colloid solution. The present invention aims to provide a novel photocolloid voltage sensor that can measure voltage without being affected by electromagnetic noise by measuring changes in quantity.

E 問題点を解決するための手段 前記問題点の解決にあたつて本考案は、少なく
とも内面が電気絶縁材よりなるコロイド溶液を密
封した容器の対向する一方の面に発光部を備えた
送光側光フアイバを接続すると共に、同軸線上に
位置して対向する他方の面に受光部を備えた受光
側光フアイバを接続し、更に前記容器内に、外部
から電圧が印加される一対の電極を、前記送光側
光フアイバと受光側光フアイバ間を通る前記発光
部からの光の進行方に対して直交方向に対設した
ことを特徴とする。
E. Means for Solving the Problems In order to solve the above-mentioned problems, the present invention provides a light emitting device which is equipped with a light emitting section on one opposing surface of a sealed container containing a colloidal solution whose inner surface is made of an electrically insulating material. In addition to connecting the side optical fibers, a light-receiving side optical fiber located on the coaxial line and having a light-receiving portion on the other surface facing each other is connected, and a pair of electrodes to which a voltage is applied from the outside is provided in the container. , characterized in that the optical fibers are disposed opposite to each other in a direction perpendicular to the direction in which light from the light emitting section travels between the light transmitting side optical fiber and the light receiving side optical fiber.

F 実施例 以下、本考案を図示の実施例により詳細に説明
する。
F. Embodiments Hereinafter, the present invention will be explained in detail with reference to illustrated embodiments.

第1図aは本考案に係る光コロイド電圧センサ
の第1実施例を示す断面図、第1図bは同光コロ
イド電圧センサの斜視図である。同図に示すよう
に、内面が電気絶縁材1aよりなるパイプ状の容
器1内には、粒径の整つた粒子を等方的に分散さ
せたコロイド溶液2が密封されている。このコロ
イド溶液2としては、シリカ砥粒(SiO2)等の
表面に電気二重層を形成しやすい粒径の整つた微
粒子を、等方的に分散させた溶液が用いられる。
また、容器1内の対向する上下の面には、長手方
向に沿つて一対の電極3a,3bが対設されてい
る。更に、この一対の電極3a,3bに対して直
角方向において、容器1の一方の端には断面円形
状の送光側光フアイバ4を挿入して接続し、他方
の端面には断面円形状の送光側光フアイバ4と同
径の受光側光フアイバ5を、送光側光フアイバ4
に対して同軸線上に位置するように挿入して接続
されている。そして、送光側光フアイバ4の先端
には、レーザー発信器やLED等の発光素子を有
する発光部6が備えられ、受光側光フアイバ5の
先端には、発光部6からの光を受光するフオトダ
イオードやフオトトランジスタ等の受光素子を有
する受光部7が備えられている。尚、8は電極3
aに接続された端子(正端子)であり、9は電極
3bに接続された端子(負端子)である。図では
端子9はアース端子である。
Fig. 1a is a cross-sectional view showing a first embodiment of the optical colloid voltage sensor according to the present invention, and Fig. 1b is a perspective view of the same optical colloid voltage sensor. As shown in the figure, a colloid solution 2 in which particles of uniform size are isotropically dispersed is sealed in a pipe-shaped container 1 whose inner surface is made of an electrical insulating material 1a. As the colloid solution 2, a solution in which fine particles of uniform size that easily form an electric double layer on the surface, such as silica abrasive grains ( SiO2 ), are isotropically dispersed is used.
A pair of electrodes 3a, 3b are provided along the longitudinal direction on the opposing upper and lower surfaces inside the container 1. Furthermore, a light-transmitting optical fiber 4 having a circular cross section is inserted and connected to one end of the container 1 in a direction perpendicular to the pair of electrodes 3a, 3b, and a light-receiving optical fiber 5 having the same diameter as the light-transmitting optical fiber 4 having a circular cross section is inserted and connected to the other end.
The light-transmitting optical fiber 4 is inserted and connected to the electrode 3 so that it is positioned on the same axis. The tip of the light-transmitting optical fiber 4 is provided with a light-emitting unit 6 having a light-emitting element such as a laser transmitter or an LED, and the tip of the light-receiving optical fiber 5 is provided with a light-receiving unit 7 having a light-receiving element such as a photodiode or a phototransistor for receiving light from the light-emitting unit 6.
In the figure, terminal 9 is a ground terminal.

次に、上記のように構成された本考案の光コロ
イド電圧センサの動作について説明する。まず、
電極3a,3b間に電圧を印加する前は第2図a
に示すように、容器1内のコロイド溶液2中のコ
ロイド粒子2aは均一に懸濁(分散)した状態と
なつているので、光の透過性が良くない。次に、
第2図bに示すように、測定しようとする電圧
(正電圧)V0を端子(正端子)8を介して電極3
aに印加すると、前述した電気泳動現象により、
コロイド溶液2中のコロイド粒子2aは電極3a
の方向へ移動する。すると、コロイド溶液2中に
境界面2bが形成されてコロイド粒子2aを含ん
だ不透明の上部境界層2cと、コロイド粒子2a
を含まない透明の下部境界層2dとに分離され、
時間の経過とともに境界面2bは電極3a方向に
移動する(第1図a参照)。つまり、コロイド粒
子2aを含まない透明な下部境界層2dの領域は
時間の経過に比例して増大し、光を透過しやすく
なる。このため、発光部6より出射された光A
は、送光側光フアイバ4中を伝播して容器1内の
下部境界層2d中を透過し、受光側光フアイバ5
中を伝播して受光部7に導入される。この際、受
光部7に導入される光A′は時間に比例して増加
し、受光部7からの出力電圧V1も増加する。こ
のことにより、第3図に示すように、コロイド溶
液2中の下部境界層2dの移動と共に移動する境
界面2bの移動速度vは、電極3aに印加される
測定電圧V0に比例する。また、コロイド溶液2
中のコロイド粒子2aの径が大きいほど境界面2
cの移動速度vは速くなる。
Next, the operation of the photocolloid voltage sensor of the present invention configured as described above will be explained. first,
Figure 2a before applying voltage between electrodes 3a and 3b
As shown in FIG. 2, the colloidal particles 2a in the colloidal solution 2 in the container 1 are in a uniformly suspended (dispersed) state, so that the light transmittance is not good. next,
As shown in Figure 2b, the voltage to be measured (positive voltage) V 0 is applied to the electrode 3 through the terminal (positive terminal) 8.
When applied to a, due to the electrophoretic phenomenon described above,
Colloidal particles 2a in colloidal solution 2 are electrodes 3a
Move in the direction of. Then, a boundary surface 2b is formed in the colloidal solution 2, and an opaque upper boundary layer 2c containing the colloidal particles 2a and the colloidal particles 2a are formed.
and a transparent lower boundary layer 2d that does not contain
As time passes, the boundary surface 2b moves toward the electrode 3a (see FIG. 1a). In other words, the area of the transparent lower boundary layer 2d that does not contain the colloidal particles 2a increases in proportion to the passage of time, and becomes easier to transmit light. Therefore, the light A emitted from the light emitting section 6
propagates through the light transmitting side optical fiber 4, passes through the lower boundary layer 2d in the container 1, and passes through the light receiving side optical fiber 5.
The light propagates inside and is introduced into the light receiving section 7. At this time, the light A' introduced into the light receiving section 7 increases in proportion to time, and the output voltage V1 from the light receiving section 7 also increases. As a result, as shown in FIG. 3, the moving speed v of the boundary surface 2b that moves with the movement of the lower boundary layer 2d in the colloidal solution 2 is proportional to the measurement voltage V 0 applied to the electrode 3a. In addition, colloid solution 2
The larger the diameter of the colloidal particles 2a inside, the more the boundary surface 2
The moving speed v of c becomes faster.

以上、前記したように、予め電極3aに印加さ
れる測定電圧V0と、コロイド溶液2中を透過す
る発光部6から出射される光Aの透過量(出力電
圧V1)との関係を測定して記憶しておくことに
より、測定時におけるコロイド溶液2中を透過す
る光A′の透過量(出力電圧V1)から電極3aに
印加される測定電圧V0を求めることができる。
また、受光素子7から出力される出力電圧V1
コンピユータ(不図示)に入力し、単位時間で分
割してサンプリングすることにより、高精度の測
定を行うことができる。そして、送光側光フアイ
バ4及び受光側光フアイバ5は、適当な長さに形
成して発光部6及び受光部7を電界の影響のない
場所に設置する。
As described above, the relationship between the measurement voltage V 0 applied to the electrode 3a in advance and the amount of transmitted light A emitted from the light emitting part 6 that passes through the colloidal solution 2 (output voltage V 1 ) is measured. By storing this value, the measurement voltage V 0 applied to the electrode 3a can be determined from the amount of light A' transmitted through the colloidal solution 2 (output voltage V 1 ) at the time of measurement.
Further, by inputting the output voltage V 1 output from the light receiving element 7 into a computer (not shown) and dividing and sampling it in unit time, highly accurate measurement can be performed. The light-transmitting optical fiber 4 and the light-receiving optical fiber 5 are formed to have appropriate lengths, and the light-emitting section 6 and the light-receiving section 7 are installed in a place where they are not affected by electric fields.

尚、電極3bに設けた端子(負端子)9はアー
ス端子に限られるものではなく、端子(正端子)
8に対する負極側の端子である。更に、前記実施
例とは逆に端子8を負端子、端子9を正端子とし
た場合は、コロイド粒子2aの移動方向が前記実
施例とは逆方向になり、負電圧を測定することが
てきる。
Note that the terminal (negative terminal) 9 provided on the electrode 3b is not limited to the earth terminal, but can also be used as a terminal (positive terminal).
This is the terminal on the negative side with respect to 8. Furthermore, if the terminal 8 is set as a negative terminal and the terminal 9 is set as a positive terminal, contrary to the above embodiment, the direction of movement of the colloidal particles 2a becomes opposite to that of the above embodiment, and a negative voltage can be measured. Ru.

また、容器1、送光側光フアイバ4、受光側光
フアイバ5は、断面円形状に限られるものでな
く、断面形状がだ円形状や角形状でも良い。
Further, the container 1, the light transmitting side optical fiber 4, and the light receiving side optical fiber 5 are not limited to circular cross sections, but may have elliptical or angular cross sections.

更に、第3図に示したように、コロイド粒子2
aの粒子径の大きさによつて、測定電圧V0と境
界面移動速度vとの関係が異なるので、適当なコ
ロイド粒子2aの径を選択することにより、測定
する電圧のレベルに応じたセンサを得ることがで
きる。
Furthermore, as shown in FIG. 3, colloid particles 2
Since the relationship between the measurement voltage V 0 and the boundary surface movement speed v differs depending on the particle size of a, by selecting an appropriate diameter of the colloidal particles 2a, the sensor can be adjusted according to the voltage level to be measured. can be obtained.

第4図aは本考案の第2実施例を示す断面図、
第4図bはそのB−B線断面図である。尚、第1
図a,bで示した第1実施例と同一部分には、同
一符号を付してその説明は省略する。
FIG. 4a is a sectional view showing a second embodiment of the present invention;
FIG. 4b is a sectional view taken along the line B--B. Furthermore, the first
Components that are the same as those in the first embodiment shown in FIGS.

この実施例においては、断面円形状の送光側光
フアイバ13及び受光側光フアイバ14は、コロ
イド粒子2aを含まない透明な下部境界層2dの
領域に相当する位置に対向して設けられている。
そして、前記実施例と同様にして測定電圧V0
測定することができる。
In this embodiment, the light transmitting side optical fiber 13 and the light receiving side optical fiber 14 having a circular cross section are provided facing each other at a position corresponding to a region of the transparent lower boundary layer 2d that does not contain colloidal particles 2a. .
Then, the measurement voltage V 0 can be measured in the same manner as in the above embodiment.

また、容器1と送光側光フアイバ13との接合
面1bにレンズ系(不図示)を配置することによ
り、コロイド溶液2中を透過する発光部6からの
光の指向性を高めることができる。
Furthermore, by arranging a lens system (not shown) on the joint surface 1b between the container 1 and the light-transmitting optical fiber 13, the directivity of the light from the light emitting part 6 that passes through the colloidal solution 2 can be increased. .

更に、第4図cに示すように、複数の小径の光
フアイバ束を用いて、電極3aに電圧を印加した
際に形成される下部境界層2dの断面形状に対応
した送光側光フアイバ束(不図示)及び受光側光
フアイバ束14′を容器1に接続しても良い。こ
れによつて、コロイド溶液2中を透過する発光部
6から出射される光の光量の増加を図ることがで
きる。
Furthermore, as shown in FIG. 4c, a plurality of small-diameter optical fiber bundles are used to form a light-transmitting side optical fiber bundle corresponding to the cross-sectional shape of the lower boundary layer 2d formed when voltage is applied to the electrode 3a. (not shown) and the receiving side optical fiber bundle 14' may be connected to the container 1. This makes it possible to increase the amount of light emitted from the light emitting section 6 that passes through the colloidal solution 2.

第5図aは本考案の第3実施例を示す断面図、
第5図bはそのC−C線断面図である。尚、第1
図a,bで示した第1実施例と同一部分には、同
一符号を付してその説明は省略する。
FIG. 5a is a sectional view showing a third embodiment of the present invention;
FIG. 5b is a sectional view taken along the line CC. Furthermore, the first
Components that are the same as those in the first embodiment shown in FIGS.

この実施例においては、容器1′を断面四角状
に形成し、この容器1′を挟んでコロイド溶液2
の上部境界層2c及び下部境界層2dにそれぞれ
2本づつの送光側光フアイバ15a,15b,1
5c,15d及び受光側光フアイバ16a,16
b,16c,16dが対向するようにして配設す
る。各送光側光フアイバ15a〜15dにはそれ
ぞれ発光部6が接続され、各受光側光フアイバ1
6a〜16dにはそれぞれ受光部7が接続されて
いる。そして、前記実施例と同様にして測定電圧
V0を測定することができる。この際、上部境界
層2cにおける各受光部7での出力電圧V11と、
下部境界層2dにおける各受光部7での出力電圧
V12との平均値を求めることにより更に精度良く
測定電圧V0を測定することができる。
In this embodiment, the container 1' is formed to have a square cross section, and the colloidal solution 2 is placed between the containers 1'.
Two light transmission side optical fibers 15a, 15b, 1 are provided in the upper boundary layer 2c and the lower boundary layer 2d of the
5c, 15d and receiving side optical fibers 16a, 16
b, 16c, and 16d are arranged so as to face each other. A light emitting section 6 is connected to each light transmitting side optical fiber 15a to 15d, and each light receiving side optical fiber 1
A light receiving section 7 is connected to each of 6a to 16d. Then, the measured voltage is
V 0 can be measured. At this time, the output voltage V 11 at each light receiving section 7 in the upper boundary layer 2c,
Output voltage at each light receiving section 7 in the lower boundary layer 2d
By finding the average value with V 12 , the measurement voltage V 0 can be measured with higher accuracy.

尚、この実施例に限らず、上部境界層2c及び
下部境界層2dに、それぞれ1本づつ又は3本以
上の送光側光フアイバ及び受光側光フアイバを配
設してそれに対応した発光部及び受光部をそれぞ
れ設ける構成でも良い。
Incidentally, the present invention is not limited to this embodiment, and the upper boundary layer 2c and the lower boundary layer 2d may be provided with one or more light-transmitting side optical fibers and three or more light-receiving side optical fibers, respectively, and corresponding light-emitting parts and A configuration in which a light receiving section is provided respectively may be used.

G 考案の効果 以上実施例とともに具体的に説明したように本
考案によれば、電気泳動現象を利用してコロイド
溶液中を透過する光の透過量の変化を測定するこ
とによつて測定電圧を求める構成により、電磁ノ
イズ等の影響を受けることなく高精度の測定がで
きる。
G. Effects of the invention As explained above in detail with the examples, according to the invention, the measurement voltage can be determined by measuring the change in the amount of light transmitted through the colloidal solution using the electrophoresis phenomenon. The desired configuration allows highly accurate measurements without being affected by electromagnetic noise.

また、構造が簡単なのでコストの低減及び小
型・軽量化を図ることができる。
Furthermore, since the structure is simple, it is possible to reduce costs, size, and weight.

更に、コロイド粒子の種類を選ぶことにより、
測定電圧を正電圧用又は負電圧用に容易に切替え
ることができる。
Furthermore, by selecting the type of colloid particles,
Measurement voltage can be easily switched to positive voltage or negative voltage.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図aは本考案に係る光コロイド電圧センサ
の第1実施例を示す断面図、第1図bは同光コロ
イド電圧センサの斜視図、第2図aは電極に電圧
を印加する前の状態を示す第1図aのA−A線断
面図、第2図bは電極に電圧を印加した後の状態
を示す第1図aのA−A線断面図、第3図は測定
電圧と境界面移動速度との関係を示す図、第4図
aは本考案の第2実施例を示す断面図、第4図b
は第4図aのB−B線断面図、第4図cは第2実
施例に係る他の実施例を示す断面図、第5図aは
本考案の第3実施例を示す断面図、第5図bは第
5図aのC−C線断面図である。 図面中、1は容器、1aは電気絶縁材、2はコ
ロイド溶液、2aはコロイド粒子、2bは境界
面、2cは上部境界層、2dは下部境界層、3
a,3bは電極、4は送光側光フアイバ、5は受
光側光フアイバ、6は送光部、7は受光部、8,
9は端子である。
FIG. 1a is a sectional view showing the first embodiment of the photocolloid voltage sensor according to the present invention, FIG. 1b is a perspective view of the same photocolloid voltage sensor, and FIG. Figure 1a is a cross-sectional view taken along the line A-A in Figure 1a showing the state, Figure 2b is a cross-sectional view taken along the line A-A in Figure 1a showing the state after voltage is applied to the electrode, and Figure 3 is the measured voltage and Figure 4a is a cross-sectional view showing the second embodiment of the present invention, Figure 4b is a diagram showing the relationship with the moving speed of the boundary surface.
is a sectional view taken along the line B-B in FIG. 4a, FIG. 4c is a sectional view showing another embodiment of the second embodiment, and FIG. 5a is a sectional view showing a third embodiment of the present invention. FIG. 5b is a sectional view taken along the line CC in FIG. 5a. In the drawing, 1 is a container, 1a is an electrical insulating material, 2 is a colloidal solution, 2a is a colloidal particle, 2b is a boundary surface, 2c is an upper boundary layer, 2d is a lower boundary layer, 3
a, 3b are electrodes, 4 is a transmitting side optical fiber, 5 is a light receiving side optical fiber, 6 is a light transmitting section, 7 is a light receiving section, 8,
9 is a terminal.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 少なくとも内面が電気絶縁材よりなるコロイド
溶液を密封した容器の対向する一方の面に発光部
を備えた送光側光フアイバを接続すると共に、同
軸線上に位置して対向する他方の面に受光部を備
えた受光側光フアイバを接続し、更に前記容器内
に、外部から電圧が印加される一対の電極を、前
記送光側光フアイバと受光側光フアイバ間を通る
前記発光部からの光の進行方向に対して直交方向
に対設したことを特徴とする光コロイド電圧セン
サ。
A light transmitting side optical fiber with a light emitting part is connected to one opposing surface of a container sealed with a colloidal solution whose at least the inner surface is made of an electrically insulating material, and a light receiving part is located on the same axis and is located on the other opposing surface. A pair of electrodes to which a voltage is applied from the outside is connected in the container, and a pair of electrodes to which a voltage is applied from the outside is connected to the light receiving side optical fiber provided with the light emitting section. A photocolloid voltage sensor characterized in that it is installed oppositely in a direction perpendicular to the direction of travel.
JP16351786U 1986-10-27 1986-10-27 Expired - Lifetime JPH059657Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16351786U JPH059657Y2 (en) 1986-10-27 1986-10-27

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16351786U JPH059657Y2 (en) 1986-10-27 1986-10-27

Publications (2)

Publication Number Publication Date
JPS6370084U JPS6370084U (en) 1988-05-11
JPH059657Y2 true JPH059657Y2 (en) 1993-03-10

Family

ID=31091786

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16351786U Expired - Lifetime JPH059657Y2 (en) 1986-10-27 1986-10-27

Country Status (1)

Country Link
JP (1) JPH059657Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7643861B2 (en) 2020-10-30 2025-03-11 株式会社荏原製作所 Method, device, and program for determining timing for removing a substrate from a cassette in a substrate processing apparatus, and substrate processing apparatus

Also Published As

Publication number Publication date
JPS6370084U (en) 1988-05-11

Similar Documents

Publication Publication Date Title
AU675082B2 (en) Optical displacement sensor
US3224279A (en) Accelerometer
US3464276A (en) Inclinometer or accelerometer
EP0027099A1 (en) Refractive-index responsive light-signal system
CN107941335A (en) Sensor fibre and fibre-optical sensing device
JPH059657Y2 (en)
CN112284565A (en) An anti-resonant fiber optic temperature detector
CN218180148U (en) A temperature sensor based on micro-nano optical fiber
JPH0668511B2 (en) Insulator for voltage detection
JPH0571914B2 (en)
RU79994U1 (en) ABSOLUTE TILT FIBER OPTICAL MEASURING TRANSMITTER
CN112269034B (en) Acceleration sensors and electronic devices
SU939935A2 (en) Device for measuring displacements
SU618627A1 (en) Displacement-measuring photoelectric device
JPS6365329A (en) Waveguide type temperature sensor
JPS63311147A (en) Optical fiber type humidity sensor
SU690283A1 (en) Capacitive transducer for measuring wire diameter
JPH0310189A (en) Charged particle beam shape measurement method
CN116839544A (en) Optical fiber sensing type nanoscale level meter
JPS62274235A (en) Measuring instrument for far visual field image of light emitting element
JPH0443810Y2 (en)
JPH01250039A (en) Measuring instrument for liquid refractive index
JPS63241427A (en) Optical liquid level sensor
JPS629255A (en) Measuring method for humidity and humidity sensor used for measuring method
JPS63311307A (en) Optical fiber type temperature sensor