JPS61204515A - Correcting device for error of inclination sensor - Google Patents

Correcting device for error of inclination sensor

Info

Publication number
JPS61204515A
JPS61204515A JP4373885A JP4373885A JPS61204515A JP S61204515 A JPS61204515 A JP S61204515A JP 4373885 A JP4373885 A JP 4373885A JP 4373885 A JP4373885 A JP 4373885A JP S61204515 A JPS61204515 A JP S61204515A
Authority
JP
Japan
Prior art keywords
medium
liquid
refractive index
thickness
error
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.)
Granted
Application number
JP4373885A
Other languages
Japanese (ja)
Other versions
JPH0479523B2 (en
Inventor
Kikuo Shimura
志村 菊雄
Hiroaki Motohashi
本橋 浩明
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
SOTSUKISHIYA KK
Sokkisha Co Ltd
Original Assignee
SOTSUKISHIYA KK
Sokkisha Co Ltd
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 by SOTSUKISHIYA KK, Sokkisha Co Ltd filed Critical SOTSUKISHIYA KK
Priority to JP4373885A priority Critical patent/JPS61204515A/en
Publication of JPS61204515A publication Critical patent/JPS61204515A/en
Publication of JPH0479523B2 publication Critical patent/JPH0479523B2/ja
Granted legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To correct an error in measurement due to variation in the refracting index of the 1st liquid and to take an accurate measurement by providing the 2nd medium in an optical path of reflected light and setting a specific relation between its refractive index and the rate of variation in refracting index or thickness. CONSTITUTION:The 2nd medium 8 having thickness D is arranged in the optical path of the reflected light from the horizontal surface 3 of the 1st liquid 2. Then, an equation holds, where K is the ratio of variation in the refractive index between the medium 8 and liquid 2, (t) is the thickness of the air part between an image forming lens 6 and a photodetector 7, and N is the refractive index of the medium 8. Consequently, even if the liquid 2 varies in refracting index with temperature, etc., the error is corrected by the medium 8, so a slanting surface is measured accurately.

Description

【発明の詳細な説明】 (産業上の利用分野) この発明は、傾斜センサの誤差補正装置、詳しくは、液
体の水平面からの反射光の変角を利用する傾斜センサに
おける液体の屈折率の変化に伴う傾斜角検出誤差を補正
する光学機構に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) This invention relates to an error correction device for a tilt sensor, and more particularly, to an error correction device for a tilt sensor, and more particularly, to a tilt sensor that uses a change in the refractive index of a liquid in a tilt sensor that utilizes the angle of change of reflected light from a horizontal surface of the liquid. The present invention relates to an optical mechanism for correcting inclination angle detection errors caused by tilt angle detection.

(従来技術) 従来、液体が重力の作用によって常に水平面を形成する
現象を利用して、液体を容れ九容器を石する傾斜針本体
の傾きを検出する傾斜センサが実用化されている。これ
は、傾斜計本体に固定した容器内の液体の水平表面から
の反射光の進路は、この本体の傾きに応じて振れを起こ
すので、光電的にこの偏角を検出することによりて傾斜
角を求めようとするものである。この際、反射光の偏角
は容器内の液体の屈折率の変化に従って変動するから、
前述のような傾斜角測定においては、温度の変化等に起
因する液体屈折率の微少変動に伴う測定誤差を免れ得な
い。
(Prior Art) Conventionally, a tilt sensor has been put into practical use that detects the tilt of a tilted needle body that holds a liquid and holds a container by utilizing the phenomenon that a liquid always forms a horizontal surface due to the action of gravity. This is because the path of the reflected light from the horizontal surface of the liquid in the container fixed to the inclinometer body deviates depending on the inclination of the inclinometer body, so by photoelectrically detecting this declination angle, This is what we are trying to find. At this time, the polarization angle of the reflected light changes according to the change in the refractive index of the liquid in the container, so
In the above-mentioned tilt angle measurement, measurement errors due to minute fluctuations in the refractive index of the liquid due to changes in temperature cannot be avoided.

これをもう少し詳しく説明すると、第3図のような従来
の傾斜センサ方式においては、透明な容器1に容れた屈
折率nの液体2が形成する常に水平な表面3によりて実
線矢印の如く反射する光は、図示の如く傾斜計本体がθ
傾くと、容器1に対する入射光の角度は変わらないので
、破線矢印のように20偏角し、その後液体2を透過し
て空中に射出するとき屈折してδ撮れる。ただし、ここ
では便宜のために角度θの傾きが起こる前には、液体2
から出る実線矢印の光は屈折しないものとしているが、
これは必ずしも必焚のない条件である。さて、このとき
sinδ=nXsin2# の関係があるので、これを
利用し、δを検出して傾斜角θを求めるものである。し
たがって、温度の変化等によってnが変化した場合、こ
れに相当する測定誤差を生ずることになる。
To explain this in more detail, in the conventional tilt sensor system as shown in FIG. The light is emitted when the inclinometer body is θ as shown in the figure.
When the light is tilted, the angle of the incident light on the container 1 does not change, so it deflects by 20 degrees as indicated by the dashed arrow, and then when it passes through the liquid 2 and is emitted into the air, it is refracted and photographed by δ. However, for convenience's sake, before the angle θ tilts, the liquid 2
It is assumed that the light indicated by the solid arrow coming out from is not refracted,
This is a condition that does not necessarily require firing. Now, since there is a relationship of sin δ=nXsin2# at this time, this is used to detect δ and obtain the inclination angle θ. Therefore, if n changes due to a change in temperature or the like, a corresponding measurement error will occur.

(発明が解決しようとする問題点) この発明は、上述のような従来の傾斜センサにおける液
体の屈折率変化による測定誤差を補正して、測定精度を
向上するための誤差補正装置を提供することを目的とす
るものである。
(Problems to be Solved by the Invention) The present invention provides an error correction device for improving measurement accuracy by correcting measurement errors caused by changes in the refractive index of liquid in the conventional tilt sensor as described above. The purpose is to

(問題点を解決するための手段) 第1図において、第1の液体2の水平面3がらの反射光
は第1の液体2を通過した後に厚さDの第2の媒質8を
通過する。この第2の媒質8は次の関係式を満足するよ
うに設足しである。
(Means for solving the problem) In FIG. 1, the reflected light from the horizontal surface 3 of the first liquid 2 passes through the second medium 8 having a thickness D after passing through the first liquid 2. This second medium 8 is provided so as to satisfy the following relational expression.

ここで、k・第2の媒質8と第1の数体2の屈折率の変
化率の比、 t:結像レンズ6と受光検出#7の 間の空気部分の厚さ、1 = 1++11゜D:第2の
媒質8の厚さ、 N:第2の媒質8の屈折率。
Here, k is the ratio of the rate of change of the refractive index of the second medium 8 and the first numerical body 2, t is the thickness of the air portion between the imaging lens 6 and the light receiving detection #7, 1 = 1++11° D: Thickness of the second medium 8; N: Refractive index of the second medium 8.

(作用) 第1の液体2の屈折率nがdn変化して、第1の液体2
から出る反射光に誤差が導入さnても、第2の媒質を上
記の関係式を満足するように設定配置すると、この誤差
は補償されて、受光検出器7に至る反射光には何ら誤差
が導入されない。
(Function) The refractive index n of the first liquid 2 changes by dn, and the first liquid 2
Even if an error is introduced into the reflected light emitted from the detector 7, if the second medium is set and arranged so as to satisfy the above relational expression, this error will be compensated for and there will be no error at all in the reflected light that reaches the photodetector 7. is not introduced.

(実施例) 次に、第1図と第2図を参照にして、本発明の詳細な説
明する。
(Example) Next, the present invention will be described in detail with reference to FIGS. 1 and 2.

第1図に示したように、傾斜計本体(不図示)に対して
、容器1、光源4、コリメートレンズ5、結像レンズ6
、受光検出器7を図示のような配置で固定して、容器1
に容れた液体2の水平表面3から平行な反射光が得られ
るよう、表面3への入射光線側に光源4及びコリメート
レンズ5が位置するようにし、反射光側に結像レンズ6
及び受光検出器7が位置していて光源4の像が受光検出
器7上に結像するようにする。こうして、反射光の受光
検出器7上での変位を利用して傾斜角を検出する傾斜セ
ンサを構成する。
As shown in FIG. 1, a container 1, a light source 4, a collimating lens 5, and an imaging lens 6 are connected to the inclinometer main body (not shown).
, the light receiving detector 7 is fixed in the arrangement shown in the figure, and the container 1 is
In order to obtain parallel reflected light from the horizontal surface 3 of the liquid 2 contained in the liquid 2, the light source 4 and the collimating lens 5 are positioned on the side of the incident light beam to the surface 3, and the imaging lens 6 is positioned on the side of the reflected light.
and the light receiving detector 7 are positioned so that the image of the light source 4 is formed on the light receiving detector 7. In this way, a tilt sensor is constructed that detects the tilt angle by utilizing the displacement of the reflected light on the light receiving detector 7.

そして、本発明では上記の反射光が液体2を透過した後
に、厚さ一様の第2の媒IX8、例えばシリコン油を通
過するようにして、第1の液体との屈折率変化による測
定誤差を補正する。そのために、媒質8の屈折率及び屈
折率の変化率、またはその厚さを後述のように設定する
In the present invention, after the reflected light passes through the liquid 2, it passes through a second medium IX8 having a uniform thickness, such as silicone oil, to prevent measurement errors due to changes in refractive index with the first liquid. Correct. For this purpose, the refractive index and rate of change in the refractive index of the medium 8, or its thickness are set as described below.

第2図は第1図の傾斜センサの光路を模式図で示すもの
であって、第1図と第2図を用いて本発明の詳細な説明
すると次のとおりである。
FIG. 2 schematically shows the optical path of the tilt sensor shown in FIG. 1, and the present invention will be described in detail as follows using FIG. 1 and FIG. 2.

n、Nは第1の液体2、第2の媒質8の屈折率、1=1
.+1.は空気部分の厚さ、Dは第2の媒質8の厚さ、
0は傾斜計本体の傾き、すなわち検出すべき傾斜角、a
とrは図示の如く第1の液体2から出る光線の振れ角及
び第2の媒fJi!、8に入射した光線の振れ角とする
と、θ=0の場合を基準にして検出器7に得られる光源
の像の位置、すなわち反射光の変位りは次の如く表わし
得る。
n, N are the refractive indices of the first liquid 2 and the second medium 8, 1=1
.. +1. is the thickness of the air portion, D is the thickness of the second medium 8,
0 is the inclination of the inclinometer body, that is, the inclination angle to be detected, a
and r are the deflection angle of the light beam emitted from the first liquid 2 and the second medium fJi! as shown in the figure. , 8, the position of the image of the light source obtained on the detector 7, that is, the displacement of the reflected light, can be expressed as follows, based on the case where θ=0.

h=h、+h雪 −一−−−−−−−−−−−−−−−
−+1)ただし、 hI= t tanδ hl=Dtanr ここで、sinδ=nsin2θ、N sin r =
n x sin 2θの関係があるから、式(1)は次
のようになる。
h=h, +h snow −1−−−−−−−−−−−−−−−
-+1) However, hI=ttanδ hl=Dtanr, where sinδ=nsin2θ, N sinr=
Since there is a relationship n x sin 2θ, equation (1) becomes as follows.

θが微少ならば、 h−t2no(t+ −)  −−−−−−−□   
 f3)となる。故に、屈折率の変化dn、dNによる
hの変化、すなわち検出誤差dhは次のとおりとなる。
If θ is small, h−t2no(t+ −) −−−−−−−□
f3). Therefore, the change in refractive index dn and the change in h due to dN, that is, the detection error dh, are as follows.

D2 n OD dh=20(t+ )dn−−−dN−(41N   
マ よって、誤差dhを無くするにはdh=oが成立すれば
よいから、kを上記液体と媒質の屈折率の変化率の比と
したとき、式(4)から、 になるようにすればよい。すなわち、式(5)が成立す
るように、第2の媒質の屈折率N及び屈折率の変化率d
N/Nを選ぶか、又はD=NX t/(k−1)を満足
する如くその厚さDを設定すれば、前記の目的を達成し
得る。
D2 n OD dh=20(t+)dn---dN-(41N
Therefore, in order to eliminate the error dh, it is sufficient that dh=o holds, so if k is the ratio of the rate of change of the refractive index of the liquid and the medium, from equation (4), if good. That is, the refractive index N and the rate of change of the refractive index d of the second medium are set so that equation (5) holds true.
The above objective can be achieved by selecting N/N or by setting the thickness D so as to satisfy D=NX t/(k-1).

(発明の効果) この発明を利用す7Lば、以上の説明から明らかなよう
に、液体を透過しその水平な表面において反射した光線
の変角を検出することによって傾斜角を測定する場合、
簡単な光学機構を付加するだけで、温度変化等に基づい
て液体の屈折率が変動することに起因する測定誤差を補
償することができるので 8度の高い傾斜センサを提供
できる。
(Effects of the Invention) As is clear from the above explanation, when the present invention is used, when measuring the tilt angle by detecting the deflection angle of a light beam that passes through a liquid and is reflected on its horizontal surface,
By simply adding a simple optical mechanism, it is possible to compensate for measurement errors caused by fluctuations in the refractive index of the liquid based on temperature changes, etc., making it possible to provide a sensor with a high tilt angle of 8 degrees.

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

第1図は本発明による誤差補正装置を備えた傾斜センサ
の1実施例の主妄部の縦断面図、第2図は第1図の傾斜
センサの光路を示す模式図、第3図は従来方式の傾斜セ
ンサを説明する友めの概略図である。 1−容器、2−第1の液体、3−第1の液体の水平表面
、4−光源、5−コリメートレンズ、6−結像レンズ、
7−受光検出器、8−M2の媒質
FIG. 1 is a longitudinal sectional view of the main part of an embodiment of a tilt sensor equipped with an error correction device according to the present invention, FIG. 2 is a schematic diagram showing the optical path of the tilt sensor of FIG. 1, and FIG. 3 is a conventional FIG. 2 is a schematic diagram illustrating a tilt sensor of this type. 1-container, 2-first liquid, 3-horizontal surface of first liquid, 4-light source, 5-collimating lens, 6-imaging lens,
7-Photodetector, 8-M2 medium

Claims (2)

【特許請求の範囲】[Claims] (1)第1の液体の水平面からの反射光の偏角によって
傾斜角を検出する傾斜センサにおいて、該反射光が該第
1の液体を通過した後に厚さ一様の第2の媒質を通過す
る様に構成すると共に、該第1の液体の屈折率の変化に
よる検出誤差を補正するように該第2の媒質の屈折率及
び屈折率の変化率、またはその厚さを設定したことを特
徴とする傾斜センサの誤差補正装置。
(1) In a tilt sensor that detects a tilt angle based on the polarization angle of reflected light from a horizontal surface of a first liquid, the reflected light passes through a second medium having a uniform thickness after passing through the first liquid. The refractive index of the second medium, the rate of change in the refractive index, or the thickness thereof are set so as to correct a detection error due to a change in the refractive index of the first liquid. Error correction device for tilt sensor.
(2)特許請求の範囲第1項において、該第2の媒質は
次の関係式を満足するように設定したことを特徴とする
傾斜センサの誤差補正装置。 k=(t+D/N)/(D/N) ここで、k:第2の媒質と第1の液体の屈折率の変化率
の比、 t:結像レンズと受光検出器の間の 空気部分の厚さ、 D:第2の媒質の厚さ、 N:第2の媒質の屈折率。
(2) An error correction device for a tilt sensor according to claim 1, wherein the second medium is set to satisfy the following relational expression. k=(t+D/N)/(D/N) where, k: ratio of change rate of refractive index of the second medium and first liquid, t: air portion between the imaging lens and the light receiving detector thickness, D: thickness of the second medium, N: refractive index of the second medium.
JP4373885A 1985-03-07 1985-03-07 Correcting device for error of inclination sensor Granted JPS61204515A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4373885A JPS61204515A (en) 1985-03-07 1985-03-07 Correcting device for error of inclination sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4373885A JPS61204515A (en) 1985-03-07 1985-03-07 Correcting device for error of inclination sensor

Publications (2)

Publication Number Publication Date
JPS61204515A true JPS61204515A (en) 1986-09-10
JPH0479523B2 JPH0479523B2 (en) 1992-12-16

Family

ID=12672116

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4373885A Granted JPS61204515A (en) 1985-03-07 1985-03-07 Correcting device for error of inclination sensor

Country Status (1)

Country Link
JP (1) JPS61204515A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5899712A (en) * 1981-12-09 1983-06-14 Tokyo Optical Co Ltd Slant angle measuring device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5899712A (en) * 1981-12-09 1983-06-14 Tokyo Optical Co Ltd Slant angle measuring device

Also Published As

Publication number Publication date
JPH0479523B2 (en) 1992-12-16

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