JPH01136010A - Clinometer - Google Patents
ClinometerInfo
- Publication number
- JPH01136010A JPH01136010A JP62293790A JP29379087A JPH01136010A JP H01136010 A JPH01136010 A JP H01136010A JP 62293790 A JP62293790 A JP 62293790A JP 29379087 A JP29379087 A JP 29379087A JP H01136010 A JPH01136010 A JP H01136010A
- Authority
- JP
- Japan
- Prior art keywords
- angle
- inclination
- angular velocity
- measured
- pedestal
- 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
- 239000000835 fiber Substances 0.000 claims abstract description 16
- 238000005259 measurement Methods 0.000 claims description 12
- 230000003287 optical effect Effects 0.000 claims description 4
- 239000013307 optical fiber Substances 0.000 abstract description 14
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical compound C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 abstract description 7
- 238000010586 diagram Methods 0.000 description 3
- 239000007788 liquid Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Landscapes
- Navigation (AREA)
- Length Measuring Devices With Unspecified Measuring Means (AREA)
- Gyroscopes (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野]
本発明は光フアイバジャイロを用いた傾斜針に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an inclined needle using an optical fiber gyro.
従来傾斜角を測定する装置としては、振子を利用し、傾
斜角の変化に伴なって動こうとする振子の動きを位置検
出器にて検出しながら、トルカを用いて振子の位置をも
とに戻す様に構成したいわゆるサーボ加速度計型のもの
や、液体を利用し、傾斜角の変化に伴なって動く液面の
位置を静電容量等を用いて検出するもの等があった。Conventional devices for measuring the angle of inclination use a pendulum, and a position detector detects the movement of the pendulum as the angle of inclination changes, while a torquer is used to determine the position of the pendulum. There were so-called servo accelerometer-type devices configured to return the sensor to the angle of inclination, and devices that used liquid and used capacitance to detect the position of the liquid surface that moved as the inclination angle changed.
さらに、傾斜角を測定する別の手段としては、傾斜変化
の際の回転中心に、例えばロータリエンコーダの樺な回
転角度を測定するセンサを設置し、傾斜の変化を回転角
度として測定する装置もあった。Furthermore, as another means of measuring the tilt angle, there is also a device that measures the rotation angle of a rotary encoder, for example, by installing a sensor at the center of rotation when the tilt changes, and measuring the change in tilt as the rotation angle. Ta.
しかしながら、振子や液面を利用した傾斜針は、本質的
に傾斜角度の変化以外にも、振動や平行移動等の加速度
を伴なう変動に対しても感度を持ち、これらは、傾斜角
度の誤差要因となり、あるいは振動の多いところでの測
定を困難にさせる等、測定条件や測定場所を制限したり
していた。However, a pendulum or a tilting needle that uses the liquid level is inherently sensitive to not only changes in the tilt angle, but also to fluctuations that involve acceleration such as vibration and parallel movement, and these are sensitive to changes in the tilt angle. This limits the measurement conditions and measurement locations, causing errors or making measurements difficult in areas with a lot of vibration.
又、傾斜角を回転角度して測定する装置では、測定用セ
ンサが常に回転中心になければならないという制限があ
り1.精密な測定には、センサと回転中心との偏心等が
誤差要因となっていた。In addition, in a device that measures the tilt angle by rotating the angle, there is a limitation that the measurement sensor must always be at the center of rotation.1. Eccentricity between the sensor and the center of rotation has been a source of error in accurate measurements.
上記問題点の解決の為に本発明では光フアイバジャイロ
をセンサとして用い、傾斜角の変化に伴なった角速度を
光フアイバジャイロにて検出シ、さらに積分することに
よって、傾斜角を測定している。In order to solve the above problems, the present invention uses an optical fiber gyro as a sensor, detects the angular velocity accompanying the change in the tilt angle with the optical fiber gyro, and further integrates it to measure the tilt angle. .
したがって本発明においては、傾斜計の回転運動に伴な
った角速度にしか反応しないので、振動や平行移動を伴
なう場合でも、傾斜角度の変化のみを正確に測定できる
。Therefore, in the present invention, since the inclinometer reacts only to the angular velocity accompanying the rotational movement, only changes in the inclination angle can be accurately measured even when vibration or parallel movement is involved.
又、ファイバジャイロはセンサの位置が回転中心とは全
く無関係であり、傾斜する物体の任意の位置に設置でき
、偏心等に対する考慮は全く必要としない。Furthermore, the position of the fiber gyro has no relation to the center of rotation, so it can be installed at any position on a tilting object, and there is no need to take eccentricity into account.
第1図は本発明における1実施例であって、その枠体は
被測定面に接触させるための測定用平面11aを形成し
た台座11と、台座11の中央台座11より狭い幅で所
定方向に突出させた保持部3とから構成され、台座11
と支持部3内には測定用平面11aと垂直な平面内にあ
るようにファイバジャイロのセンサ用ファイバループ2
を巻回してあり、枠体内には、いわゆる位相変調式光フ
アイバジャイロ3が内蔵されている。又、本体外部には
、傾斜角度を表示するための表示器4と表示器の表示を
0とするためのリセットスイッチ5、電源をON10
F Fするための電源スィッチ6が設置しである。FIG. 1 shows one embodiment of the present invention, in which the frame body includes a pedestal 11 forming a measuring plane 11a for contacting the surface to be measured, and a frame body 11 having a width narrower than that of the central pedestal 11 of the pedestal 11. It consists of a protruding holding part 3 and a pedestal 11.
A fiber loop 2 for the sensor of the fiber gyro is disposed in the supporting part 3 in a plane perpendicular to the measuring plane 11a.
A so-called phase modulation type optical fiber gyro 3 is built into the frame. Also, on the outside of the main body, there is a display 4 for displaying the tilt angle, a reset switch 5 for setting the display to 0, and a switch 5 for turning on the power.
A power switch 6 for FF is installed.
以上の様に構成された傾斜計1を用いた傾斜角度の測定
について説明する。Measurement of the inclination angle using the inclinometer 1 configured as above will be explained.
第2図に示す様な傾斜する被測定物7上に傾斜計1の被
測定面11aを密着させる。ここで電源スィッチ6をO
Nにし、リセットスイッチ5を押すと角度表示がOとな
る。The surface 11a to be measured of the inclinometer 1 is brought into close contact with the inclined object 7 to be measured as shown in FIG. Now turn the power switch 6 to
When the setting is set to N and the reset switch 5 is pressed, the angle display becomes O.
ここで第3図に示す様に被測定物が回転(傾斜)すると
回転に伴なった角速度を位相変調式ファイバジャイロが
感知し、この角速度を積分することにより、傾斜角度が
表示器4に表示される。As shown in Fig. 3, when the object to be measured rotates (tilts), the phase modulating fiber gyro senses the angular velocity accompanying the rotation, and by integrating this angular velocity, the tilt angle is displayed on the display 4. be done.
尚、本実施例においては、光フアイバジャイロは1つし
か内蔵されておらず、第2図、第3図における紙面内で
の回転における傾斜角度しか測定できないが、光フアイ
バジャイロを2つ又は3つ、互いに直交する様に配置す
れば、2次元あるいは3次元的に傾斜角度が測定できる
事はもちろんである。−例として3次元計測のできる傾
斜計の概略図を第4図に示す、第4図において、第1図
と同符号のものは同一機能部材を示す。光フアイバジャ
イロは、ファイバループの巻回されている面内での回転
角度を測定しうるので、ファイバループ2に直交する面
内に巻回されたファイバループ12.22を設けると共
に、それぞれのファイバループ12.22による傾斜測
定のための表示器14.24リセツトスイツチ15.2
5を設けである。そして、ファイバループ2.12を保
持する様に基板11から十字状に突出した外枠は、保持
部を兼用している。In this embodiment, only one optical fiber gyro is built in, and only the inclination angle in rotation within the plane of the paper in FIGS. 2 and 3 can be measured. However, two or three optical fiber gyros are installed. Of course, if they are arranged so that they are orthogonal to each other, the inclination angle can be measured two-dimensionally or three-dimensionally. - As an example, a schematic diagram of an inclinometer capable of three-dimensional measurement is shown in FIG. 4. In FIG. 4, the same reference numerals as in FIG. 1 indicate the same functional parts. Since the optical fiber gyro can measure the rotation angle in the plane in which the fiber loop is wound, the fiber loops 12 and 22 are provided wound in the plane perpendicular to the fiber loop 2, and each fiber Indicator 14.24 Reset switch 15.2 for tilt measurement by loop 12.22
5 is provided. The outer frame projecting in a cross shape from the substrate 11 to hold the fiber loop 2.12 also serves as a holding portion.
又、ファイバジャイロも特に位相変調方式に限ることな
く、あらゆるタイプのファイバジャイロが使用できるこ
とはもちろんである。Further, the fiber gyro is not limited to the phase modulation method, and it goes without saying that any type of fiber gyro can be used.
又、いわゆるレーザジャイロも同様に使用できる。すな
わち、サンアック効果の原理に基づく光ジャイロの全て
に適用できることはいうまでもな第5図は、光フアイバ
ジャイロの特に位相変調方式の光フアイバジャイロ電気
処理系を示している。すなわち、第5図において、スー
パールミネッセントダイオード等の光源52がらの光は
、所定面内にて巻回された光フアイバループ2を経て光
検出器54に入光する。光フアイバループ2は、その一
部がピエゾ素子52に巻回され、ピエゾ素子52が発振
器53からの信号で周期的に伸縮されることで伸縮され
、光検出器55がらの信号は、いわゆる位相変調された
信号となる。光検出器54からの信号は発振器53から
の信号にょリロソクィンアンプ55でロックイン検波さ
れ、測定したい角速度に比例した信号が検出される。Also, a so-called laser gyro can be used similarly. That is, it goes without saying that the invention can be applied to all optical gyros based on the principle of the Sunack effect, and FIG. 5 shows an optical fiber gyro electrical processing system, particularly a phase modulation type optical fiber gyro. That is, in FIG. 5, light from a light source 52 such as a superluminescent diode enters a photodetector 54 through an optical fiber loop 2 wound within a predetermined plane. A part of the optical fiber loop 2 is wound around a piezo element 52, and the piezo element 52 is expanded and contracted periodically by a signal from an oscillator 53, and a signal from a photodetector 55 is transmitted with a so-called phase difference. It becomes a modulated signal. The signal from the photodetector 54 is subjected to lock-in detection by the oscillator 53 based on the signal from the oscillator 53, and a signal proportional to the angular velocity to be measured is detected.
ロッ゛クインアンプ55で検出された角速度に比例した
信号はコンピュータ56にて所定のプログラムに沿って
処理される。コンピュータ56の機能で特に重要なのは
積分機能であり、これによって角速度から回転角が求め
られる。なお、2次元、あるいは3次元の場合は、光源
5、ピエゾ素子52、発振器53を共用することで、精
度を高めながら、構成を簡単にできる。A signal proportional to the angular velocity detected by the lock-in amplifier 55 is processed by a computer 56 according to a predetermined program. A particularly important function of the computer 56 is the integral function, which determines the rotation angle from the angular velocity. Note that in the case of two-dimensional or three-dimensional, the configuration can be simplified while improving accuracy by sharing the light source 5, piezo element 52, and oscillator 53.
〔発明の効果]
以上の様に本発明によれば、傾斜角の変化に伴なう角速
度を光ジャイロを用いて測定し、それを積分することに
より傾斜角を求めているので、振動等の影響を受けずに
傾斜角を測定することができ、さらに傾斜計の設置場所
は傾斜する物体上であれば傾斜の回転中心によらずどこ
でもよ(特に制限を受けない利点がある。[Effects of the Invention] As described above, according to the present invention, the angular velocity accompanying a change in the tilt angle is measured using an optical gyro, and the tilt angle is determined by integrating the measured angular velocity, so that vibrations etc. The angle of inclination can be measured without being affected, and the inclinometer can be installed anywhere on a tilting object, regardless of the center of rotation of the tilt (it has the advantage of not being subject to any particular restrictions).
第1図は本発明による傾斜計の一実施例の斜視図、第2
図及び第3図は傾斜角測定時の動作状況を示す図、第4
図は本発明の第2実施例の斜視図、第5図は位相変調方
式の光フアイバジャイロの電気系のブロック図である。
〔主要部分の符号の説明]
1・・・傾斜計、 lla・・・測定用平面、2.1
2.22・・・ファイバループ。
第1図
第2 図 笛8図FIG. 1 is a perspective view of one embodiment of the inclinometer according to the present invention;
Figures 3 and 3 are diagrams showing operating conditions during tilt angle measurement, Figure 4
The figure is a perspective view of a second embodiment of the present invention, and FIG. 5 is a block diagram of the electrical system of a phase modulation type optical fiber gyro. [Explanation of symbols of main parts] 1... Inclinometer, lla... Measurement plane, 2.1
2.22...Fiber loop. Figure 1 Figure 2 Flute Figure 8
Claims (1)
、測定用平面に対して垂直な平面内にセンサ用ファイバ
ループを巻回した光ジャイロを内蔵し、光ジャイロから
の角速度信号を傾斜角に変換して表示することを特徴と
する傾斜計。It has a measurement plane for contacting the surface to be measured and also has a built-in optical gyro with a sensor fiber loop wound in a plane perpendicular to the measurement plane, and converts the angular velocity signal from the optical gyro into a tilt angle. An inclinometer that is characterized by converting and displaying information.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62293790A JPH01136010A (en) | 1987-11-20 | 1987-11-20 | Clinometer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62293790A JPH01136010A (en) | 1987-11-20 | 1987-11-20 | Clinometer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01136010A true JPH01136010A (en) | 1989-05-29 |
Family
ID=17799198
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62293790A Pending JPH01136010A (en) | 1987-11-20 | 1987-11-20 | Clinometer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01136010A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0495710A (en) * | 1990-08-06 | 1992-03-27 | Hotsukou Denshiya:Kk | Apparatus for detecting inclination of steel tower |
US6546639B2 (en) * | 2000-12-10 | 2003-04-15 | Federico Singer | Inclination measurement apparatus |
US6715213B2 (en) * | 2001-07-27 | 2004-04-06 | Lars Richter | 3D angle measurement instrument |
US6722049B2 (en) | 2001-07-30 | 2004-04-20 | Yuval Singer | Inclination measurement apparatus |
-
1987
- 1987-11-20 JP JP62293790A patent/JPH01136010A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0495710A (en) * | 1990-08-06 | 1992-03-27 | Hotsukou Denshiya:Kk | Apparatus for detecting inclination of steel tower |
US6546639B2 (en) * | 2000-12-10 | 2003-04-15 | Federico Singer | Inclination measurement apparatus |
US6715213B2 (en) * | 2001-07-27 | 2004-04-06 | Lars Richter | 3D angle measurement instrument |
US6722049B2 (en) | 2001-07-30 | 2004-04-20 | Yuval Singer | Inclination measurement apparatus |
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