JPS5813841B2 - How to measure the amount of movement of an object - Google Patents
How to measure the amount of movement of an objectInfo
- Publication number
- JPS5813841B2 JPS5813841B2 JP4084878A JP4084878A JPS5813841B2 JP S5813841 B2 JPS5813841 B2 JP S5813841B2 JP 4084878 A JP4084878 A JP 4084878A JP 4084878 A JP4084878 A JP 4084878A JP S5813841 B2 JPS5813841 B2 JP S5813841B2
- Authority
- JP
- Japan
- Prior art keywords
- moving object
- amount
- movement
- optical medium
- spatial filter
- 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
Links
Landscapes
- Length Measuring Devices By Optical Means (AREA)
Description
【発明の詳細な説明】
本発明は移動する物体の速度、長さ等の移動量を非接触
且つ高精度で測定する方法の改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a method for measuring the amount of movement of a moving object, such as speed and length, in a non-contact manner and with high precision.
移動する物体、例えば鋼板、鋼線、及び電線等を対象に
速度及び長さ等の移動量を高精度で測定することは工業
上不可欠なことであり、しかも移動物体の温度又は形状
等の関係により、移動量の測定を非接触で行なわなけれ
ばならない場合が多い。It is industrially essential to measure the amount of movement, such as speed and length, of moving objects, such as steel plates, steel wires, and electric wires, with high precision. Therefore, it is often necessary to measure the amount of movement without contact.
そこで、千行光を移動物体に照射して移動物体の影をス
リガラス状の板面に投影し、レンズ系を介して格子状光
電池上に結像させ、この像の動きを電気信号に変換し、
その出力信号の周波数を信号処理回路で演算することに
よって移動物体の長さを測定する方法が本願の出願人に
よって提案されている(特願昭52−59534号)。Therefore, by irradiating a moving object with a thousand lines of light, the shadow of the moving object is projected onto a ground glass plate surface, and an image is formed on a grid-like photocell through a lens system, and the movement of this image is converted into an electrical signal. ,
The applicant of the present application has proposed a method of measuring the length of a moving object by calculating the frequency of the output signal using a signal processing circuit (Japanese Patent Application No. 59534/1982).
この方法をさらに詳しく述べると、第1及び2図に示す
ように移動物体1に対して直角方向から平行光αを照射
する光源6を配置し、この光源6の照射方向の延長線上
にスリガラス状の光学的媒介体7、空間フィルタ4の順
序でそれぞれを配置している。To describe this method in more detail, as shown in FIGS. 1 and 2, a light source 6 that irradiates parallel light α from a direction perpendicular to the moving object 1 is arranged, and a ground glass shape is placed on the extension line of the irradiation direction of this light source 6. The optical media 7 and the spatial filter 4 are arranged in this order.
そして、スリガラス状の光学的媒介付7としては、石英
ガラス、プラスチック等の材個の板を摺面加工によりス
リガラス状にしたものを用いるものであり、又空間フィ
ルタ4はスリット状光電池を移動物体1の移動方向に相
対するように配列してあるものである。The ground glass-like optical medium 7 is made of a plate made of quartz glass, plastic, etc., which has been made into a ground glass state by surface processing, and the spatial filter 4 uses a slit-like photovoltaic cell as a moving object. They are arranged so as to face each other in the direction of movement of the first one.
又光源6としては、発光体の光を凹面鏡に反射させるも
のを用いても又2つのレンズの焦点長さの位置にスリッ
ト板を配置した光学系により発光体の光を平行に放射さ
せるものを用いてもよい。The light source 6 may be one that reflects the light from the light emitter onto a concave mirror, or one that emits the light from the light emitter in parallel using an optical system that has a slit plate placed at the focal length of two lenses. May be used.
又このような光源6の平行光αにより移動物体1の上端
部分を照射することにしたが、移動物体1の下端部分或
はその両方を照射しても勿論よいものである。Further, although the upper end portion of the moving object 1 is irradiated with the parallel light α of the light source 6, it is of course possible to irradiate the lower end portion of the moving object 1 or both.
又平行光を移動物体1に対し直角方向から照射しなくて
もよく、その平行光が移動物体1に交差すればよいもの
である。Further, it is not necessary to irradiate the moving object 1 with parallel light from a direction perpendicular to the moving object 1; it is sufficient that the parallel light intersects the moving object 1.
移動物体1に対して平行光αを照射して移動物体1のシ
ルエットを光学的媒介体7に投影し、その光学的媒介体
7に於ける投影像をレンズ2を通して空間フィルタ4に
投影する。A moving object 1 is irradiated with parallel light α to project the silhouette of the moving object 1 onto an optical medium 7, and the projected image on the optical medium 7 is projected onto a spatial filter 4 through a lens 2.
その為、移動物体1が振動し、或はその移動物体1が形
状、大きさ等に連続性が無いことにより、移動物体1と
レンズ2との間の距離が一定に保持されていなくても、
光学的媒介体7に於ける投影像は、平行光の照射による
ものであるから移動物体1の大きさに一致した大きさと
なる。Therefore, even if the distance between the moving object 1 and the lens 2 is not kept constant because the moving object 1 vibrates or the moving object 1 has no continuity in shape, size, etc. ,
The projected image on the optical medium 7 has a size that matches the size of the moving object 1 because it is produced by irradiation with parallel light.
従って、光学的媒介体7とレンズ2との間の距離L1を
常に一定の関係で保持しておけば、移動物体1を対象に
レンズ2の倍率を常に一定にしたことになる。Therefore, if the distance L1 between the optical medium 7 and the lens 2 is always maintained in a constant relationship, the magnification of the lens 2 with respect to the moving object 1 will always be constant.
しかも光学的媒介体7に於ける投影像の形状を表わす線
は移動物体1の表面むらに対応して光量に変化が生じて
いるものであるから、その光学的媒介体7に於ける投影
像がレンズ2を通して空間フィルタ4に投影されると、
空間フィルタ4は移動物体10表面むらに対応した周波
数を有する電気信号を出力することになり、この空間フ
ィルタ4の出力信号の周波数を例えば第3図のブロック
線図に示すような信号処理回路で積算することにより、
移動物体1の移動量を測定することができるものである
。Moreover, since the line representing the shape of the projected image on the optical medium 7 has a change in light intensity corresponding to the surface unevenness of the moving object 1, the projected image on the optical medium 7 is projected onto the spatial filter 4 through the lens 2,
The spatial filter 4 outputs an electrical signal having a frequency corresponding to the surface unevenness of the moving object 10, and the frequency of the output signal of the spatial filter 4 is determined by a signal processing circuit as shown in the block diagram of FIG. By integrating,
The amount of movement of the moving object 1 can be measured.
但し第3図に示した信号処理回路に於いて、4は上記空
間フィルタであり、この空間フィルタ4から取出された
ランダムな電気信号をトラッキングパスフィルタ回路4
aを通して中心周波数推定回路4bに加えると、この中
心周波数推定回路4bでは、例えば自己相関係数を用い
て中心周波数を検出する。However, in the signal processing circuit shown in FIG.
When the signal is applied to the center frequency estimating circuit 4b through the signal a, the center frequency estimating circuit 4b detects the center frequency using, for example, an autocorrelation coefficient.
このようにして検出された周波数をスケールファクタ回
路4cにより長さパルスに変換し、このパルスをカウン
タ4dにより計数するこフとにより、物体の移動量を測
定するものである。The frequency thus detected is converted into length pulses by the scale factor circuit 4c, and the pulses are counted by the counter 4d, thereby measuring the amount of movement of the object.
か\る上述の提案では移動物体の表面に微小な凹凸があ
る場合は高精度に計測出来るものであるが、移動物体が
例えばポリエチレン、塩化ビニールやアルミパイプで被
覆された表面のなめらかなケーブルでは明確な電気信号
を得ることは出来ず、従って正確に計測することが出来
ないことが見出された。The above proposal can measure with high precision when the surface of a moving object has minute irregularities, but it is difficult to measure when the moving object has a smooth surface covered with polyethylene, vinyl chloride, or aluminum pipe, for example. It has been found that it is not possible to obtain a clear electrical signal and therefore it is not possible to measure accurately.
そこで発明者達はさきに提案された平行光法では表面に
凹凸がある表面の粗い移動物体であれば電気信号を得て
精確に計測できることに着目して、移動物体のなめらか
な表面を一時的に粗面化して信号を得やすくして計測す
る特許請求の範囲に記載の物体の移動量測定方法を提供
するものである。Therefore, the inventors focused on the fact that with the parallel light method proposed earlier, it was possible to accurately measure a moving object with a rough surface by obtaining an electric signal. The object of the present invention is to provide a method for measuring the amount of movement of an object according to the claims, in which the surface is roughened to make it easier to obtain a signal.
本発明の実施例を示す図面にもとづいて詳述すると、第
4図イ,口,ハ及び第5図に示すように、光源6より移
動物体1に平行光αをあてスリガラス状板の光学的媒介
物7に出来た影をレンズ2を介して格子状光電池である
フィルタ4上に結像し、この像の動きによって生じる電
気信号を第3図に;示すようなトラッキングパスフィル
タ回路4a、中心周波数推定回路4b、スケールファク
タ回路4c及びカウンタ4dにより計数し、物体の移動
量を測定しており、装置としては第1,2及び3図に用
いた装置をそのま瓦用いているが、本発明では平行光α
の上流側にメリケン粉などの粉状体9の付着装置8を移
動物体1の真上に設置している。Embodiments of the present invention will be described in detail based on drawings showing embodiments of the present invention. As shown in FIGS. 4A, 4B, and 5, and FIG. The shadow formed on the medium 7 is imaged through the lens 2 onto the filter 4, which is a lattice-shaped photocell, and the electric signal generated by the movement of this image is generated by the tracking pass filter circuit 4a, center as shown in FIG. The frequency estimation circuit 4b, scale factor circuit 4c, and counter 4d count and measure the amount of movement of the object, and the device used in Figures 1, 2, and 3 is used as is, but this In the invention, parallel light α
On the upstream side of the moving object 1, an adhering device 8 for applying powder 9 such as American flour is installed directly above the moving object 1.
付着装置8は粉状体6の出口附近に目の細い金網10が
設けてあり、パイプレーター(図示せず)で振動しなが
ら、粉状体9を移動物体1の表面に一様に落下させてお
り、粉状体9が平行光αを通過してから例えば電気掃除
器などの吸引装置(図示せず)で粉状体9を吸取ってい
る。The adhesion device 8 has a thin wire mesh 10 installed near the outlet of the powder 6, and allows the powder 9 to fall uniformly onto the surface of the moving object 1 while being vibrated by a pipelator (not shown). After the powder 9 passes through the parallel light α, the powder 9 is sucked up by a suction device (not shown) such as a vacuum cleaner.
こうして移動物体1のなめらかな表面を一時に粗面化し
て測定精度を飛躍的に向上している。In this way, the smooth surface of the moving object 1 is simultaneously roughened and the measurement accuracy is dramatically improved.
移動物体1がアルミパイプであって、表面に粉状体(こ
こでは小麦粉を使用した)を付着した場合と、粉状体を
付着しなかった場合の計尺精度を表1に示しているが、
本発明の実施例では信号成分が明確に出力されているの
で平均値又X=3 6 4.6 7vtmに対し、偏差
値’ n−1/X = 0. 1 8 mmと非常に小
さいのに対し、本発明の未実施例では平均値Xが3 6
4.6 7mmになるべきものが、X=250.OO
m7ILと大きくずれているとともに、偏差値σn −
1/Xも65.80mmときわめて大きく偏在している
。Table 1 shows the measuring accuracy when the moving object 1 is an aluminum pipe and the surface is coated with powder (flour was used here) and when no powder is attached. ,
In the embodiment of the present invention, since the signal components are clearly output, the deviation value 'n-1/X = 0. While the average value X is very small at 18 mm, the average value
4.6 What should be 7mm is X=250. OO
There is a large deviation from m7IL, and the deviation value σn −
1/X is also extremely large and unevenly distributed at 65.80 mm.
これは感度を上げるために必然的に出力波形にノイズ成
分が多く含むことになったからである。This is because the output waveform inevitably contains many noise components in order to increase sensitivity.
なお、粉状体90代りにグリースなどの比較的粘度の大
きい粘性物11をローラ12を介して移動物体1に塗布
してもよく、平行光αを通過させる時に表面張力でなめ
らかな面にならないものであればよい。Note that instead of the powder 90, a relatively high viscosity viscous substance 11 such as grease may be applied to the moving object 1 via the roller 12, and the surface tension will not result in a smooth surface when the parallel light α is passed through. It is fine as long as it is something.
又、平行光αを通過させた後は粘性物11をふきとると
よい。Further, it is preferable to wipe off the viscous material 11 after passing the parallel light α.
以上説明したように本発明の測定方法は、なめらかな表
面に粗面を施した移動物体に対して平行光を照射して移
動物体のシルエットをスリガラス状の光学的媒介体に投
影し、その光学的媒介体に生じた投影像を空間フィルタ
に投影し、空間フィルタにより入射光量に対応した周波
数を有する電気信号を出力し、その出力信号の周波数を
信号処理回路で積算して移動物体の移動量を測定するも
のであるから、移動物体が振動し、或はその移動物体が
形状、大きさ等に連続性が無いときであっても、移動物
体を対象にレンズの倍率を常に一定のものとすることが
できるものである。As explained above, the measurement method of the present invention projects a silhouette of the moving object onto an optical medium such as ground glass by irradiating parallel light onto a moving object with a roughened smooth surface. The projected image generated on the target medium is projected onto a spatial filter, the spatial filter outputs an electrical signal having a frequency corresponding to the amount of incident light, and the frequency of the output signal is integrated by a signal processing circuit to determine the amount of movement of the moving object. Therefore, even if the moving object vibrates or has no continuity in shape, size, etc., the magnification of the lens will always be constant for the moving object. It is something that can be done.
又、平行光法で計測する移動物体の表面そのものを粗面
化するのではなく、粉状体や粘性物で移動物体の表面を
みかけ上一時的に粗面化するものであるから、移動物体
の品質を下げることなく、又きわめて簡単に移動物体の
表面を一時的に粗面化するものであり、計測精度を飛躍
的に向上させ、これによって得られる効果はきわめて大
きい。In addition, the surface of the moving object measured by the parallel light method is not roughened itself, but the surface of the moving object is temporarily roughened using powder or viscous material, so the surface of the moving object is not roughened. This method can temporarily roughen the surface of a moving object very easily without reducing the quality of the surface of the moving object, dramatically improving measurement accuracy, and the effect obtained by this is extremely large.
第1図、第2図及び第3図は従来の測定方法の説明図、
第4図イ,口,ハ及び第5図は本発明の一実施例の測定
方法の説明図である。
図中、使用する番号は、1は移動物体、2はレンズ、4
は空間フィルタ、6は光源、7は光学的媒介体、8は付
着装置、9は粉状体、11は粘性物を示す。Figures 1, 2 and 3 are explanatory diagrams of conventional measurement methods;
FIGS. 4A, 4B and 5C are explanatory diagrams of a measuring method according to an embodiment of the present invention. In the figure, the numbers used are 1 for the moving object, 2 for the lens, and 4 for the moving object.
is a spatial filter, 6 is a light source, 7 is an optical medium, 8 is an adhesion device, 9 is a powder, and 11 is a viscous material.
Claims (1)
行光を照射して、前記移動物体のシルエットをスリガラ
ス状の光学的媒介体に投影し、該スリガラス状の光学的
媒介体に於ける投影像をレンズ等の光学系を介して、前
記移動物体の移動方向に相対する関係で光電池等のスリ
ット状光検出素子な配列してなる空間フィルタに投影し
、該空間フィルタで入射光量に対応した周波数を有する
電気信号を出力し、その出力信号の周波数を信号処理回
路で積算して前記移動物体の移動量を測定することを特
徴とする物体の移動量測定方法。 2 なめらかな表面に粗面を施した移動物体に対して千
行光を照射して、前記移動物体のシルエットをシリンド
リカルレンズの如き光学的媒介体により拡大してスリガ
ラス状の光学的媒介体に投影し、該スリガラス状の光学
的媒介体に於ける投影像をレンズ等の光学系を介して、
前記移動物体の移動方向に相対する関係で光電池等のス
リット状光検出素子を配列してなる空間フイルタに投影
し該空間フィルタで入射光量に対応した周波数を有する
電気信号を出力し、その出力信号の周波数を信号処理回
路で積算して前記移動物体の移動量を測定することを特
徴とする物体の移動量測定方法3 移動物体の長手方向
に粉状物を滴下して粗面にした特許請求の範囲第1項又
は第2項記載の物体の移動量測定方法。 4 移動物体の長手方向に粘性物を塗布して粗面にした
特許請求の範囲第1項又は第2項記載の物体の移動量測
定方法。[Claims] 1. A moving object having a smooth surface with a rough surface is irradiated with a thousand lines of light, the silhouette of the moving object is projected onto a ground glass-like optical medium, and the silhouette of the moving object is projected onto a ground glass-like optical medium. A projected image on an optical medium is projected through an optical system such as a lens onto a spatial filter consisting of an array of slit-shaped photodetecting elements such as photocells in a relationship facing the moving direction of the moving object. A method for measuring the amount of movement of an object, characterized in that a spatial filter outputs an electrical signal having a frequency corresponding to the amount of incident light, and a signal processing circuit integrates the frequency of the output signal to measure the amount of movement of the moving object. . 2. A moving object with a roughened smooth surface is irradiated with a thousand lines of light, and the silhouette of the moving object is magnified by an optical medium such as a cylindrical lens and projected onto an optical medium such as ground glass. Then, the projected image on the ground glass optical medium is transmitted through an optical system such as a lens,
The image is projected onto a spatial filter formed by arranging slit-shaped light detection elements such as photocells in a relationship facing the moving direction of the moving object, and the spatial filter outputs an electrical signal having a frequency corresponding to the amount of incident light, and the output signal is A method for measuring the amount of movement of an object, characterized in that the amount of movement of the moving object is measured by integrating the frequencies of A method for measuring the amount of movement of an object according to item 1 or 2. 4. A method for measuring the amount of movement of an object according to claim 1 or 2, wherein the moving object is coated with a viscous material in the longitudinal direction to make the surface rough.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4084878A JPS5813841B2 (en) | 1978-04-06 | 1978-04-06 | How to measure the amount of movement of an object |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4084878A JPS5813841B2 (en) | 1978-04-06 | 1978-04-06 | How to measure the amount of movement of an object |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS54133155A JPS54133155A (en) | 1979-10-16 |
| JPS5813841B2 true JPS5813841B2 (en) | 1983-03-16 |
Family
ID=12591992
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4084878A Expired JPS5813841B2 (en) | 1978-04-06 | 1978-04-06 | How to measure the amount of movement of an object |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5813841B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6028934U (en) * | 1983-08-02 | 1985-02-27 | 株式会社小松製作所 | Lift cylinder device of material feeding device |
| JPH0490138U (en) * | 1991-05-24 | 1992-08-06 |
-
1978
- 1978-04-06 JP JP4084878A patent/JPS5813841B2/en not_active Expired
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6028934U (en) * | 1983-08-02 | 1985-02-27 | 株式会社小松製作所 | Lift cylinder device of material feeding device |
| JPH0490138U (en) * | 1991-05-24 | 1992-08-06 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS54133155A (en) | 1979-10-16 |
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