Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6017043B2 - How to measure the distance between two parallel planes - Google Patents
[go: Go Back, main page]

JPS6017043B2 - How to measure the distance between two parallel planes - Google Patents

How to measure the distance between two parallel planes

Info

Publication number
JPS6017043B2
JPS6017043B2 JP14995479A JP14995479A JPS6017043B2 JP S6017043 B2 JPS6017043 B2 JP S6017043B2 JP 14995479 A JP14995479 A JP 14995479A JP 14995479 A JP14995479 A JP 14995479A JP S6017043 B2 JPS6017043 B2 JP S6017043B2
Authority
JP
Japan
Prior art keywords
planes
parallel
light
distance
measurement
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
Application number
JP14995479A
Other languages
Japanese (ja)
Other versions
JPS5673308A (en
Inventor
明 小野
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP14995479A priority Critical patent/JPS6017043B2/en
Publication of JPS5673308A publication Critical patent/JPS5673308A/en
Publication of JPS6017043B2 publication Critical patent/JPS6017043B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Length Measuring Devices By Optical Means (AREA)

Description

【発明の詳細な説明】 本発明は離間対向した平行2平面をもった物品.の測定
、検査に好適な平行2平面の間隔測定方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention is an article having two spaced parallel planes facing each other. The present invention relates to a method for measuring the distance between two parallel planes suitable for measuring and inspecting.

従来2個の物品の間隔を光学的に測定する方法として第
1図および第2図に示すものが知られている。
2. Description of the Related Art Conventionally, the method shown in FIGS. 1 and 2 is known as a method for optically measuring the distance between two articles.

第1図に示す方法は、物品1,2の間に測定光3として
平行なしーザ光を投射し、その通過光4の光量を光電変
換体などからなるセンサで検出する。そしてこの電気信
号に変換された光童が間隔Wに対応することを利用して
間隔Wを知る方法である。また第2図に示す方法は、測
定光3を細い平行なしーザ光からなる走査光とし、これ
を矢印5方向に平行移動させて物品1および物品2の間
を走査し、両物品1,2間を通過した通過光4を後方に
設けたセンサで受光し、その一走査毎の受光時間が間隔
Wに比例することにより間隔Wを知る方法である。上述
の方法は測定光3としてレーザ光を使用した場合は特に
高精度な測定ができる。しかるにこれらの方法を平行な
2平面の間隔の測定に利用する場合には種々な不都合が
生じるのである。
In the method shown in FIG. 1, parallel laser light is projected as measurement light 3 between articles 1 and 2, and the amount of light 4 passing therethrough is detected by a sensor made of a photoelectric converter or the like. This is a method of knowing the interval W by utilizing the fact that the light output converted into the electric signal corresponds to the interval W. Further, in the method shown in FIG. 2, the measurement light 3 is scanned light consisting of narrow parallel laser light, and is moved in parallel in the direction of the arrow 5 to scan between the articles 1 and 2. In this method, the interval W is determined by receiving the passing light 4 that has passed between the 2 and 2 with a sensor provided at the rear, and the time of receiving the light for each scan is proportional to the interval W. The above-mentioned method allows particularly highly accurate measurement when a laser beam is used as the measurement light 3. However, when these methods are used to measure the distance between two parallel planes, various problems arise.

これをブラウン管の電子銃の製造工程における場合を例
に説明する。第3図は電子銃11の要部を示すもので、
複数個の板状のグリツド12,・・・が離間対向して平
行に設けられていて、間隔Wが所定の値に保たれている
かどうかは厳密に測定される。この測定に上述の光学的
方法を適用する場合は、グリッド12,12を正確に測
定光3と平行に設置しなければならない。すなわち、第
4図において、平行な一対のグリツド12,12の対向
した平行2面13,14の間隔Wを第1図に示す方法で
測定する場合に、グリッド12,12が若干でも測定光
3に対して煩斜した状態で測定したとすると、結局Wで
なくこれより小さいW′が得られることになる。従って
電子銃のように平坦な基準面のないものは、測定に際し
て所定の位置に固定するのが面頚で、作業能率が悪く、
しかも正確を期し難いなどのため一般にシックネスゲー
ジに頼っているのが現状で、精度、能率がともに悪く、
しかもグリッドを傷付ける事故も起きるなどの不都合が
あった。本発明は上述の事情にかんがみてなされたもの
で、測定される物品の平行2面が測定光に平行になる所
定の位置を通るように物品を回動させながら通過光を光
電変換体で受光して測定し、その側定値の最大値を検出
して間隔とする平行2平面の間隔測定方法であって、測
定される平行2平面が測定光に対して煩斜して設置され
ても精度を悪くすることなく測定でき、作業能率を著し
く向上させたものである。
This will be explained using an example of the manufacturing process of an electron gun for a cathode ray tube. FIG. 3 shows the main parts of the electron gun 11.
A plurality of plate-shaped grids 12, . . . are provided in parallel and spaced apart from each other, and it is strictly measured whether the interval W is maintained at a predetermined value. If the optical method described above is applied to this measurement, the grids 12, 12 must be placed exactly parallel to the measurement light 3. That is, in FIG. 4, when measuring the distance W between two opposing parallel surfaces 13 and 14 of a pair of parallel grids 12 and 12 by the method shown in FIG. If the measurement is made in a tilted state, then W', which is smaller than W, will be obtained instead of W. Therefore, in the case of an electron gun that does not have a flat reference surface, it is fixed at a predetermined position during measurement, which reduces work efficiency.
Moreover, because it is difficult to ensure accuracy, the current situation is that we generally rely on thickness gauges, which have poor accuracy and efficiency.
Moreover, there were other inconveniences such as accidents that caused damage to the grid. The present invention has been made in view of the above-mentioned circumstances, and the object to be measured is rotated so that the two parallel surfaces of the object pass through a predetermined position parallel to the measurement light, and the passing light is received by a photoelectric converter. This is a method for measuring the distance between two parallel planes in which the maximum value on that side is detected and the distance is determined, and the accuracy is high even if the two parallel planes to be measured are installed obliquely to the measurement light. This allows measurements to be taken without compromising performance, significantly improving work efficiency.

以下本発明の詳細を実施例により説明する。The details of the present invention will be explained below with reference to Examples.

第5図に示す装置は第1の実施例に使用したもので、第
1図に示した測定方法を改良したものであって、測定さ
れるものはブラウン管の電子銃11である。レーザ発振
装置21から送出された測定光3としてのレーザ光は、
コリメータレンズ体22により直径を拡大されて、その
直径は電子銃11の測定される2平面13,14の間隔
Wよりわずかに大きい状態で2平面13,14の間に投
射される。電子銃11は測定体23に着脱自在に固定さ
れていて、この測定体23はピン24により回動自在に
軸支されている。このピン24と同心の円弧をもった外
端面25は、モータ26の健濠ローラ27に接していて
、測定体23はモータ26の正逆回転により礎漆ローラ
27を介して左右に角度8の間回動する。この回動の中
間において、ある瞬間に平行2面13,14は測定光3
に平行となり、所定の位置を通る。この平行2平面13
,14の回動により、この間を通過するレーザ光3の光
量は2平面13,14がレーザ光3に平行な位置すなわ
ち所定の位置において最大となり、その前後はいずれも
これより小となる。測定体23の後方には光電変換体と
してのセンサ30が設けられていて、レーザ光3の通過
光4は、すべてセンサ3川こ入射する。センサ3川ま入
射光量に応じて変化する出力を出し、これはセンサ3灘
猿笑窪露毒害鱒腿後濠示装置32・に入り、電気信号が
間隔Wに換算されて表示される。
The apparatus shown in FIG. 5 was used in the first embodiment, and is an improved version of the measuring method shown in FIG. 1, in which the electron gun 11 of a cathode ray tube is measured. The laser beam as the measurement light 3 sent out from the laser oscillation device 21 is
The diameter is enlarged by the collimator lens body 22, and the beam is projected between the two planes 13 and 14 with the diameter being slightly larger than the distance W between the two planes 13 and 14 measured by the electron gun 11. The electron gun 11 is detachably fixed to a measuring body 23, and this measuring body 23 is rotatably supported by a pin 24. The outer end surface 25 having an arc concentric with the pin 24 is in contact with the hard moat roller 27 of the motor 26, and the measurement object 23 is moved left and right at an angle of 8 through the foundation lacquer roller 27 by the forward and reverse rotation of the motor 26. Rotate for a while. In the middle of this rotation, at a certain moment the two parallel surfaces 13 and 14
becomes parallel to and passes through a predetermined position. These two parallel planes 13
, 14, the amount of light of the laser beam 3 passing therebetween becomes maximum at a position where the two planes 13 and 14 are parallel to the laser beam 3, that is, at a predetermined position, and becomes smaller both before and after that. A sensor 30 as a photoelectric converter is provided behind the measuring body 23, and all of the passing light 4 of the laser beam 3 is incident on the sensor 3. The sensor 3 outputs an output that changes according to the amount of incident light, which is input to the sensor 3 and the sensor 3, which converts the electric signal into an interval W and displays it.

次に第6図を参照して第2の実施例につき説明する。Next, a second embodiment will be described with reference to FIG.

本実施例は第2図に示した測定方法を改良したものであ
る。レーザ発振装置21から送出された測定光3として
のレーザ光は、集東レンズ35に入り、これの,焦点位
置に回動中心36を置いた振動ミラー37で反射し、こ
の回動中心36に焦点を置いた走査レンズ38に入射す
る。このレーザ光3は走査レンズ38により走査レンズ
38の光軸に平行な細いレーザ光となるが、振動ミラ‐
37の回動によりレーザ光3は実線で示したレーザ光3
の位置3aと破線で示したレーザ光3の位置3bとの間
を矢印5の方向に往復勤しながら後方に置かれた測定す
べき電子銃11に入射する。なお築東レンズ35、振動
ミラー37、走査レンズ38でスキャナ−40を構成し
ている。電子銃11は第1の実施例におけると同様に測
定体23に着脱自在に固定されている。なお測定体23
は第1の実施例と同様に構成されているので、詳細な説
明は省略する。第6図においては2平面13,14が走
査レンズ38の光軸に平行な位置つまり所定の位置にあ
る瞬間が示されている。振動ミラー37の回動によりレ
ーザ光3は2平面13,14の間を走査するが、この2
平面13,14の間を通過した通過光4は、後方に置か
れた光電変換体であるセンサ40‘こ入り、このセンサ
40‘ま通過光4が入射中にのみ電気信号を出力する。
そして振動ミラー37が振動中、すなわちレーザ光3が
走査中は測定体23はパルスモータ26により角度8の
範囲の回動が与えられているので、2平面13,14は
しーザ光3の方向に対し、第4図に示すような煩斜した
位置か別項次完全に平行な所定位置となり、これを過ぎ
て反射側に懐いた位置になる。この間高速で走査が行な
われているので、2平面1.3,14が、例えば第4図
に示すように懐いている場合は間隔W′を走査している
間だけセンサ40からの出力がセンサ401こ接続され
た信号処理装贋41に送られ、丁度2平面13,14が
走査レーザ光3の方向と平行になったとき間隔Wを走査
し、それに応じた時間だけセンサ40から信号処理装置
41に出力が送られる。このように往動または復動の都
度出される信号送出時間の長さは、その走査レーザ光3
の方向と2平面が平行のとき最大となる。信号処理袋贋
41は一定時間内に送られて来る複数個の信号の中から
最大受光時間値を検出し、これを表示装置42に送る。
ここでこの値を間隔Wに換算して表示する。以上詳述し
たように本発明の平行2平面の間隔測定方法は、離間対
向した平行2平面間に、これら平面と平行な測定光を投
射して2平面間の間を通過した通過光を光電変換体で検
出して2平面間の間隔を測定するに際し、平行2平面が
測定光と平行になる所定位置を通過する回動を平行2平
面に与えながら測定するように構成したので、回鰯中に
得られる測定値の中に所定の位置における測定値が必ら
ず含まれているのでこれを検出すればよいから、測定に
際しての2平面の固定は所定の位置近傍でよく、固定が
簡単となり、さらにまた光電変換体により間隔を電気信
号で処理するのと相まって、精度を維持したまま高能率
に測定することができる。
This example is an improvement on the measuring method shown in FIG. The laser beam as the measuring beam 3 sent out from the laser oscillation device 21 enters the focusing lens 35, is reflected by the vibrating mirror 37 whose rotation center 36 is placed at the focal position, and is reflected at the rotation center 36. It enters a focused scanning lens 38. This laser beam 3 is turned into a thin laser beam parallel to the optical axis of the scanning lens 38 by the scanning lens 38.
Due to the rotation of 37, the laser beam 3 changes to the laser beam 3 shown by the solid line.
While reciprocating in the direction of the arrow 5 between the position 3a of the laser beam 3 and the position 3b of the laser beam 3 shown by the broken line, the laser beam 3 enters the electron gun 11 to be measured placed at the rear. Note that the scanner 40 is composed of the Chikuto lens 35, the vibrating mirror 37, and the scanning lens 38. The electron gun 11 is detachably fixed to the measuring body 23 as in the first embodiment. Note that the measurement object 23
Since the configuration is similar to that of the first embodiment, detailed explanation will be omitted. FIG. 6 shows the moment when the two planes 13 and 14 are at a position parallel to the optical axis of the scanning lens 38, that is, at a predetermined position. The laser beam 3 scans between the two planes 13 and 14 by the rotation of the vibrating mirror 37.
The passing light 4 that has passed between the planes 13 and 14 enters a sensor 40' which is a photoelectric converter placed at the rear, and outputs an electrical signal only while the passing light 4 is incident on the sensor 40'.
While the vibrating mirror 37 is vibrating, that is, while the laser beam 3 is scanning, the measurement object 23 is rotated within an angle range of 8 by the pulse motor 26, so that the two planes 13 and 14 are With respect to the direction, the position is either an oblique position as shown in FIG. 4, or a predetermined position completely parallel to the direction shown in FIG. During this period, scanning is performed at high speed, so if the two planes 1, 3, and 14 are aligned as shown in FIG. 401 is sent to the connected signal processing device 41, and when the two planes 13 and 14 are exactly parallel to the direction of the scanning laser beam 3, it scans the interval W, and the signal is sent from the sensor 40 to the signal processing device for a corresponding period of time. The output is sent to 41. In this way, the length of the signal sending time for each forward or backward movement is determined by the scanning laser beam 3.
It is maximum when the direction of and the two planes are parallel. The signal processing bag counterfeit 41 detects the maximum light reception time value from among the plurality of signals sent within a certain period of time, and sends this to the display device 42.
Here, this value is converted into an interval W and displayed. As described in detail above, the method for measuring the distance between two parallel planes of the present invention involves projecting measurement light parallel to these planes between two parallel planes that are spaced apart from each other, and photoelectrically converting the passing light that has passed between the two planes. When measuring the distance between two planes by detecting with a converter, the two parallel planes are configured to rotate while passing through a predetermined position where they become parallel to the measurement light. The measured values obtained during the measurement always include the measured value at a predetermined position, so it is only necessary to detect this, so the two planes can be fixed near the predetermined position during measurement, and the fixing is easy. Furthermore, in combination with processing the distance using an electrical signal using a photoelectric converter, it is possible to measure with high efficiency while maintaining accuracy.

なお実施例においては測定光としてレーザ光を使用した
が、これに限定されず平行な光であればよい。
In the embodiment, a laser beam was used as the measurement light, but the measurement light is not limited to this, and any parallel light may be used.

また測定される物品も電子銃に限定されなし、。Also, the items to be measured are not limited to electron guns.

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

第1図および第2図は従釆例の説明図、第3図は本発明
の各実施例において測定される物品の要部を示す説明斜
視図、第4図は従来例の測定誤差説明図、第5図は本発
明の第1の実施例を実施するための装置の構成説明図、
第6図は本発明の第2の実施例を実施するための装置の
構成説明図である。 3,3′・・・・・・測定光、レーザ光、13,14・
・・・・・2平面、30,40・・・・・・光電変換体
。 第1図第2図 第3図 第4図 第5図 第6図
FIGS. 1 and 2 are explanatory diagrams of subordinate examples, FIG. 3 is an explanatory perspective view showing the main parts of the article measured in each embodiment of the present invention, and FIG. 4 is an explanatory diagram of measurement error in the conventional example. , FIG. 5 is an explanatory diagram of the configuration of an apparatus for carrying out the first embodiment of the present invention,
FIG. 6 is an explanatory diagram of the configuration of an apparatus for carrying out the second embodiment of the present invention. 3, 3'... Measuring light, laser light, 13, 14...
...2 planes, 30, 40...photoelectric conversion body. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6

Claims (1)

【特許請求の範囲】[Claims] 1 離間対向した平行2平面間に上記2平面と平行な測
定光を投射し上記2平面間を通過した上記測定光を光電
変換体で検出して上記2平面の間隔を測定する平行2平
面の間隔測定方法において、上記2平面に上記2平面が
上記測定光に対し平行となる所定位置を通る回動を与え
ながら測定することを特徴とする平行2平面の間隔測定
方法。
1. Measurement light parallel to the two planes is projected between two parallel planes that are spaced apart from each other, and the measurement light that has passed between the two planes is detected by a photoelectric converter to measure the distance between the two planes. A method for measuring a distance between two parallel planes, characterized in that measurement is carried out while subjecting the two planes to rotation passing through a predetermined position where the two planes are parallel to the measurement light.
JP14995479A 1979-11-21 1979-11-21 How to measure the distance between two parallel planes Expired JPS6017043B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14995479A JPS6017043B2 (en) 1979-11-21 1979-11-21 How to measure the distance between two parallel planes

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14995479A JPS6017043B2 (en) 1979-11-21 1979-11-21 How to measure the distance between two parallel planes

Publications (2)

Publication Number Publication Date
JPS5673308A JPS5673308A (en) 1981-06-18
JPS6017043B2 true JPS6017043B2 (en) 1985-04-30

Family

ID=15486217

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14995479A Expired JPS6017043B2 (en) 1979-11-21 1979-11-21 How to measure the distance between two parallel planes

Country Status (1)

Country Link
JP (1) JPS6017043B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63267019A (en) * 1987-04-24 1988-11-04 Matsushita Electric Ind Co Ltd sound equipment

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58139007A (en) * 1982-02-13 1983-08-18 Toshiba Corp Method for measuring distance between two parallel planes
JPS58161809A (en) * 1982-03-19 1983-09-26 Toshiba Corp Device for measuring interval between two parallel planes
JPS61123912U (en) * 1985-01-24 1986-08-04

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63267019A (en) * 1987-04-24 1988-11-04 Matsushita Electric Ind Co Ltd sound equipment

Also Published As

Publication number Publication date
JPS5673308A (en) 1981-06-18

Similar Documents

Publication Publication Date Title
EP0134597B1 (en) Measuring system based on the triangulation principle for the dimensional inspection of an object
US4146327A (en) Optical triangulation gauging system
JPH04232580A (en) Method and apparatus for forming three-dimensional color image
JPH02173505A (en) Light wave interference type minute surface shape measuring instrument
US6353473B1 (en) Wafer thickness measuring apparatus and detection method thereof
US4778271A (en) Photoeletric type measuring method and device
JPH09292334A (en) Surface plasmon sensor
JPS6017043B2 (en) How to measure the distance between two parallel planes
KR20010053281A (en) Method and apparatus for ultrasonic laser testing
JP5487920B2 (en) Optical three-dimensional shape measuring apparatus and optical three-dimensional shape measuring method
JPH10122842A (en) Steel plate flatness measurement method
JPH10170247A (en) Method and device for non-contact measurement of surface roughness
JPH06258040A (en) Laser displacement meter
JPS6262208A (en) Range-finding apparatuws and method
JPH05312538A (en) Three-dimensional shape measuring instrument
JP2638724B2 (en) Vehicle dimension measuring device
CN118999758B (en) A non-contact transceiver integrated device and method for measuring vibration.
JPH08193810A (en) Device for measuring displacement
JPS6136884Y2 (en)
JP2674129B2 (en) Distance measuring device
JPS58169007A (en) Optical position measuring device
JPH0426403B2 (en)
JP3444575B2 (en) Rangefinder
JPS58139007A (en) Method for measuring distance between two parallel planes
JPH05248830A (en) Three-dimensional shape measuring apparatus