JP2944002B2 - Method and apparatus for measuring thickness - Google Patents
Method and apparatus for measuring thicknessInfo
- Publication number
- JP2944002B2 JP2944002B2 JP10355091A JP10355091A JP2944002B2 JP 2944002 B2 JP2944002 B2 JP 2944002B2 JP 10355091 A JP10355091 A JP 10355091A JP 10355091 A JP10355091 A JP 10355091A JP 2944002 B2 JP2944002 B2 JP 2944002B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic
- pair
- measured
- transmitting
- units
- 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 - Fee Related
Links
- 238000000034 method Methods 0.000 title claims description 25
- 230000005540 biological transmission Effects 0.000 claims description 44
- 238000005259 measurement Methods 0.000 claims description 35
- 238000012360 testing method Methods 0.000 claims description 13
- 238000012545 processing Methods 0.000 claims description 8
- 238000002604 ultrasonography Methods 0.000 claims description 3
- 238000007493 shaping process Methods 0.000 description 2
- 239000013256 coordination polymer Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
Landscapes
- Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
- Testing Of Optical Devices Or Fibers (AREA)
Description
【0001】[0001]
【産業上の利用分野】この発明は、レンズなどの被測定
物の厚さを超音波を利用して測定する厚さ測定方法およ
びその装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method and apparatus for measuring the thickness of an object to be measured such as a lens using ultrasonic waves.
【0002】[0002]
【従来の技術】一般に、レンズなどの被測定物において
は、マイクロメータなどの機械的な測定装置で厚さを測
定すると、被測定物の表面に傷を付けるため、最近では
超音波を利用して被測定物の厚さを非接触状態で測定す
る方法が検討されている。この一例として、従来では、
発信部と受信部を有する1個の超音波素子を基準となる
テーブルの上方に一定間隔で固定し、これらの間の距離
を予め測定しておき、この状態で超音波素子の発信部か
ら発信した超音波がテーブルの上面で反射して受信部で
受信されるまでの時間を測定し、次に、テーブル上に被
測定物を載置して、発信部から発信した超音波が被測定
物で反射して受信部で受信されるまでの時間を測定する
ことにより、両者の時間差から被測定物の厚さを算出す
る方法が考えられている。2. Description of the Related Art Generally, when a thickness of an object to be measured such as a lens is measured with a mechanical measuring device such as a micrometer, the surface of the object to be measured is scratched. A method of measuring the thickness of an object to be measured in a non-contact state has been studied. As an example of this, conventionally,
One ultrasonic element having a transmitting unit and a receiving unit is fixed at a fixed interval above a table serving as a reference, the distance between them is measured in advance, and in this state, transmission is performed from the transmitting unit of the ultrasonic element. The time until the reflected ultrasonic wave is reflected on the upper surface of the table and received by the receiving unit is measured. Next, the device under test is placed on the table, and the ultrasonic wave transmitted from the transmitting unit is measured by the ultrasonic device. A method of calculating the thickness of the object to be measured from the time difference between the two by measuring the time until the light is reflected and received by the receiving unit has been considered.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、上述し
た厚さ測定方法では、以下のような問題がある。すなわ
ち、超音波素子が1個であるから被測定物の片面測定と
なり、このため両面が曲面であるレンズなどの被測定物
では、テーブル上に載置した際に基準面の位置が明確に
ならないため厚さを測定することができない。また、超
音波は空気中を伝わる速度が温度によって変動するた
め、測定毎に温度補正をしなければ正確な測定値が得ら
れない。さらに、超音波素子の発信部から発信される超
音波は徐々に振幅が大きくなるため、発信時と受信時に
おける超音波の同一箇所を正確に捕らえることが難し
く、計測時間が不正確となり、測定誤差が生じる。この
発明の目的は、被測定物の両面が曲面であっても、正確
に厚さ測定ができ、かつ温度変化に応じた補正も正確に
できる厚さ測定方法を提供するとともに、超音波の発信
時から受信時までの計測時間を正確に捕らえることがで
き、極めて精度の高い測定ができる厚さ測定装置を提供
することである。However, the above-mentioned thickness measuring method has the following problems. That is, since one ultrasonic element is used, one-side measurement of the object to be measured is performed. Therefore, in the case of an object to be measured such as a lens having both curved surfaces, the position of the reference surface is not clear when the object is placed on the table. Therefore, the thickness cannot be measured. Further, since the speed at which the ultrasonic wave travels in the air varies depending on the temperature, an accurate measured value cannot be obtained unless the temperature is corrected for each measurement. In addition, since the amplitude of the ultrasonic wave transmitted from the transmitting section of the ultrasonic element gradually increases, it is difficult to accurately capture the same part of the ultrasonic wave at the time of transmission and reception, and the measurement time becomes inaccurate. An error occurs. SUMMARY OF THE INVENTION An object of the present invention is to provide a thickness measuring method capable of accurately measuring a thickness even when both surfaces of an object to be measured are curved surfaces and accurately correcting the temperature according to a temperature change, and transmitting an ultrasonic wave. It is an object of the present invention to provide a thickness measuring apparatus capable of accurately capturing a measurement time from time to reception and performing extremely accurate measurement.
【0004】[0004]
【課題を解決するための手段】この発明の厚さ測定方法
は、発信部および受信部を有する一対の超音波素子をそ
の中心線を一致させて所定間隔に対向配置し、一方の超
音波素子の発信部から発信した超音波が他方の超音波素
子の受信部で受信されるまでの時間を測定し、この状態
で一対の超音波素子間に基準物体を配置して、各発信部
から発信した超音波が基準物体の表裏面でそれぞれ反射
して各受信部に受信されるまでの各時間を測定する基準
値設定工程と、再度、一方の超音波素子の発信部から発
信した超音波が他方の超音波素子の受信部で受信される
までの時間を測定し、この状態で一対の超音波素子間に
被測定物を配置して、各発信部から発信した超音波が被
測定物の表裏面でそれぞれ反射されて各受信部で受信さ
れるまでの各時間を測定する測定工程と、基準値設定工
程と測定工程とでそれぞれ測定された各測定値および基
準物体の厚さデータを演算部で演算処理して被測定物の
厚さを算出するデータ処理工程とからなることを特徴と
する。また、この発明の厚さ測定装置は、発信部および
受信部をそれぞれ有し、その中心線が一致して所定間隔
で対向配置され、かつこれらの間に基準物体もしくは被
測定物が配置される一対の超音波素子と、これら一対の
超音波素子の各発信部から発信する超音波の振幅が次第
に大きくなって一定振幅となるようにするための駆動信
号を複数発の発信パルスに基づいて出力するとともに、
この超音波の振幅が急変する特定点における発信パルス
をスタート信号として出力する一対の発信回路部と、一
対の超音波素子の各受信部で受信した超音波の波形を処
理してその振幅が急変する特定点における整形パルスを
ストップ信号として出力する一対の受信回路部と、各発
信回路部からのスタート信号と各受信回路部からのスト
ップ信号とが入力するまでの時間を超音波の発信周波数
のn倍の周波数をもつクロックでカウントして検出する
一対のカウンタ部と、一対の超音波素子間に基準物体も
しくは被測定物が配置されていない状態で各カウンタ部
で検出された時間、および一対の超音波素子間に基準物
体もしくは被測定物が配置されているそれぞれの状態で
各カウンタ部で検出された時間、並びに基準物体の厚さ
データを演算処理することにより被測定物の厚さを算出
する演算部とを備えたことを特徴とする。According to a thickness measuring method of the present invention, a pair of ultrasonic elements having a transmitting part and a receiving part are arranged opposite to each other at a predetermined interval so that their center lines coincide with each other, and one ultrasonic element is provided. The time until the ultrasonic wave transmitted from the transmitting part of the other ultrasonic element is received by the receiving part of the other ultrasonic element is measured, and in this state, the reference object is arranged between the pair of ultrasonic elements and transmitted from each transmitting part. A reference value setting step of measuring each time until the received ultrasonic wave is reflected by the front and back surfaces of the reference object and received by each receiving unit, and again, the ultrasonic wave transmitted from the transmitting unit of one ultrasonic element is The time until reception by the receiving unit of the other ultrasonic element is measured, and an object to be measured is placed between the pair of ultrasonic elements in this state, and the ultrasonic waves transmitted from each transmitting unit are transmitted to the object to be measured. Each time from when it is reflected on the front and back sides and received by each receiver A measurement step of measuring, and a data processing step of calculating the thickness of the measured object by performing an arithmetic process on each measured value and the thickness data of the reference object measured in the reference value setting step and the measurement step, respectively, in the arithmetic unit. It is characterized by consisting of. Further, the thickness measuring apparatus of the present invention has a transmitting section and a receiving section, respectively, and their center lines coincide with each other, are arranged at predetermined intervals, and a reference object or an object to be measured is arranged therebetween. A pair of ultrasonic elements and a drive signal for making the amplitude of the ultrasonic waves transmitted from each transmitting section of the pair of ultrasonic elements gradually increase to a constant amplitude are output based on a plurality of transmission pulses. Along with
A pair of transmission circuit sections that output a transmission pulse at a specific point where the amplitude of the ultrasonic wave suddenly changes as a start signal, and a waveform of the ultrasonic wave received by each receiving section of the pair of ultrasonic elements is processed to suddenly change the amplitude. A pair of receiving circuit units that output a shaped pulse at a specific point as a stop signal, and a time until a start signal from each transmitting circuit unit and a stop signal from each receiving circuit unit are input are determined by the transmission frequency of the ultrasonic wave. a pair of counters for counting and detecting with a clock having a frequency of n times, a time detected by each counter in a state where the reference object or the measured object is not arranged between the pair of ultrasonic elements, and Computes the time detected by each counter unit and the thickness data of the reference object in each state where the reference object or the measured object is placed between the ultrasonic elements of Characterized in that an arithmetic unit for calculating the thickness of the object to be measured by Rukoto.
【0005】[0005]
【作用】この発明によれば、発信部および受信部を有す
る一対の超音波素子をその中心線を一致させて所定間隔
で対向配置し、これら一対の超音波素子間に被測定物を
配置して厚さを測定するので、レンズなどのように両面
が曲面に形成された被測定物であっても、基準面を明確
にする必要がないため、簡単かつ正確に測定することが
できる。また、この発明の厚さ測定方法によれば、基準
値設定工程で一方の超音波素子の発信部から発信した超
音波が他方の超音波素子の受信部で受信されるまでの時
間を測定し、測定工程で再度一方の超音波素子の発信部
から発信した超音波が他方の超音波素子の受信部で受信
されるまでの時間を測定するので、基準値設定工程と測
定工程とで超音波の速度が温度変化によって変動しても
両者の測定値により温度補正ができ、被測定物の厚さを
正確に測定することが可能となり、しかも基準値設定工
程で一度基準値を設定すれば、測定工程のみを繰り返す
だけで、被測定物を順次測定することができる。さら
に、この発明の厚さ測定装置によれば、超音波素子の発
信部から発信する超音波の振幅が急変する特定点におけ
る発信パルスをスタート信号として発信回路部からカウ
ンタ部に出力するとともに、超音波素子の受信部で受信
した超音波の波形を受信回路部で処理してその振幅が急
変する特定点における整形パルスをストップ信号として
受信回路部からカウンタ部に出力するので、発信時と受
信時における超音波の同一箇所を正確に捕らえることが
でき、計測時間を正確に決めることができる。しかも、
カウンタ部では発信回路部からのスタート信号と受信回
路部からのストップ信号とが入力するまでの時間を超音
波の発信周波数のn倍の周波数をもつクロックでカウン
トするので、極めて精度の高い厚さ測定が可能となる。According to the present invention, a pair of ultrasonic elements having a transmitting section and a receiving section are arranged facing each other at predetermined intervals so that their center lines coincide with each other, and an object to be measured is arranged between the pair of ultrasonic elements. Since the thickness is measured by using the measuring method, it is not necessary to clarify the reference plane even if the object to be measured has a curved surface such as a lens, so that the measurement can be performed easily and accurately. Further, according to the thickness measuring method of the present invention, the time until the ultrasonic wave transmitted from the transmitting section of one ultrasonic element is received by the receiving section of the other ultrasonic element in the reference value setting step is measured. In the measuring step, the time until the ultrasonic wave transmitted from the transmitting section of one ultrasonic element is received again by the receiving section of the other ultrasonic element is measured. Even if the speed fluctuates due to temperature changes, the temperature can be corrected by the measured values of both, it is possible to accurately measure the thickness of the measured object, and once the reference value is set in the reference value setting step, The object to be measured can be measured sequentially only by repeating the measurement process. Further, according to the thickness measuring apparatus of the present invention, the transmission pulse at a specific point where the amplitude of the ultrasonic wave transmitted from the transmission section of the ultrasonic element changes suddenly is output as a start signal from the transmission circuit section to the counter section, The waveform of the ultrasonic wave received by the receiving unit of the acoustic wave element is processed by the receiving circuit unit, and a shaped pulse at a specific point where the amplitude changes suddenly is output as a stop signal from the receiving circuit unit to the counter unit. , The same location of the ultrasonic wave can be accurately detected, and the measurement time can be accurately determined. Moreover,
The counter unit counts the time until the start signal from the transmission circuit unit and the stop signal from the reception circuit unit are input using a clock having a frequency n times the transmission frequency of the ultrasonic wave. Measurement becomes possible.
【0006】[0006]
【実施例】以下、図1〜図4を参照して、この発明の一
実施例を説明する。図1は厚さ測定装置を示す。この図
において、1は基台である。この基台1上の左側には支
持柱2が立設されている。この支持柱2には縦長の取付
部材3が上下の適宜位置に固定されている。この取付部
材3の右側面の中間にはテーブル4が水平に固定されて
おり、上端部には上支持部材5が上下方向に移動可能に
固定されているとともに、下端部には下支持部材6が固
定されている。テーブル4は基準物体7または被測定物
8を所定位置に載置するためのものであり、その中心部
に貫通孔9が上下に貫通して設けられている。また、上
支持部材5の上部側と下支持部材6の下部側にはそれぞ
れ回路基板10がビス11により取り付けられている。
これら上下の各回路基板10にはそれぞれ第1、第2の
超音波素子12、13がテーブル4を挾んで対向して設
けられている。すなわち、各超音波素子12、13はそ
れぞれ発信部と受信部を内蔵し、その各中心線がテーブ
ル4の貫通孔9の中心と一致して設けられている。この
場合、各超音波素子12、13の対向する先端部にはそ
れぞれ超音波をガイドする超音波ノズル14が各支持部
材5、6の挿通孔5a、6aを通り抜けて突出して設け
られている。なお、各回路基板10は図示ない制御装置
に電気的に接続されている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to FIGS. FIG. 1 shows a thickness measuring device. In this figure, 1 is a base. A support column 2 is erected on the left side of the base 1. A vertically long attachment member 3 is fixed to the support column 2 at an appropriate upper and lower position. A table 4 is fixed horizontally in the middle of the right side surface of the mounting member 3, an upper support member 5 is fixed to an upper end portion so as to be vertically movable, and a lower support member 6 is fixed to a lower end portion. Has been fixed. The table 4 is for placing the reference object 7 or the device under test 8 at a predetermined position, and has a through hole 9 vertically penetrating the center thereof. A circuit board 10 is attached to the upper side of the upper support member 5 and the lower side of the lower support member 6 by screws 11.
First and second ultrasonic elements 12 and 13 are provided on the upper and lower circuit boards 10 so as to face each other with the table 4 interposed therebetween. That is, each of the ultrasonic elements 12 and 13 has a built-in transmitting unit and a receiving unit, and each of the center lines is provided so as to coincide with the center of the through hole 9 of the table 4. In this case, ultrasonic nozzles 14 for guiding ultrasonic waves are provided at the opposing distal ends of the ultrasonic elements 12 and 13 so as to protrude through the insertion holes 5a and 6a of the support members 5 and 6, respectively. Each circuit board 10 is electrically connected to a control device (not shown).
【0007】図2は上述した厚さ測定装置の回路構成を
示す。この厚さ測定装置は、対向する第1、第2の超音
波素子12、13毎にそれぞれ発信回路部20、21、
受信回路部22、23、カウンタ部24、25、および
切替スイッチ26、27を備え、これらをCPU(中央
演算処理装置)28で制御する構成となっている。CP
U28は装置全般の制御および測定データの演算処理な
どを行うものであり、操作スイッチ部29から測定開始
信号および基準物体7の厚さデータが与えられ、測定開
始信号に基づいて第1、第2の切替スイッチ26、27
を同時もしくは選択的に閉成し、各発信回路部20、2
1の両者もしくはいずれかに発信開始を指示する。第
1、第2の発信回路部20、21は、CPU28からの
指令に基づいて各超音波素子12、13の発信部から発
信する超音波の振幅が図3に示すように次第に大きくな
って一定振幅となるようにするための駆動信号を複数発
(図3では6発)の発信パルスに基づいて出力するとと
もに、超音波の振幅が急に大きくなる特定点Aにおける
発信パルスをスタート信号として各カウンタ部24、2
5に出力する。すなわち、超音波は図3に示す発信パル
スに基づく駆動信号に応じて次第に振幅が大きくなり、
発信パルスの2〜4発目で急に大きくなって安定する。
この急に大きくなって安定する箇所が特定点Aとなる。
この特定点Aは超音波素子によって異なるが、この実施
例の超音波素子12、13では発信パルスの3発目が特
定点Aとなる。この場合、第1の発信回路20は、一対
の超音波素子12、13の間に基準物体7または被測定
物8が配置されていない状態では第2の超音波素子13
側のカウンタ25にスタート信号を出力し、一対の超音
波素子12、13の間に基準物体7または被測定物8が
配置されている状態では第1の超音波素子12側のカウ
ンタ24にスタート信号を出力する。同様に、第2の発
信回路21は、一対の超音波素子12、13の間に基準
物体7または被測定物8が配置されていない状態では第
1の超音波素子12側のカウンタ24にスタート信号を
出力し、一対の超音波素子12、13の間に基準物体7
または被測定物8が配置されている状態では第1の超音
波素子12側のカウンタ25にスタート信号を出力す
る。第1、第2の受信回路部22、23は、それぞれ各
超音波素子12、13の各受信部で受信した超音波の波
形を整形処理するとともに、受信した超音波の振幅が急
に大きくなる特定点Bと対応する整形パルスをストップ
信号として各カウンタ部24、25に出力する。すなわ
ち、受信した超音波は発信した超音波と同じであるか
ら、整形パルスの3発目で急に大きくなって安定する。
この3発目が特定点Bとなる。第1、第2のカウンタ部
24、25は各発信回路部20、21からのスタート信
号と各受信回路部22、23からのストップ信号とが入
力するまでの時間を超音波の発信周波数(例えば400
KHz)のn倍(例えば50倍)の周波数(例えば20
MHz)のクロックでカウントし、このカウント値(以
下、測定値という)をCPU28に出力する。なお、C
PU28は、各カウンタ部24、25から与えられた測
定値、および操作スイッチ部29で入力された基準物体
7の厚さデータを演算処理して被測定物8の厚さを算出
し、この算出結果を表示部30に表示するとともに、パ
ーソナルコンピュータなどの外部機器31との間でデー
タの授受を行う。FIG. 2 shows a circuit configuration of the above-described thickness measuring apparatus. The thickness measuring device includes transmitting circuit units 20, 21, for each of the opposed first and second ultrasonic elements 12, 13, respectively.
It has receiving circuit units 22 and 23, counter units 24 and 25, and changeover switches 26 and 27, and these are controlled by a CPU (Central Processing Unit) 28. CP
U28 performs overall control of the apparatus, arithmetic processing of measurement data, and the like. A measurement start signal and thickness data of the reference object 7 are given from the operation switch unit 29, and first and second signals are given based on the measurement start signal. Changeover switches 26 and 27
Are simultaneously or selectively closed, and each of the transmission circuit units 20, 2
1 or both of them are instructed to start transmission. The first and second transmitting circuit units 20 and 21 are configured such that the amplitudes of the ultrasonic waves transmitted from the transmitting units of the respective ultrasonic elements 12 and 13 gradually increase and become constant as shown in FIG. A drive signal for obtaining an amplitude is output based on a plurality of (six in FIG. 3) transmission pulses, and a transmission pulse at a specific point A where the amplitude of the ultrasonic wave suddenly increases is used as a start signal. Counter unit 24, 2
5 is output. That is, the amplitude of the ultrasonic wave gradually increases according to the drive signal based on the transmission pulse shown in FIG.
It increases suddenly and becomes stable at the second to fourth emission pulses.
The point where the size suddenly increases and becomes stable is the specific point A.
Although the specific point A differs depending on the ultrasonic element, the third point of the transmission pulse is the specific point A in the ultrasonic elements 12 and 13 of this embodiment. In this case, the first transmitting circuit 20 operates the second ultrasonic element 13 when the reference object 7 or the device under test 8 is not arranged between the pair of ultrasonic elements 12 and 13.
The start signal is output to the counter 25 of the first ultrasonic element 12 and the start signal is output to the counter 24 of the first ultrasonic element 12 when the reference object 7 or the DUT 8 is disposed between the pair of ultrasonic elements 12 and 13. Output a signal. Similarly, the second transmission circuit 21 starts the counter 24 on the first ultrasonic element 12 side when the reference object 7 or the device under test 8 is not arranged between the pair of ultrasonic elements 12 and 13. A signal is output, and the reference object 7 is placed between the pair of ultrasonic elements 12 and 13.
Alternatively, a start signal is output to the counter 25 on the first ultrasonic element 12 side when the device under test 8 is arranged. The first and second receiving circuit units 22 and 23 shape the waveforms of the ultrasonic waves received by the respective receiving units of the ultrasonic elements 12 and 13, respectively, and the amplitude of the received ultrasonic waves suddenly increases. The shaped pulse corresponding to the specific point B is output to each of the counters 24 and 25 as a stop signal. That is, since the received ultrasonic wave is the same as the transmitted ultrasonic wave, it becomes large suddenly and becomes stable at the third generation of the shaping pulse.
This third shot is the specific point B. The first and second counter units 24 and 25 determine the time until the start signal from each of the transmission circuit units 20 and 21 and the stop signal from each of the reception circuit units 22 and 23 are input by the transmission frequency of the ultrasonic wave (for example, 400
KHz) of n times (for example, 50 times) frequency (for example, 20 times)
MHz), and outputs the count value (hereinafter referred to as a measured value) to the CPU 28. Note that C
The PU 28 calculates the thickness of the DUT 8 by performing arithmetic processing on the measurement values given from the respective counter units 24 and 25 and the thickness data of the reference object 7 input from the operation switch unit 29. The result is displayed on the display unit 30, and data is exchanged with an external device 31 such as a personal computer.
【0008】次に、図4(a)〜図4(d)を参照し
て、厚さ測定方法を説明する。まず、図4(a)に示す
ように、一定間隔で上下に対向配置された第1、第2の
超音波素子12、13間に何も配置しない状態、つまり
テーブル4上に基準物体7や被測定物8を載置しない状
態で、第1の超音波素子12の発信部から発信した超音
波が第2の超音波素子13の受信部に受信されるまでの
時間TR(または第2の超音波素子13の発信部から発
信した超音波が第1の超音波素子12の受信部に受信さ
れるまでの時間TR)を測定する。この場合には、ま
ず、操作スイッチ部29を操作してCPU28に測定開
始指令を与えると、CPU28が例えば第1の切替スイ
ッチ26を閉成した後、第1の発信回路部20に発信開
始を指示する。すると、第1の発信回路部20は、6発
の発信パルスに基づいて駆動信号を出力し、第1の超音
波素子12の発信部から400KHzの超音波を発信さ
せるとともに、特定点Aと対応する3発目の発信パルス
をスタート信号として出力して第2のカウンタ部25で
のカウントを開始させる。そして、第1の超音波素子1
2の発信部から発信した超音波が第2の超音波素子13
の受信部で受信されると、この受信された超音波の波形
が第2の受信回路部23で整形処理され、この受信回路
部23が特定点Bと対応する3発目の整形パルスをスト
ップ信号として出力して第2のカウンタ部25でのカウ
ントを停止させる。このとき、第2のカウンタ部25で
は、スタート信号が入力した時点からストップ信号が入
力する時点までの時間TRを発信周波数の約50倍の周
波数(20MHz)のクロックでカウントし、その測定
値をCPU28に出力する。Next, a thickness measuring method will be described with reference to FIGS. 4 (a) to 4 (d). First, as shown in FIG. 4A, a state in which nothing is arranged between the first and second ultrasonic elements 12 and 13 which are vertically arranged at regular intervals, that is, the reference object 7 or A time T R (or a second time) until the ultrasonic wave transmitted from the transmitting unit of the first ultrasonic element 12 is received by the receiving unit of the second ultrasonic element 13 in a state where the device under test 8 is not placed. ultrasonic wave transmitted from the transmitting portion of the ultrasonic element 13 measures the time T R) to be received in the receiving portion of the first ultrasonic element 12. In this case, first, when the operation switch unit 29 is operated to give a measurement start command to the CPU 28, the CPU 28 closes the first switch 26, for example, and then starts transmission to the first transmission circuit unit 20. To instruct. Then, the first transmission circuit unit 20 outputs a drive signal based on the six transmission pulses, transmits an ultrasonic wave of 400 KHz from the transmission unit of the first ultrasonic element 12, and corresponds to the specific point A. The third transmission pulse to be output is output as a start signal, and the second counter 25 starts counting. Then, the first ultrasonic element 1
The ultrasonic wave transmitted from the transmitting unit 2 is the second ultrasonic element 13
Is received by the receiving unit, the waveform of the received ultrasonic wave is shaped by the second receiving circuit unit 23, and the receiving circuit unit 23 stops the third shaped pulse corresponding to the specific point B. It is output as a signal to stop counting in the second counter unit 25. At this time, the second counter 25 counts the clock of about 50 times the frequency (20 MHz) of the transmission frequency of the time T R from the time the start signal is input to when the stop signal is inputted, the measured value Is output to the CPU 28.
【0009】この後、速やかにテーブル4上に基準物体
7を載置する。つまり図4(b)に示すように、一対の
超音波素子12、13間に基準物体7(厚さtR)を配
置する。この状態で、各超音波素子12、13の各発信
部から発信した超音波が基準物体7の表裏面でそれぞれ
反射されて各超音波素子12、13の各受信部で受信さ
れるまでの各時間(2×TR1、2×TR2)を測定する。
この場合には、まず、操作スイッチ部29で基準物体7
の厚さtRをCPU28に入力した後、操作スイッチ部
29から測定開始指示をCPU28に与える。すると、
CPU28は第1、第2の発信回路部20、21にそれ
ぞれ発信開始指示を与えるので、各発信回路部20、2
1は上述と同様に第1、第2の超音波素子12、13の
各発信部から超音波を発信させるとともに、スタート信
号を第1、第2のカウンタ部24、25に出力して各カ
ウンタ部24、25でのカウントを開始させる。そし
て、各発信部から発信した超音波が基準物体7の表裏面
で反射されて各超音波素子12、13の各受信部で受信
されると、上述と同様に各受信回路部22、23からス
トップ信号が各カウンタ部24、25に与えられる。こ
のとき、各カウンタ部24、25では、スタート信号が
入力した時点からストップ信号が入力する時点までの各
時間(2×TR1、2×TR2)を発信周波数の約50倍の
周波数(20MHz)のクロックでカウントし、その測
定値をCPU28に出力する。これにより基準値設定工
程が終了する。なお、この基準値設定工程は、一度設定
すれば、第1、第2の超音波素子12、13の間隔を変
えない限り、設定し直す必要はない。Thereafter, the reference object 7 is quickly placed on the table 4. That is, as shown in FIG. 4B, the reference object 7 (thickness t R ) is arranged between the pair of ultrasonic elements 12 and 13. In this state, the ultrasonic waves transmitted from the transmitting units of the ultrasonic elements 12 and 13 are reflected by the front and back surfaces of the reference object 7 and received by the receiving units of the ultrasonic elements 12 and 13 respectively. The time (2 × T R1 , 2 × T R2 ) is measured.
In this case, first, the reference object 7 is
After entering the thickness t R in CPU 28, supplied from the operation switch unit 29 a measurement start instruction to the CPU 28. Then
The CPU 28 gives a transmission start instruction to the first and second transmission circuit units 20 and 21, respectively.
1 transmits an ultrasonic wave from each of the transmitting units of the first and second ultrasonic elements 12 and 13 in the same manner as described above, and outputs a start signal to the first and second counter units 24 and 25 to output each counter. The counting in the units 24 and 25 is started. Then, when the ultrasonic waves transmitted from the respective transmitting units are reflected on the front and back surfaces of the reference object 7 and received by the respective receiving units of the respective ultrasonic elements 12 and 13, from the respective receiving circuit units 22 and 23 as described above. A stop signal is provided to each of the counters 24 and 25. At this time, each of the counters 24 and 25 calculates each time (2 × T R1 , 2 × T R2 ) from the time when the start signal is input to the time when the stop signal is input to a frequency (20 MHz) which is about 50 times the transmission frequency. ), And outputs the measured value to the CPU 28. Thus, the reference value setting step is completed. Once the reference value setting step is set, there is no need to reset the reference value unless the interval between the first and second ultrasonic elements 12 and 13 is changed.
【0010】基準値を設定した後は、被測定物8の厚さ
tSを測定するのであるが、この場合には、まず、上述
と同様に、再度、テーブル4上に何も載置しない状態、
つまり図4(c)に示すように、一定間隔で対向配置さ
れた各超音波素子12、13間に何も配置しない状態
で、第1の超音波素子12の発信部から発信した超音波
が第2の超音波素子13の受信部に受信されるまでの時
間TSを第2のカウンタ部25でカウントし、その測定
値をCPU28に出力する。この後、速やかにテーブル
4上に被測定物8を載置する。つまり図4(d)に示す
ように、各超音波素子12、13間に被測定物8を配置
する。この状態で、上述と同様に、各超音波素子12、
13の各発信部から発信した超音波が被測定物8の表裏
面でそれぞれ反射されて各超音波素子12、13の各受
信部で受信されるまでの各時間(2×TS1、2×TS2)
を各カウンタ部24、25でカウントし、その測定値を
CPU28に出力する。これにより測定工程が終了す
る。After setting the reference value, the thickness t S of the object 8 is measured. In this case, nothing is placed on the table 4 again as described above. Status,
That is, as shown in FIG. 4C, in a state in which nothing is arranged between the ultrasonic elements 12 and 13 which are arranged at regular intervals and opposed to each other, the ultrasonic wave transmitted from the transmitting section of the first ultrasonic element 12 The second counter 25 counts the time T S until it is received by the receiving unit of the second ultrasonic element 13, and outputs the measured value to the CPU 28. Thereafter, the device under test 8 is immediately placed on the table 4. That is, as shown in FIG. 4D, the device under test 8 is arranged between the ultrasonic elements 12 and 13. In this state, similarly to the above, each ultrasonic element 12,
Each time (2 × T S1 , 2 ×) until the ultrasonic wave transmitted from each of the transmitting units 13 is reflected on the front and back surfaces of the DUT 8 and received by each of the receiving units of the ultrasonic elements 12 and 13. T S2 )
Is counted by the counter units 24 and 25, and the measured value is output to the CPU 28. This ends the measurement process.
【0011】測定工程が終了すると、基準値設定工程と
測定工程とでそれぞれ測定された各測定値(TR、2×
TR1、2×TR2、TS、2×TS1、2×TS2)および基
準物体7の厚さtRをCPU28で演算処理して被測定
物8の厚さtSを算出し、この算出結果を表示部30に
表示するとともに、外部機器31に与え、この外部機器
31との間でデータの授受を行う。これによりデータ処
理工程が終了する。この場合、被測定物8の厚さtSは
以下の式によってCPU28の演算処理で算出される。
すなわち、基準値設定工程と測定工程とで、一対の超音
波素子12、13の間隔が一定であるから、 V1×TR=V2×TS …………(1) ただし、V1は基準値設定工程における超音波の速度、
V2は測定工程における超音波の速度であり、 V1=tR/(TR−TR1−TR2) …………(2) V2=tS/(TS−TS1−TS2) …………(3) となる。これら式(2)と式(3)を式(1)に代入す
ると、When the measurement process is completed, each measured value (T R , 2 × 2) measured in the reference value setting process and the measurement process, respectively.
T R1 , 2 × T R2 , T S , 2 × T S1 , 2 × T S2 ) and the thickness t R of the reference object 7 are processed by the CPU 28 to calculate the thickness t S of the DUT 8, The calculation result is displayed on the display unit 30 and is given to the external device 31 to exchange data with the external device 31. This ends the data processing step. In this case, the thickness t S of the DUT 8 is calculated by the CPU 28 using the following equation.
That is, since the distance between the pair of ultrasonic elements 12 and 13 is constant in the reference value setting step and the measurement step, V 1 × T R = V 2 × T S (1) where V 1 Is the speed of the ultrasonic wave in the reference value setting process,
V 2 is the ultrasonic velocity in the measuring step, V 1 = t R / ( T R -T R1 -T R2) ............ (2) V 2 = t S / (T S -T S1 -T S2 )... (3) When these equations (2) and (3) are substituted into equation (1),
【数1】 となり、これを整理すると、(Equation 1) And if you organize this,
【数2】 となり、これにより被測定物8の厚さtSが求められ
る。(Equation 2) Thus, the thickness t S of the device under test 8 is obtained.
【0012】このように、上述した厚さ測定方法では、
基準値設定工程で第1の超音波素子12の発信部から発
信した超音波が第2の超音波素子13の受信部で受信さ
れるまでの時間TRを測定し、測定工程で再度第1の超
音波素子12の発信部から発信した超音波が第2の超音
波素子13の受信部で受信されるまでの時間TSを測定
することにより、基準値設定工程と測定工程とで超音波
の速度が温度変化によって変動しても、両者の測定値に
より温度補正することができ、このため温度変化に左右
されずに被測定物8の厚さtSを正確に測定することが
できる。しかも、基準値設定工程で一度基準値を設定す
れば、第1、第2の超音波素子12、13の間隔を変え
ない限り、設定し直す必要がないため、測定工程のみを
繰り返すだけで、順次被測定物8を正確に測定すること
ができ、能率よく測定作業を行うことができる。As described above, in the thickness measuring method described above,
Ultrasonic wave transmitted from the transmitting portion of the reference value setting step in the first ultrasonic element 12 measures the time T R until it is received by the receiver of the second ultrasonic element 13, a first measurement step again By measuring the time T S until the ultrasonic wave transmitted from the transmitting unit of the ultrasonic element 12 is received by the receiving unit of the second ultrasonic element 13, the ultrasonic wave can be measured in the reference value setting step and the measuring step. Even if the speed fluctuates due to a change in temperature, the temperature can be corrected based on the measured values of the two, so that the thickness t S of the DUT 8 can be accurately measured without being affected by the change in temperature. Moreover, once the reference value is set in the reference value setting step, there is no need to reset it unless the interval between the first and second ultrasonic elements 12 and 13 is changed. Therefore, only the measurement step is repeated. The device under test 8 can be measured sequentially and accurately, and the measuring operation can be performed efficiently.
【0013】また、上述した厚さ測定装置では、発信部
および受信部を有する第1、第2の超音波素子12、1
3をその中心線を一致させて所定間隔で対向配置したの
で、レンズなどのように両面が曲面に形成された被測定
物8であっても、従来のように被測定物の基準面を明確
にする必要がないため、各超音波素子12、13間に配
置するだけで容易に被測定物8の厚さを測定することが
できる。この場合、被測定物8はピン玉程度以上の曲率
半径をもつレンズであれば充分に測定することができ
る。In the above-described thickness measuring apparatus, the first and second ultrasonic elements 12, 1 having a transmitting section and a receiving section are provided.
3 is arranged opposite to each other at a predetermined interval with its center line coincident, so that the reference surface of the object to be measured can be clearly defined even in the case of the object to be measured 8 having a curved surface such as a lens. Therefore, the thickness of the DUT 8 can be easily measured simply by disposing it between the ultrasonic elements 12 and 13. In this case, the object to be measured 8 can be sufficiently measured by using a lens having a radius of curvature equal to or larger than that of a pin ball.
【0014】さらに、この厚さ測定装置では、各発信回
路部20、21の6発の発信パルスに基づく駆動信号に
より各超音波素子12、13の各発信部から発信する超
音波の振幅が次第に大きくなるとともに、この振幅が急
に大きくなって安定する特定点Aと対応する3発目の発
信パルスを各カウンタ部24、25でカウントを開始す
るスタート信号として各発信回路部20、21から出力
し、また各超音波素子12、13の各受信部で受信され
た超音波を各受信回路部22、23で波形整形処理し
て、受信した超音波の振幅が急に大きくなって安定する
特定点Bと対応する3発目の受信パルスを各カウンタ部
24、25でのカウントを停止させるストップ信号とし
て各受信回路部22、23から出力するので、基準値設
定工程および測定工程で発信時と受信時における超音波
の同一箇所を正確に捕らえることができ、計測時間を正
確に決めることができる。しかも、各カウンタ部25
は、発信回路部20、21からのスタート信号と受信回
路部22、23からのストップ信号とが入力するまでの
計測時間を発信周波数のn倍の周波数のクロックでカウ
ントするので、極めて精度の高い厚さ測定ができる。例
えば、超音波素子12、13の各発信部から発信される
超音波の発信周波数が400KHzであれば、超音波の
発信時から受信時までの計測時間を発信周波数の50倍
の周波数をもつクロック、例えば20MHzのクロック
でカウントすると、約16μmの分解能を得ることがで
き、非常に精度の高い測定が可能になる。Further, in this thickness measuring device, the amplitude of the ultrasonic wave transmitted from each transmitting section of each of the ultrasonic elements 12 and 13 is gradually increased by a drive signal based on the six transmitting pulses of each transmitting circuit section 20 and 21. The third transmission pulse corresponding to the specific point A, at which the amplitude suddenly increases and stabilizes as the amplitude increases, is output from each of the transmission circuit units 20 and 21 as a start signal to start counting in each of the counter units 24 and 25. In addition, the ultrasonic waves received by the respective receiving units of the respective ultrasonic elements 12 and 13 are subjected to waveform shaping processing by the respective receiving circuit units 22 and 23, and the amplitude of the received ultrasonic waves suddenly increases and becomes stable. Since the third reception pulse corresponding to the point B is output from each of the reception circuit units 22 and 23 as a stop signal for stopping the counting in each of the counter units 24 and 25, the reference value setting step and the measurement process are performed. In ultrasound same position when placing the at reception can catch accurately, the measurement time can be determined accurately. Moreover, each counter 25
Counts the measurement time until a start signal from the transmission circuit units 20 and 21 and a stop signal from the reception circuit units 22 and 23 are input by a clock having a frequency n times the transmission frequency, so that the accuracy is extremely high. The thickness can be measured. For example, if the transmitting frequency of the ultrasonic wave transmitted from each transmitting unit of the ultrasonic elements 12 and 13 is 400 KHz, the measuring time from the time of transmitting the ultrasonic wave to the time of receiving the ultrasonic wave is a clock having a frequency 50 times the transmitting frequency. For example, when counting with a clock of 20 MHz, a resolution of about 16 μm can be obtained, and measurement with extremely high accuracy can be performed.
【0015】[0015]
【発明の効果】この発明によれば、発信部および受信部
を有する一対の超音波素子をその中心線を一致させて所
定間隔で対向配置し、これら一対の超音波素子間に被測
定物を配置して厚さを測定するので、レンズなどのよう
に両面が曲面に形成された被測定物であっても、基準面
を明確にする必要がないため、簡単かつ正確に測定する
ことができる。また、この発明の厚さ測定方法によれ
ば、基準値設定工程で一方の超音波素子の発信部から発
信した超音波が他方の超音波素子の受信部で受信される
までの時間を測定し、測定工程で再度一方の超音波素子
の発信部から発信した超音波が他方の超音波素子の受信
部で受信されるまでの時間を測定するので、基準値設定
工程と測定工程とで超音波の速度が温度変化によって変
動しても両者の測定値により温度補正ができ、温度変化
に左右されずに被測定物の厚さを正確に測定することが
でき、しかも基準値設定工程で一度基準値を設定すれ
ば、測定工程のみを繰り返すだけで、順次被測定物を正
確に測定することができ、能率よく測定作業を行うこと
ができる。さらに、この発明の厚さ測定装置によれば、
超音波素子の発信部から発信する超音波の振幅が急変す
る特定点における発信パルスをスタート信号として発信
回路部からカウンタ部に出力するとともに、超音波素子
の受信部で受信した受信超音波の波形を受信回路で処理
して振幅が急変する特定点における整形パルスをストッ
プ信号として受信回路部からカウンタ部に出力するの
で、発信時と受信時における超音波の同一箇所を正確に
捕らえることができ、計測時間を正確に決めることがで
きる。しかも、カウンタ部では発信回路部のスタート信
号と受信回路部のストップ信号とが入力するまでの時間
を発信周波数のn倍の周波数をもつクロックでカウント
するので、極めて精度の高い厚さ測定ができる。According to the present invention, a pair of ultrasonic elements having a transmitting part and a receiving part are arranged facing each other at predetermined intervals with their center lines coincident with each other, and an object to be measured is placed between the pair of ultrasonic elements. Since the thickness is measured by arranging, it is possible to measure easily and accurately even if the measurement target has a curved surface such as a lens, because there is no need to clarify the reference surface. . Further, according to the thickness measuring method of the present invention, the time until the ultrasonic wave transmitted from the transmitting section of one ultrasonic element is received by the receiving section of the other ultrasonic element in the reference value setting step is measured. In the measuring step, the time until the ultrasonic wave transmitted from the transmitting section of one ultrasonic element is received again by the receiving section of the other ultrasonic element is measured. Even if the speed changes due to temperature change, the temperature can be corrected by the measured values of both, the thickness of the object to be measured can be accurately measured without being affected by the temperature change, and the reference is set once in the reference value setting process. If the value is set, the object to be measured can be sequentially and accurately measured only by repeating the measurement process alone, and the measurement operation can be performed efficiently. Furthermore, according to the thickness measuring device of the present invention,
The transmission pulse at a specific point where the amplitude of the ultrasonic wave transmitted from the transmission unit of the ultrasonic element suddenly changes is output as a start signal from the transmission circuit unit to the counter unit, and the waveform of the received ultrasonic wave received by the reception unit of the ultrasonic element Is processed by the receiving circuit and the shaped pulse at a specific point where the amplitude changes suddenly is output as a stop signal from the receiving circuit unit to the counter unit, so that the same place of the ultrasonic wave at the time of transmission and at the time of reception can be accurately captured, The measurement time can be determined accurately. In addition, since the counter section counts the time until the start signal of the transmission circuit section and the stop signal of the reception circuit section are input using a clock having a frequency n times the transmission frequency, extremely accurate thickness measurement can be performed. .
【図1】厚さ測定装置の概略側面図。FIG. 1 is a schematic side view of a thickness measuring device.
【図2】厚さ測定装置の回路構成を示すブロック図。FIG. 2 is a block diagram showing a circuit configuration of the thickness measuring device.
【図3】発信側と受信側とにおける各超音波の波形と各
パルスとのタイミング図。FIG. 3 is a timing chart of waveforms of ultrasonic waves and pulses on a transmitting side and a receiving side.
【図4】厚さ測定方法を示す工程図。FIG. 4 is a process chart showing a thickness measuring method.
7 基準物体 8 被測定物 12、13 超音波素子 20、21 発信回路部 22、23 受信回路部 24、25 カウンタ部 28 CPU A、B 特定点 7 Reference object 8 Device under test 12, 13 Ultrasonic element 20, 21 Transmitting circuit unit 22, 23 Receiving circuit unit 24, 25 Counter unit 28 CPU A, B Specific point
フロントページの続き (56)参考文献 特開 昭61−104211(JP,A) 実開 昭55−59311(JP,U) 実開 昭49−79260(JP,U) 特公 昭49−16830(JP,B1) (58)調査した分野(Int.Cl.6,DB名) G01B 17/00 - 17/04 G01M 11/00 Continuation of the front page (56) References JP-A-61-104211 (JP, A) JP-A-55-59311 (JP, U) JP-A-49-79260 (JP, U) JP-B-49-16830 (JP) , B1) (58) Fields surveyed (Int. Cl. 6 , DB name) G01B 17/00-17/04 G01M 11/00
Claims (2)
波素子をその中心線を一致させて所定間隔で対向配置
し、前記一方の超音波素子の発信部から発信した超音波
が前記他方の超音波素子の受信部で受信されるまでの時
間を測定するとともに、この状態で前記一対の超音波素
子間に基準物体を配置して、前記各発信部から発信した
超音波が前記基準物体の表裏面でそれぞれ反射されて各
受信部で受信されるまでの各時間を測定する基準値設定
工程と、再度、前記一方の超音波素子の発信部から発信
した超音波が前記他方の超音波素子の受信部で受信され
るまでの時間を測定するとともに、この状態で前記一対
の超音波素子間に被測定物を配置して、前記各発信部か
ら発信した超音波が前記被測定物の表裏面でそれぞれ反
射されて各受信部で受信されるまでの各時間を測定する
測定工程と、前記基準値設定工程と前記測定工程とでそ
れぞれ測定された各測定値および前記基準物体の厚さデ
ータを演算部で演算処理することにより前記被測定物の
厚さを算出するデータ処理工程と、からなる厚さ測定方
法。1. A pair of ultrasonic elements having a transmitting part and a receiving part are arranged facing each other at predetermined intervals with their center lines coincident with each other, and the ultrasonic wave transmitted from the transmitting part of said one ultrasonic element is transmitted to said other ultrasonic element. While measuring the time until it is received by the receiving unit of the ultrasonic element, the reference object is arranged between the pair of ultrasonic elements in this state, and the ultrasonic waves transmitted from each of the transmitting units are the ultrasonic waves of the reference object. A reference value setting step of measuring each time until each of the ultrasonic elements is reflected by the front and back surfaces and received by each of the receiving units, and again, the ultrasonic wave transmitted from the transmitting unit of the one ultrasonic element is the other ultrasonic element. While measuring the time until it is received by the receiving unit, an object to be measured is arranged between the pair of ultrasonic elements in this state, and the ultrasonic waves transmitted from each of the transmitting units are displayed on the surface of the object to be measured. The light is reflected by the back side and received by each receiver. The measurement step of measuring each time until it is transmitted, and the reference value setting step and the measurement data measured in the measurement step and the thickness data of the reference object are processed by a calculation unit in the calculation unit. A data processing step of calculating the thickness of the object to be measured.
の中心線が一致して所定間隔で対向配置され、かつこれ
らの間に基準物体もしくは被測定物が配置される一対の
超音波素子と、前記一対の超音波素子と対応して設けら
れ、前記各発信部から発信する超音波の振幅が次第に大
きくなって一定振幅となるようにするための駆動信号を
複数発の発信パルスに基づいて出力するとともに、前記
超音波の振幅が急変する特定点における前記発信パルス
をスタート信号として出力する一対の発信回路部と、前
記一対の超音波素子と対応して設けられ、前記各受信部
で受信した超音波の波形を処理してその振幅が急変する
特定点における整形パルスをストップ信号として出力す
る一対の受信回路部と、前記一対の超音波素子と対応し
て設けられ、前記各発信回路部からのスタート信号と前
記各受信回路部からのストップ信号とが入力するまでの
時間を超音波の発信周波数のn倍の周波数をもつクロッ
クでカウントして検出する一対のカウンタ部と、前記一
対の超音波素子間に前記基準物体もしくは前記被測定物
が配置されていない状態で前記各カウンタ部で検出され
た時間、および前記一対の超音波素子間に前記基準物体
もしくは前記被測定物が配置されているそれぞれの状態
で前記各カウンタ部で検出された時間、並びに前記基準
物体の厚さデータを演算処理することにより前記被測定
物の厚さを算出する演算部と、を備えたことを特徴とす
る厚さ測定装置。2. A pair of ultrasonic elements each having a transmitting section and a receiving section, which are arranged opposite to each other at predetermined intervals so that their center lines coincide with each other, and between which a reference object or an object to be measured is arranged. Based on a plurality of transmission pulses, a drive signal is provided corresponding to the pair of ultrasonic elements, so that the amplitude of the ultrasonic waves transmitted from each of the transmission units gradually increases and becomes a constant amplitude. A pair of transmitting circuit units that output and output the transmitting pulse as a start signal at a specific point where the amplitude of the ultrasonic wave suddenly changes, and are provided corresponding to the pair of ultrasonic elements and received by the receiving units. A pair of receiving circuit units that process the waveform of the ultrasound waves and output a shaped pulse at a specific point where the amplitude changes suddenly as a stop signal, and are provided in correspondence with the pair of ultrasound elements, A pair of counter units for counting and detecting the time until the start signal from the transmission circuit unit and the stop signal from each of the reception circuit units are input with a clock having a frequency n times the transmission frequency of the ultrasonic wave, The time detected by each counter unit in a state where the reference object or the device under test is not arranged between the pair of ultrasonic elements, and the reference object or the device under test between the pair of ultrasonic devices. A calculation unit for calculating the thickness of the object to be measured by performing arithmetic processing on the time detected by each of the counter units in each state where the arrangement is arranged, and the thickness data of the reference object. A thickness measuring device, characterized in that:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10355091A JP2944002B2 (en) | 1991-04-10 | 1991-04-10 | Method and apparatus for measuring thickness |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10355091A JP2944002B2 (en) | 1991-04-10 | 1991-04-10 | Method and apparatus for measuring thickness |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04313010A JPH04313010A (en) | 1992-11-05 |
| JP2944002B2 true JP2944002B2 (en) | 1999-08-30 |
Family
ID=14356935
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10355091A Expired - Fee Related JP2944002B2 (en) | 1991-04-10 | 1991-04-10 | Method and apparatus for measuring thickness |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2944002B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5341567B2 (en) * | 2009-03-05 | 2013-11-13 | トヨタ自動車株式会社 | Inspection device |
| JP6022895B2 (en) * | 2012-10-29 | 2016-11-09 | トヨタ自動車株式会社 | Ultrasonic measurement method and ultrasonic measurement apparatus |
| KR102645311B1 (en) * | 2018-08-13 | 2024-03-08 | 삼성디스플레이 주식회사 | Apparatus for measuring sample thickness and method for measuring sample thickness |
| CN114440808A (en) * | 2022-02-24 | 2022-05-06 | 广东奥迪威传感科技股份有限公司 | Ultrasonic thickness measurement method and device |
-
1991
- 1991-04-10 JP JP10355091A patent/JP2944002B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04313010A (en) | 1992-11-05 |
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