JPS60105907A - Ultrasonic thickness meter - Google Patents

Ultrasonic thickness meter

Info

Publication number
JPS60105907A
JPS60105907A JP21313183A JP21313183A JPS60105907A JP S60105907 A JPS60105907 A JP S60105907A JP 21313183 A JP21313183 A JP 21313183A JP 21313183 A JP21313183 A JP 21313183A JP S60105907 A JPS60105907 A JP S60105907A
Authority
JP
Japan
Prior art keywords
reflected wave
power
thickness
measured
surface reflected
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
Application number
JP21313183A
Other languages
Japanese (ja)
Inventor
Koji Takinami
滝波 孝治
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.)
Omron Corp
Original Assignee
Tateisi Electronics Co
Omron Tateisi Electronics Co
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 Tateisi Electronics Co, Omron Tateisi Electronics Co filed Critical Tateisi Electronics Co
Priority to JP21313183A priority Critical patent/JPS60105907A/en
Publication of JPS60105907A publication Critical patent/JPS60105907A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B17/00Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations
    • G01B17/02Measuring arrangements characterised by the use of infrasonic, sonic or ultrasonic vibrations for measuring thickness

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Abstract

PURPOSE:To enable the measurement of a thin article to be measured, by emitting ultrasonic waves having different frequencies while respectively detecting reflected waves from the surface and bottom surface of the article to be measured by first and second detectors and operating both detection values on the basis of a specific formula to calculate a thickness. CONSTITUTION:Ultrasonic waves having frequencies f1, f2 are successively emitted from a probe 1 under the control of CPU 7 and a surface reflected wave is detected by a first power detector 2 while a bottom surface reflected wave is detected by a second power detector 9 and both detection values are subjected to A/D conversion to be stored in memory 8. On the other hand, alpha (the ratio of surface reflected wave power with frequency f1 and bottom surface reflected wave power) and beta (the ratio of surface reflected wave power with frequency f2 and bottom surface reflected wave power) are substituted for formulae I , II to calculate acoustic impedance rhoc and a thickness (d). Subsequently, the thickness (d) is displayed by a display part 6.

Description

【発明の詳細な説明】 [発明の技術分野〕 この発明は超音波厚さ計に関する。[Detailed description of the invention] [Technical field of invention] This invention relates to an ultrasonic thickness gauge.

[従来技術および欠点] 従来の超音波厚さ計は単一の周波数のパルス状の超音波
のエコ一時間を測定する構成となっている。従って高い
分解能を得るには数Mllzから数十Mtlzの高い周
波数の超音波パルスを発射できる手段と、高速なカウン
タを有する必要があり、薄い被測定物の厚さを測定しに
くいという欠点がある。
[Prior Art and Disadvantages] A conventional ultrasonic thickness gauge is configured to measure the echo time of pulsed ultrasonic waves of a single frequency. Therefore, in order to obtain high resolution, it is necessary to have a means that can emit ultrasonic pulses with a high frequency of several Mllz to several tens of Mtlz and a high-speed counter, which has the disadvantage that it is difficult to measure the thickness of thin objects to be measured. .

[発明の目的コ それ故、この発明の目的は、異なる周波数の超音波を、
2つまたは複数使用し、薄い被測定物の厚さを測定でき
る超音波厚さ訂を提供することにある。
[Purpose of the Invention Therefore, the purpose of the invention is to transmit ultrasonic waves of different frequencies to
An object of the present invention is to provide an ultrasonic thickness measuring device that can measure the thickness of a thin object by using two or more.

[発明の構成および効果] この発明は、異なる周波数のビーム状の超音波を使い、
その超音波が被検出物の表面および底面で反射された後
、該反射波のパワーをそれぞれ記憶しておき、演算手段
によって記憶されているパワーにもとづいて被測定物の
厚さを測定するようにしたので、高い周波数の超音波を
発生する素子や、高速な時間を計測する素子を用いずと
も薄い被測定物の厚さを測定でき、低価格で簡単な構成
の超音波厚さ計を提供することができる。
[Configuration and effects of the invention] This invention uses beam-shaped ultrasound waves of different frequencies,
After the ultrasonic waves are reflected by the surface and bottom of the object, the power of each reflected wave is memorized, and the thickness of the object is measured based on the stored power by the calculation means. This makes it possible to measure the thickness of a thin object without using an element that generates high-frequency ultrasonic waves or an element that measures high-speed time. can be provided.

(実施例の説明] 以下この発明の一実施例を図面を用いて説明する。(Explanation of Examples) An embodiment of the present invention will be described below with reference to the drawings.

第1図は本発明の超音波厚さ削のブロックタイアゲラム
である。1は探触子であり、2と9はパワー検出部であ
り、3は送信部、4はA/D変換変換コント−ロールっ
て異なる周波数の超音波を発生づることかできるしのと
りる。い、1探触子1が被測定物に垂直に取付番プられ
ているものとする。
FIG. 1 shows a block tiagelum which has been subjected to ultrasonic thickness cutting according to the present invention. 1 is a probe, 2 and 9 are power detectors, 3 is a transmitter, and 4 is an A/D conversion control that can generate ultrasonic waves of different frequencies. . Assume that 1 probe 1 is mounted perpendicularly to the object to be measured.

(被測定物に触れる探触子の音響インピーダンスは予め
測定して分っているものとする。、)超音波発生部5は
CPU7の命令によって周波数f1の超音波を探触7−
1より発射し、第1のパワー検出部2はただちに表面か
らの反射波のパワーを検出する。検出されたパワーはA
/D変換器4でA/D変換されCPU7を介してメモリ
8に一旦記憶される。次に第2のパワー検出部9は被測
定物の底面で反射して被測定物を透過してやってくる透
過波パワーを検出する。さらにこのパワーもA/D変換
器4でA/D変換され、メモリ8に記憶される。さらに
異なる周波数のf、の超音波に対しても同様な動作を行
う。この結果法の式(1)、(2)が得られる。
(It is assumed that the acoustic impedance of the probe that touches the object to be measured is measured and known in advance.) The ultrasonic generator 5 transmits ultrasonic waves of frequency f1 to the probe 7- in accordance with the instructions of the CPU 7.
1, and the first power detection unit 2 immediately detects the power of the reflected wave from the surface. The detected power is A
The signal is A/D converted by the /D converter 4 and temporarily stored in the memory 8 via the CPU 7. Next, the second power detection section 9 detects the transmitted wave power that is reflected from the bottom surface of the object to be measured and transmitted through the object to be measured. Furthermore, this power is also A/D converted by the A/D converter 4 and stored in the memory 8. The same operation is performed for ultrasonic waves of a further different frequency f. As a result, equations (1) and (2) are obtained.

F=(ρc、d、f1)−α・G(ρc、d、fl)・
・・(1)F = <oc 、d、f2)= β・G 
(、QC、d、f2)・t2)ここでEおよびGは予め
理論的に分っている関数であり、ρCは被測定物質の音
響インピーダンス、dは被測定物体の厚さ、flおよび
f2は超音波の周波数、αは周波数で1の超音波が被測
定物体の表面で反射された表面反射波のパワーと底面で
反射された底面反射波のパワーの比であり、βは同様に
周波数f2の超音波の表面反射波と底面反射波との比で
ある。
F=(ρc, d, f1)-α・G(ρc, d, fl)・
...(1) F = <oc, d, f2) = β・G
(, QC, d, f2)・t2) Here, E and G are functions that are known theoretically in advance, ρC is the acoustic impedance of the measured object, d is the thickness of the measured object, fl and f2 is the frequency of the ultrasonic wave, α is the ratio of the power of the surface reflected wave when an ultrasonic wave with a frequency of 1 is reflected from the surface of the object to be measured, and the power of the bottom reflected wave when reflected from the bottom surface, and β is the frequency This is the ratio between the surface reflected wave and the bottom reflected wave of the f2 ultrasonic wave.

上記(1)式および(2)式を連立方程式として解けば
、岳費インピーダンスρGと厚さdとをめることができ
る。そして請求められた厚さdを表示部6に表示する。
By solving equations (1) and (2) above as simultaneous equations, it is possible to determine the impedance ρG and the thickness d. The requested thickness d is then displayed on the display section 6.

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

第1図は本発明の一実施例である超音波厚さ計のブロッ
クタイアゲラムである。 1・・・探触子、2・・・第1のパワー検出部、4・・
・A/D変換器、5・・・超音波発生部、7・・・CP
tJ、8・・・メモリ、9・・・第2のパワー検出部。 R訂出願人 立石電機株式会社
FIG. 1 shows a block tie gellum of an ultrasonic thickness gauge which is an embodiment of the present invention. 1... Probe, 2... First power detection section, 4...
・A/D converter, 5... Ultrasonic generator, 7... CP
tJ, 8...Memory, 9...Second power detection section. R revision applicant Tateishi Electric Co., Ltd.

Claims (1)

【特許請求の範囲】 箕なる周波数のビーム状の超音波を発射する手段と、 この超音波発射手段により発射された超音波が被測定物
の表面で反則した反射波のパワーを検出する第1のパワ
ー検出部と、 前記iIA音波が被測定物の底面で反射した反則波のパ
ワーを検出り−る第2のパワー検出部と、前記第1、第
2のパワー検出部出ノJを△/D変換するΔ/D変換T
段と、 とのΔ/D変換器出ノ〕を記憶するメモリと、このメL
りに記憶された異なる周波数にもとづ(第1のパワー検
出部のパワー検出値と第2のパワー検出部のパワー検出
値とを予め定められた式にもとづいて演算する演算手段
とを備え被測定物の厚さをめることを特徴とする超音波
戸さ旧。
[Scope of Claims] A means for emitting beam-shaped ultrasonic waves with a low frequency; a second power detecting section that detects the power of the repulsive wave that the iIA sound wave reflects on the bottom surface of the object to be measured; /D conversion Δ/D conversion T
A memory for storing the Δ/D converter outputs of stages and
a calculation means for calculating the power detection value of the first power detection section and the power detection value of the second power detection section based on a predetermined formula based on the different frequencies stored in the first power detection section; An old ultrasonic door that is characterized by measuring the thickness of the object to be measured.
JP21313183A 1983-11-11 1983-11-11 Ultrasonic thickness meter Pending JPS60105907A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21313183A JPS60105907A (en) 1983-11-11 1983-11-11 Ultrasonic thickness meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21313183A JPS60105907A (en) 1983-11-11 1983-11-11 Ultrasonic thickness meter

Publications (1)

Publication Number Publication Date
JPS60105907A true JPS60105907A (en) 1985-06-11

Family

ID=16634084

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21313183A Pending JPS60105907A (en) 1983-11-11 1983-11-11 Ultrasonic thickness meter

Country Status (1)

Country Link
JP (1) JPS60105907A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101806590A (en) * 2010-03-25 2010-08-18 南京卓实电气有限责任公司 Method for using higher standing wave resonance for quantitatively detecting thickness of elastic plates

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101806590A (en) * 2010-03-25 2010-08-18 南京卓实电气有限责任公司 Method for using higher standing wave resonance for quantitatively detecting thickness of elastic plates

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