JPS6140932B2 - - Google Patents
Info
- Publication number
- JPS6140932B2 JPS6140932B2 JP7169180A JP7169180A JPS6140932B2 JP S6140932 B2 JPS6140932 B2 JP S6140932B2 JP 7169180 A JP7169180 A JP 7169180A JP 7169180 A JP7169180 A JP 7169180A JP S6140932 B2 JPS6140932 B2 JP S6140932B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- temperature
- circuit
- sample
- output
- 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
- 238000001514 detection method Methods 0.000 claims description 42
- 238000012937 correction Methods 0.000 claims description 13
- 238000012360 testing method Methods 0.000 claims description 11
- 230000005855 radiation Effects 0.000 claims description 4
- 239000000284 extract Substances 0.000 claims 1
- 238000009826 distribution Methods 0.000 description 15
- 230000001360 synchronised effect Effects 0.000 description 12
- 238000005259 measurement Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 230000003287 optical effect Effects 0.000 description 3
- 238000002474 experimental method Methods 0.000 description 2
- 230000020169 heat generation Effects 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 230000003252 repetitive effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress, in general
- G01L1/24—Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
- G01L1/248—Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet using infrared
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)
Description
【発明の詳細な説明】
本発明は被検試料に加わる応力値又は応力分布
を短時間で正確に取得することのできる新規な応
力測定装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a novel stress measuring device that can accurately obtain stress values or stress distributions applied to a test sample in a short time.
機械部品等を作成するにあたつては荷重による
応力が特定部位に集中しない様に注意を払う必要
がある。そこで特に耐久性を重視する用途などで
は実物又は実物に近い模型に実際に荷重を印加
し、各部の応力を測定することが行われている
が、実際の測定は被測定体の各部に多数の歪ゲー
ジを取付け、各ゲージらの出力をモニタするため
大がかりで長時間を要するものとなつていた。 When creating mechanical parts, etc., care must be taken to ensure that stress due to loads does not concentrate on specific parts. Therefore, in applications where durability is particularly important, a load is actually applied to the actual object or a model close to the actual object and the stress in each part is measured. Installing strain gauges and monitoring the output of each gauge was a large-scale and time-consuming process.
本発明はこの点に鑑みてなされたものであり、
荷重変化に基づく温度変化を求めることにより応
力を測定すると共に単一の歪検出素子を被検試料
を取付け、該検出素子からの信号に基づく補正を
行うことにより正確な測定を行うことのできる応
力測定装置を提供することを目的とするものであ
る。以下図面を用いて本発明を詳説する。 The present invention has been made in view of this point,
Stress can be measured accurately by determining the temperature change based on the load change, and by attaching a single strain detection element to the test sample and making corrections based on the signal from the detection element. The purpose of this invention is to provide a measuring device. The present invention will be explained in detail below using the drawings.
被検試料に繰返し圧縮荷重及び引張り荷重を印
加した時の該被検試料表面の温度を測定したとこ
ろ、本発明者は応力の集中する部位では表面温度
が単に上昇するのではなく、荷重印加に同期して
周囲温度(正確には荷重零での試料温度)よりも
上昇する期間と周囲よりも下降する期間とが交互
に繰返されることを見出した。即ち第1図aに示
す様な正弦波形の荷重を試料に印加したところ、
該試料の応力集中部位の表面温度は同図bに示す
様に荷重印加に同期した正弦波形で周囲温度より
も高温になる期間と周囲温度より低温になる期間
とが交互に繰返される結果となつている。 When the temperature of the surface of the test sample was measured when compressive and tensile loads were repeatedly applied to the test sample, the inventor found that the surface temperature did not simply increase in areas where stress was concentrated, but that the surface temperature increased with the application of load. It has been found that periods in which the temperature rises above the ambient temperature (more accurately, the sample temperature at zero load) and periods in which it falls below the ambient temperature are alternately repeated. That is, when a sinusoidal waveform load as shown in Figure 1a was applied to the sample,
As shown in Figure b, the surface temperature of the stress concentration area of the sample has a sinusoidal waveform synchronized with the load application, resulting in alternating periods of higher temperature than the ambient temperature and periods of lower temperature than the ambient temperature. ing.
これは圧縮力が加えられている期間応力集中部
位で発熱作用が現われ、引張り力が加えられてい
る期間は吸熱作用が現われ、この発熱が比較的短
い周期で繰返されるため、周囲への熱の拡散或い
は周囲からの熱の流入が断たれた断熱状態で上記
応力集中部位の表面温度が変化するものである。
このことは例えば第1図cに示す様に圧縮力のみ
を矩形波形で印加すると同図dの様にそれに同期
した矩形波形の温度上昇のみが発生し、同図eの
様に引張り力のみを印加すると同図fの様に温度
低下のみが発生することからも確認された。 This is because heat generation occurs at the stress concentration area during the period when compressive force is applied, and endothermic effect appears during the period when tensile force is applied, and this heat generation is repeated in relatively short cycles, so that heat is not transferred to the surroundings. The surface temperature of the stress concentration area changes in an adiabatic state in which diffusion or inflow of heat from the surroundings is cut off.
For example, if only compressive force is applied in a rectangular waveform as shown in Fig. 1c, only a temperature rise in the rectangular waveform synchronized with it will occur as shown in Fig. 1d, and only a tensile force will be applied as shown in Fig. 1e. This was also confirmed by the fact that only a temperature drop occurred when the voltage was applied, as shown in figure f.
そして諸条件を種々変えて実験を繰返し検討を
重ねた結果、温度変化量と応力変化(正確には応
力による変位量)との間には比例関係があること
が判明した。第2図a,bは実際に実験で求めた
荷重−温度変化及び周囲温度−温度変化の比例関
係を示す図である。 As a result of repeated experiments under various conditions, it was found that there is a proportional relationship between the amount of temperature change and the stress change (more precisely, the amount of displacement due to stress). FIGS. 2a and 2b are diagrams showing the proportional relationships between load and temperature change and between ambient temperature and temperature change, which were actually determined through experiments.
この関係から被測定体に異なつた荷重を順次印
加し、その時の特定部位の表面温度変化巾を検出
すれば該部位にかかつた応力を知ることができ、
しかもその測定部位を徐々に水平走査すればその
走査線に沿つた応力分布を知ることができるし、
加えて該走査線位置を徐々に垂直方向に移動させ
れば走査領域における2次元的な応力分布を測定
することが可能である。 Based on this relationship, by sequentially applying different loads to the object to be measured and detecting the range of surface temperature change of a specific part at that time, it is possible to know the stress applied to that part.
Moreover, by gradually scanning the measurement site horizontally, the stress distribution along the scanning line can be determined.
In addition, by gradually moving the scanning line position in the vertical direction, it is possible to measure the two-dimensional stress distribution in the scanning area.
更に赤外線カメラを用いて異なつた荷重印加時
の被検試料の温度分布像の取得(映像信号の形
で)し、2つの像の差のパターン即ち温度変化の
度合を示すパターンを求めれば、このパターンが
試料各点における温度変化巾を示すものとなり、
応力分布を極めて短時間で取得することができ
る。 Furthermore, by using an infrared camera to obtain temperature distribution images of the test sample under different loads (in the form of video signals) and finding the pattern of the difference between the two images, that is, the pattern that indicates the degree of temperature change, this can be done. The pattern shows the range of temperature change at each point on the sample,
Stress distribution can be obtained in an extremely short time.
本発明はこの様な新規な応力測定装置におい
て、試料上の1点に歪ゲージ等の歪検出素子を取
付け、該検出素子から得られる検出信号に基づい
て上記方法での測定結果を補正することを特徴と
している。第3図は本発明の一実施例の構成を示
し、同図において1は加振機である。該加振機1
は油圧駆動されるピストン2,3と該ピストンの
間に被検試料4を固定するための保持機構5,6
とを備えている。 The present invention provides such a novel stress measuring device, in which a strain detection element such as a strain gauge is attached to one point on a sample, and the measurement results obtained by the above method are corrected based on the detection signal obtained from the detection element. It is characterized by FIG. 3 shows the configuration of an embodiment of the present invention, in which numeral 1 represents a vibrator. The vibration exciter 1
are hydraulically driven pistons 2, 3 and holding mechanisms 5, 6 for fixing the test sample 4 between the pistons.
It is equipped with
7は試料4上の特定点の温度を検出するための
放射温度計であり、該温度計は集束レンズ8、赤
外線検出器9、モータ10によつて回転されるチ
ヨツパ11、検出器9から得られる検出信号を増
巾する増巾器12、検出信号を前記チヨツパ11
によるチヨツピングと同期して検波する同期検波
回路13、該検波回路13からの検波出力が温度
とリニアな関係を持つ温度信号になる様に補正す
るリニアライザ14から構成される。 7 is a radiation thermometer for detecting the temperature of a specific point on the sample 4; an amplifier 12 for amplifying the detected signal;
The detection circuit 13 includes a synchronous detection circuit 13 that performs detection in synchronization with the chopping, and a linearizer 14 that corrects the detection output from the detection circuit 13 so that it becomes a temperature signal having a linear relationship with the temperature.
該リニアライザ14から得られる温度信号はフ
イルタ又はレベルシフト回路等の直流分除去回路
15を介して交流成分のみが取出され、該交流成
分は前記加振機1から発生する荷重印加に同期し
た同期信号16が供給される同期検波回路17へ
送られる。該検波回路17の出力信号はスイツチ
18により演算回路19又は演算回路20へ選択
的に送られる。該演算回路19の他方の入力端子
には前記試料4の所定位置に取付けられた歪ゲー
ジ等の歪検出素子21からの検出信号に基づいて
該所定位置の応力値を求める検出回路22の出力
が供給されている。そして該演算回路19の演算
出力はホールド回路23を介して前記演算回路2
0へ送られる。24,25は該演算回路20の出
力値を表示するためのメータ及び数字表示器であ
る。 Only the AC component of the temperature signal obtained from the linearizer 14 is extracted through a DC component removal circuit 15 such as a filter or a level shift circuit, and the AC component is converted into a synchronous signal synchronized with the load application generated from the vibrator 1. 16 is sent to the synchronous detection circuit 17 to which the signal 16 is supplied. The output signal of the detection circuit 17 is selectively sent to an arithmetic circuit 19 or 20 by a switch 18. The other input terminal of the arithmetic circuit 19 receives the output of a detection circuit 22 that determines the stress value at a predetermined position of the sample 4 based on a detection signal from a strain detection element 21 such as a strain gauge attached to the sample 4. Supplied. The arithmetic output of the arithmetic circuit 19 is transmitted to the arithmetic circuit 2 through a hold circuit 23.
Sent to 0. 24 and 25 are meters and numerical displays for displaying the output values of the arithmetic circuit 20.
上記の如き構成において、被検試料4にはピス
トン2,3によつて第4図aの様に圧縮荷重と引
張り荷重が矩形波形で交互に印加されているとす
ると、試料各部の表面温度は先に述べた如く各部
分に加わてつている圧縮荷重及び引張り荷重に応
じた巾で周囲温度を中心に例えば第4図bに示す
様に変化する。従つて試料上の特定点Pの温度変
化を測定した温度計7の出力も同図bに対応した
波形変化を示し、該出力中の変化分(交流信号)
が除去回路15を介して第4図cの様に取出され
る。そして被検回路17は該交流信号を加振機1
から発生する同期信号(第4図d)に基づいて同
期検波するため、その出力としては第4図eに示
す様に交流信号の振巾に対応した直流信号Apが
得られる。該直流信号は観測点における温度変化
巾即ちその点にかかる応力値に対応したものであ
ることは先に述べた通りである。 In the above configuration, if compressive load and tensile load are applied alternately to the test sample 4 in a rectangular waveform as shown in FIG. 4a by the pistons 2 and 3, the surface temperature of each part of the sample is As mentioned above, the ambient temperature changes as shown in FIG. 4b, for example, with a range corresponding to the compressive load and tensile load applied to each part. Therefore, the output of the thermometer 7 that measured the temperature change at a specific point P on the sample also shows a waveform change corresponding to b in the same figure, and the change in the output (AC signal)
is taken out via the removal circuit 15 as shown in FIG. 4c. Then, the circuit under test 17 transmits the AC signal to the vibrator 1.
Since synchronous detection is performed based on the synchronous signal (Fig. 4 d) generated from the synchronous signal, a DC signal Ap corresponding to the amplitude of the AC signal is obtained as an output, as shown in Fig. 4 e. As mentioned above, the DC signal corresponds to the range of temperature change at the observation point, that is, the stress value applied to that point.
ところがこの直流信号値は応力値が同一でも、
試料の放射率や材質によつて異なり、又回路系の
利得が経時変化、電圧変化等によつて変動すると
それに応じて変化し、誤差が発生してしまう。そ
こで本発明では温度計7による観測点Pと同一場
所にかかる正しい応力値を歪検出素子21及び検
出器22を用いて検出し、得られた検出信号Bp
と温度計7を用いて取得した応力に対応する直流
信号Apとの比即ち補正係数を演算回路19にお
いて求め、得られた係数により他の部位の測定値
を補正するようにしている。 However, even if the stress value is the same for this DC signal value,
It varies depending on the emissivity and material of the sample, and if the gain of the circuit system fluctuates due to changes over time, voltage changes, etc., it changes accordingly, resulting in errors. Therefore, in the present invention, the correct stress value applied to the same place as the observation point P by the thermometer 7 is detected using the strain detection element 21 and the detector 22, and the obtained detection signal Bp
The ratio of the DC signal Ap corresponding to the stress obtained using the thermometer 7, that is, the correction coefficient, is determined in the arithmetic circuit 19, and the measured values of other parts are corrected using the obtained coefficient.
即ち測定に先立つてスイツチ18が演算回路1
9側へ倒されると共に、温度計7の観測点は歪検
出素子21の取付位置又はその極く近傍の位置に
設定される。演算回路19からはスイツチ18を
介して送られる検出信号Apと検出器22を介し
て送られる検出信号Bpとの比K=Bp/Apが求め
られ、該比Kは補正係数としてホールド回路23
によつて保持される。 That is, prior to measurement, the switch 18
9 side, and the observation point of the thermometer 7 is set at the mounting position of the strain detection element 21 or a position very close to it. The arithmetic circuit 19 calculates the ratio K=Bp/Ap between the detection signal Ap sent via the switch 18 and the detection signal Bp sent via the detector 22, and the ratio K is sent to the hold circuit 23 as a correction coefficient.
held by.
そして補正係数が保持された後、スイツチ18
を切換えると共に温度計7の観測点を試料4上の
所望位置へ移動させれば、該所望位置に関する検
出信号Aは演算回路20へ送られ、該演算回路2
0において信号Aに補正係数Kが掛け合わされ
A・Kという正しい測定値が得られる。得られた
正しい測定値はメータ24又は表示器25に送ら
れて表示される。 After the correction coefficient is held, the switch 18
If the observation point of the thermometer 7 is moved to a desired position on the sample 4 at the same time, the detection signal A regarding the desired position is sent to the arithmetic circuit 20;
At 0, the signal A is multiplied by the correction coefficient K to obtain the correct measured value A·K. The correct measurements obtained are sent to the meter 24 or display 25 for display.
この様にして任意の点における応力値が補正さ
れた正しい値として得られるが、温度計7の前面
に2次元又は1次元的な光学的走査機構26を設
け温度計の観測点を徐々に移動走査すると共に、
それに伴なつて演算回路20から得られる測定値
を上記走査と同期した表示装置27へ輝度変調信
号又はY方向変調信号として導入すれば、応力値
に応じた輝度を持つ応力分布像又は応力分布波形
を表示することができることは言うまでもない。 In this way, the stress value at any point can be obtained as a corrected value, but a two-dimensional or one-dimensional optical scanning mechanism 26 is provided in front of the thermometer 7 to gradually move the observation point of the thermometer. Along with scanning,
Along with this, if the measured value obtained from the arithmetic circuit 20 is introduced as a luminance modulation signal or a Y-direction modulation signal to the display device 27 synchronized with the scanning, a stress distribution image or stress distribution waveform having a luminance according to the stress value is generated. Needless to say, it is possible to display
ところで、上述の如く試料表面上の異なつた位
置の点では各点における応力値に応じた巾で温度
変化をしているのであるから、第1図aの様な操
返し荷重が印加されているうちの圧縮荷重の半周
期T1には、試料表面の各点は各点における応力
値に応じた温度上昇(周囲温度からの)を示し、
引張り荷重の半周期T2には各点における応力値
に応じた温度低下(周囲温度からの)を示すはず
である。従つてT1の間に試料表面の温度上昇し
た温度分布像を取得し、T2の間に同一面の温度
低下した温度分布像を取得し、2つの温度分布像
の差のパターンを求めれば、該パターンは試料上
の各点における期間T1の時とT2の時の温度差
即ち応力に応じたものとなり、極めて短時間T1
+T2で応力分布パターンを取得することができ
る。 By the way, as mentioned above, the temperature changes at different positions on the sample surface in a range corresponding to the stress value at each point, so a repetitive load as shown in Figure 1 a is applied. During the half period T1 of the compressive load, each point on the sample surface shows a temperature rise (from the ambient temperature) according to the stress value at each point,
Half period T2 of the tensile load should show a temperature drop (from ambient temperature) depending on the stress value at each point. Therefore, by acquiring a temperature distribution image of the sample surface whose temperature has increased during T1, and acquiring a temperature distribution image of the same surface whose temperature has decreased during T2, and finding the pattern of the difference between the two temperature distribution images, The pattern corresponds to the temperature difference, that is, the stress, between the periods T1 and T2 at each point on the sample.
A stress distribution pattern can be obtained at +T2.
第5図はこの様な考え方に基づく本発明の他の
実施例の構成を示す。同図において28は試料4
から発生する赤外線を走査検出し、該試料の温度
分布像を撮影するための赤外線カメラであり、該
カメラは加振機1から発生する同期信号29に基
づいて間歇的に1画面ずつ撮影を行う。撮影に伴
なつて得られる1画面分のビデオ信号(温度信
号)はA−D変換器30によつてデジタル信号に
変換された後、前記同期信号29に基づいて切換
えられるスイツチ31により書込制御回路32又
は引算回路33へ選択的に供給される。該書込制
御回路は供給された1画面分の温度信号を前記カ
メラ28の走査同期信号34に基づいてメモリ3
5へ格納する。 FIG. 5 shows the configuration of another embodiment of the present invention based on this idea. In the same figure, 28 is sample 4.
This is an infrared camera that scans and detects the infrared rays generated from the sample and photographs the temperature distribution image of the sample, and the camera intermittently photographs one screen at a time based on the synchronization signal 29 generated from the vibrator 1. . A video signal (temperature signal) for one screen obtained in conjunction with photographing is converted into a digital signal by an A-D converter 30, and then write control is performed by a switch 31 that is switched based on the synchronization signal 29. It is selectively supplied to the circuit 32 or the subtraction circuit 33. The write control circuit writes the supplied temperature signal for one screen into the memory 3 based on the scan synchronization signal 34 of the camera 28.
Store in 5.
そして格納された温度信号は次の1画面撮影の
際走査同期信号34に基づいて作動する読出し制
御回路36によつて読出されて引算回路33へ送
られると共にレベル判別回路38に送られる。該
引算回路33の出力信号はスイツチ37を介して
レベル判別回路38からの指令パルスに基づいて
作動するサンプルホールド回路39、又は演算回
路40へ選択的に供給される。 The stored temperature signal is then read out by a readout control circuit 36 which operates based on the scan synchronization signal 34 when photographing the next one screen, and sent to the subtraction circuit 33 and also to the level determination circuit 38. The output signal of the subtraction circuit 33 is selectively supplied via a switch 37 to a sample and hold circuit 39 operated based on a command pulse from a level discrimination circuit 38 or to an arithmetic circuit 40.
41は該サンプルホールド回路39の出力Aと
A−D変換器42を介して送られる検出回路22
からの検出信号Bの比を求める演算回路であり、
該演算回路41の出力はホールド回路42を介し
て前記演算回路40へ送られる。そして該演算回
路40の出力は前記走査同期信号34に基づいて
作動する陰極線管(CRT)表示装置45へD−
A変換器44を介して輝度変調信号として供給さ
れる。 41 is a detection circuit 22 that sends the output A of the sample hold circuit 39 and the A-D converter 42.
It is an arithmetic circuit that calculates the ratio of the detection signal B from the
The output of the arithmetic circuit 41 is sent to the arithmetic circuit 40 via a hold circuit 42. The output of the arithmetic circuit 40 is sent to a cathode ray tube (CRT) display device 45 which operates based on the scan synchronization signal 34.
It is supplied via the A converter 44 as a brightness modulation signal.
上述の如き構成において、加振機1は試料4に
例えば第6図aに示す様な矩形波形の荷重を2秒
の繰返し周期で印加するものとする。該加振機1
からは荷重印加に同期した同期信号29(第6図
b)が発生し、該同期信号29に基づいてカメラ
28は第6図cに示す様なタイミングで圧縮荷重
期間T1及び引張り荷重期間T2内に1回ずつ1
画面走査を行う。 In the configuration as described above, the vibrator 1 applies a rectangular waveform load as shown in FIG. 6a, for example, to the sample 4 at a repetition period of 2 seconds. The vibration exciter 1
A synchronization signal 29 (Fig. 6b) synchronized with the load application is generated, and based on the synchronization signal 29, the camera 28 detects the timing within the compressive load period T1 and the tensile load period T2 at the timing shown in Fig. 6c. 1 time each
Perform screen scanning.
この時スイツチ31は第6図dに示す様に荷重
印加に同期して切換えられるため、T1における
1画面走査に伴なつて得られる温度信号Z1は書
込み制御回路32を介して一旦メモリ35へ記憶
され、T2における1画面走査に伴なつて得られ
る温度信号Z2は引算回路33へ送られる。この
T2の期間読出し制御回路36はカメラ28によ
る1画面走査と同期してT1の期間に得られた温
度信号Z1を読出し、引算回路33へ送るため、
該引算回路33の出力としてはZ1とZ2の差信
号が得られる。即ちT1の期間の温度とT2の期
間の温度との温度差(温度変化)に対応する差信
号が1画面を構成する各画素毎に得られることに
なる。この温度差信号が各画素に対応する試料上
の微小点にかかる応力を示していることは先に述
べた通りであり、該信号をCRT表示装置45へ
送れば応力に応じた輝度が与えられた応力分布像
が得られることになる。 At this time, the switch 31 is switched in synchronization with the load application as shown in FIG. The temperature signal Z2 obtained with one screen scan at T2 is sent to the subtraction circuit 33. The T2 period readout control circuit 36 reads the temperature signal Z1 obtained during the T1 period in synchronization with one screen scan by the camera 28 and sends it to the subtraction circuit 33.
As the output of the subtraction circuit 33, a difference signal between Z1 and Z2 is obtained. That is, a difference signal corresponding to the temperature difference (temperature change) between the temperature during the period T1 and the temperature during the period T2 is obtained for each pixel forming one screen. As mentioned above, this temperature difference signal indicates the stress applied to the minute point on the sample corresponding to each pixel, and if this signal is sent to the CRT display device 45, the brightness will be given according to the stress. A stress distribution image can be obtained.
ところがこの差信号も歪値が同一でも被写体の
放射率、材質によつて異つた値を示し、又回路系
の利得が経時変化、電圧変化等によつて変動する
とそれに応じて変化し、誤差が発生してしまう。
そこで本実施例では赤外線カメラ28の視野内の
試料上に歪検出素子21を取付け、該素子21及
び検出回路22により取付け場所における正しい
応力値を検出し、得られた検出信号Bと赤外線カ
メラ28を用いて取得した上記取付け場所の応力
に対応する信号Aとの比即ち補正係数を求め、得
られた補正係数により他の部位の測定値を補正す
るようにしている。 However, even if the distortion value is the same, this difference signal will show a different value depending on the emissivity of the subject and the material, and if the gain of the circuit changes due to changes over time or voltage changes, it will change accordingly, causing an error. It will happen.
Therefore, in this embodiment, the strain detection element 21 is mounted on the sample within the field of view of the infrared camera 28, and the correct stress value at the mounting location is detected by the element 21 and the detection circuit 22, and the obtained detection signal B and the infrared camera 28 The ratio of the stress to the signal A corresponding to the stress at the installation location obtained using the above method, that is, the correction coefficient, is determined, and the measured values of other parts are corrected using the obtained correction coefficient.
即ち歪検出素子21の外側表面は例えば鏡面仕
上等が施され放射率が周囲に比べ極端に小さく、
殆んど零にされており、そのためZ1,Z2とも
該歪検出素子21の表面を走査している期間は信
号レベルがその前後に比べ極端に低下し、その結
果読出し制御回路36の出力信号もその期間信号
レベルが極端に低下したものとなる。そこで荷重
印加の最初の1周期の間スイツチ37を接点a側
に倒し、その期間に得られる読出し制御回路36
の出力信号のレベルを判別回路38で監視し、信
号レベルが極端に低下する期間(換言すれば歪検
出素子を検出している期間)の直前又は直後のタ
イミングで該判別回路38からの指令パルスを発
生させ、その信号レベルが極端に低下する期間の
直前又は直後の引算回路33の出力信号をホール
ド回路39においてサンプルホールドすれば、該
サンプルホールドされた出力信号値Aは歪検出素
子21の極く近傍即ち実質的に該素子の取付け位
置の応力値に対応したものとなる。 That is, the outer surface of the strain detection element 21 is given a mirror finish, for example, and has an extremely low emissivity compared to the surrounding area.
Therefore, during the period when the surface of the strain detection element 21 is being scanned for both Z1 and Z2, the signal level is extremely lower than before and after that, and as a result, the output signal of the readout control circuit 36 is also During that period, the signal level becomes extremely low. Therefore, the switch 37 is turned to the contact a side during the first cycle of load application, and the readout control circuit 36 obtained during that period is
The level of the output signal is monitored by the discrimination circuit 38, and a command pulse from the discrimination circuit 38 is issued at a timing immediately before or after a period in which the signal level is extremely reduced (in other words, a period in which the distortion detection element is being detected). If the output signal of the subtraction circuit 33 is sampled and held in the hold circuit 39 immediately before or immediately after the period in which the signal level drops extremely, the sampled and held output signal value A will be the output signal of the distortion detection element 21. The stress value corresponds to the stress value in the very vicinity, that is, substantially at the mounting position of the element.
そして演算回路41からは上記取付け位置の応
力値の正しい測定値Bと、赤外線カメラ28によ
る測定値Aとの比K=B/Aが求められ、該比K
は補正係数としてホールド回路43によつてホー
ルドされる。 Then, the calculation circuit 41 calculates the ratio K=B/A between the correct measurement value B of the stress value at the mounting position and the measurement value A obtained by the infrared camera 28, and the ratio K
is held by the hold circuit 43 as a correction coefficient.
この様にして補正係数が保持された後、第6図
eに示す様に荷重印加の2番目の周期からスイツ
チ37を接点b側へ切換えると、引算回路33の
出力信号は演算回路40へ送られ、該演算回路4
0において該出力信号に補正係数Kが掛け合わさ
れた正しい信号が得られる。該信号はD−A変換
器44を介してCRT表示装置45へ輝度信号と
して送られるため、該表示装置の画面には補正に
より正しい輝度が与えられた応力分布像が得られ
ることになる。表示方法としては上記の様な輝度
変調法だけではなく、例えば輝度信号を一定と
し、前記演算回路40の出力信号をCRTの垂直
方向偏向信号に重畳させる所謂偏向変調法を用い
ても良いし、他の表示方法を用いても良いことは
言うまでもない。 After the correction coefficient is held in this way, when the switch 37 is switched to the contact b side from the second cycle of load application as shown in FIG. and the arithmetic circuit 4
0, a correct signal is obtained by multiplying the output signal by the correction coefficient K. Since this signal is sent as a luminance signal to the CRT display device 45 via the DA converter 44, a stress distribution image with correct luminance given by correction is obtained on the screen of the display device. As a display method, in addition to the above-mentioned brightness modulation method, for example, a so-called deflection modulation method may be used in which the brightness signal is kept constant and the output signal of the arithmetic circuit 40 is superimposed on the vertical direction deflection signal of the CRT. It goes without saying that other display methods may be used.
尚印加荷重の波形も上記例の様に矩形波形に限
らず正弦波形でも良いし、又荷重の方向も第1図
c又はeの様に圧縮方向又は引張方向のみ印加す
る様にしても良く、更には一定荷重に変動分が重
畳された様なものでも良い。 The waveform of the applied load is not limited to the rectangular waveform as in the above example, but may be a sine waveform, and the direction of the load may also be applied only in the compression or tension direction as shown in Figure 1c or e. Furthermore, it may be such that a variation is superimposed on a constant load.
又赤外線カメラとしては光学的走査を行うもの
でも、赤外線ビジコンの様に電子的走査を行うも
のでもよい。 The infrared camera may be one that performs optical scanning or one that performs electronic scanning such as an infrared vidicon.
更に又、上記実施例は加振器による加重印加が
一定振幅で行われる場合であつたが、振幅が変化
する場合は歪検出素子による測定点以外の補正係
数をその振幅変化に応じて変化させるようにすれ
ば良い。 Furthermore, in the above embodiment, the weight application by the vibrator is performed with a constant amplitude, but when the amplitude changes, the correction coefficients other than the measurement points by the strain detection element are changed in accordance with the change in amplitude. Just do it like this.
以上詳述した如く本発明によれば従来に比べ桁
違いに短い時間で、補正された精密な応力分布像
を得ることができる。 As described in detail above, according to the present invention, a corrected and precise stress distribution image can be obtained in an order of magnitude shorter time than conventional methods.
第1図は本発明の原理を説明するための波形
図、第2図は荷重と温度変化及び周囲温度と温度
変化の関係を示す図、第3図及び第5図は本発明
の一実施例の構成を示す図、第4図及び第6図は
その動作を説明するための波形図である。
1:加振機、4:被検試料、7:放射温度計、
15:直流分除去回路、17:同期検波回路、1
8,31,37:スイツチ、19,20,40,
41:演算回路、21:歪検出素子、22:検出
回路、23,43:ホールド回路、24:メー
タ、25:表示器、26:光学的走査手段、2
7,45:CRT表示装置、28:赤外線カメ
ラ、30,42:A−D変換器、32:書込み制
御回路、33:引算回路、35:メモリ、36:
読出し制御回路、38:レベル判別回路、39:
サンプルホールド回路、44:D−A変換器。
Fig. 1 is a waveform diagram for explaining the principle of the present invention, Fig. 2 is a diagram showing the relationship between load and temperature change, and ambient temperature and temperature change, Fig. 3 and Fig. 5 are one embodiment of the present invention. 4 and 6 are waveform diagrams for explaining the operation. 1: Vibrator, 4: Test sample, 7: Radiation thermometer,
15: DC component removal circuit, 17: Synchronous detection circuit, 1
8, 31, 37: Switch, 19, 20, 40,
41: Arithmetic circuit, 21: Strain detection element, 22: Detection circuit, 23, 43: Hold circuit, 24: Meter, 25: Display, 26: Optical scanning means, 2
7, 45: CRT display device, 28: Infrared camera, 30, 42: A-D converter, 32: Write control circuit, 33: Subtraction circuit, 35: Memory, 36:
Read control circuit, 38: Level discrimination circuit, 39:
Sample and hold circuit, 44: DA converter.
Claims (1)
発生する赤外線に基づき荷重変化に同期した試料
における温度変化を検出する手段と、上記試料に
取付けられた歪検出素子と、該検出素子の出力と
該検出素子の取付位置と同一位置に関する前記温
度変化検出手段の出力との比を求める演算手段
と、該比の値に基づいて前記温度変化検出手段の
出力を補正する手段と、該補正手段の出力が供給
される表示又は記録手段とを備えたことを特徴と
する応力測定装置。 2 前記温度変化検出手段は試料温度を測定する
放射温度計と、該放射温度計の出力信号から交流
信号を取出す回路と、該交流信号の振巾を検出す
る回路とから構成される特許請求の範囲第1項記
載の応力測定装置。 3 前記温度変化検出手段は2種の異なつた荷重
が順次印加される被検試料を撮影するための赤外
線カメラと、一方の荷重印加時に該赤外線カメラ
から得られる1画面分の温度信号を記憶する記憶
手段と、他方の荷重印加時に前記赤外線カメラか
ら得られる1画面分の温度信号と前記記憶手段に
記憶されている温度信号との差を求める引算回路
とから構成される特許請求の範囲第1項記載の応
力測定装置。 4 前記異なつた荷重の一方は圧縮荷重であり他
方は引張荷重である特許請求の範囲第1項乃至第
3項のいずれかに記載の応力測定装置。 5 前記異なつた荷重のうち一方は零である特許
請求の範囲第1項乃至第3項のいずれかに記載の
応力測定装置。[Scope of Claims] 1. A means for detecting temperature changes in a sample in synchronization with load changes based on infrared rays generated from a test sample to which different loads are sequentially applied, and a strain detection element attached to the sample; Calculating means for calculating the ratio between the output of the detection element and the output of the temperature change detection means at the same position as the mounting position of the detection element, and means for correcting the output of the temperature change detection means based on the value of the ratio. and display or recording means to which the output of the correction means is supplied. 2. The temperature change detection means comprises a radiation thermometer that measures the sample temperature, a circuit that extracts an AC signal from the output signal of the radiation thermometer, and a circuit that detects the amplitude of the AC signal. The stress measuring device according to scope 1. 3. The temperature change detection means stores an infrared camera for photographing the test sample to which two different loads are sequentially applied, and one screen worth of temperature signals obtained from the infrared camera when one of the loads is applied. Claim 1, which comprises a storage means, and a subtraction circuit that calculates the difference between the temperature signal for one screen obtained from the infrared camera when the other load is applied and the temperature signal stored in the storage means. The stress measuring device according to item 1. 4. The stress measuring device according to any one of claims 1 to 3, wherein one of the different loads is a compressive load and the other is a tensile load. 5. The stress measuring device according to any one of claims 1 to 3, wherein one of the different loads is zero.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7169180A JPS56168141A (en) | 1980-05-29 | 1980-05-29 | Stress measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7169180A JPS56168141A (en) | 1980-05-29 | 1980-05-29 | Stress measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56168141A JPS56168141A (en) | 1981-12-24 |
| JPS6140932B2 true JPS6140932B2 (en) | 1986-09-11 |
Family
ID=13467818
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7169180A Granted JPS56168141A (en) | 1980-05-29 | 1980-05-29 | Stress measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56168141A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP4610955B2 (en) * | 2004-07-15 | 2011-01-12 | ▲隆▼英 阪上 | Method and apparatus for measuring thermal influence due to plastic deformation |
| JP6142074B2 (en) * | 2014-03-19 | 2017-06-07 | 株式会社日立製作所 | Fatigue testing equipment |
-
1980
- 1980-05-29 JP JP7169180A patent/JPS56168141A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56168141A (en) | 1981-12-24 |
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