CN101975555B - A strain measurement method and device based on light transmission measurement technology - Google Patents

A strain measurement method and device based on light transmission measurement technology Download PDF

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CN101975555B
CN101975555B CN2010102914964A CN201010291496A CN101975555B CN 101975555 B CN101975555 B CN 101975555B CN 2010102914964 A CN2010102914964 A CN 2010102914964A CN 201010291496 A CN201010291496 A CN 201010291496A CN 101975555 B CN101975555 B CN 101975555B
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test section
strain
specimen test
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rigidity
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姚磊江
郑翔
童小燕
曾垂宽
赵凯
胡国镇
魏佩佳
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Northwestern Polytechnical University
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Abstract

本发明提出一种基于光透过测量技术的应变测量方法及其装置,其方法特征在于:在试样试验段两侧固定两根相互平行的刚性引针,刚性引针与试样试验段拉伸方向的中心轴线垂直,刚性引针长度大于试样试验段的宽度,采用光透式数字测微计测量两根刚性引针间的初始距离,拉伸过程中的实时距离和拉伸结束后的最终距离,计算得到试样试验段的实时应变和最终应变,其中测微计的测量位置位于试样试验段两侧,且与试样试验段拉伸方向中心轴线的距离相等。本发明通过光透过测量技术测量刚性引针在拉伸过程中的距离变化,实现了对小试验面积材料、柔性材料和大形变情况应变的快速方便测量。克服了现有测量方法的缺陷,较好地弥补了几种方法应用的盲区。

The present invention proposes a strain measurement method and device based on light transmission measurement technology, the method is characterized in that: two rigid guide pins parallel to each other are fixed on both sides of the sample test section, the rigid guide pins are perpendicular to the central axis of the stretching direction of the sample test section, the length of the rigid guide pins is greater than the width of the sample test section, and a light transmission digital micrometer is used to measure the initial distance between the two rigid guide pins, the real-time distance during the stretching process, and the final distance after the stretching is completed, and the real-time strain and final strain of the sample test section are calculated, wherein the measurement position of the micrometer is located on both sides of the sample test section, and the distance from the central axis of the stretching direction of the sample test section is equal. The present invention measures the distance change of the rigid guide pins during the stretching process through the light transmission measurement technology, and realizes the rapid and convenient measurement of the strain of small test area materials, flexible materials and large deformation conditions. It overcomes the defects of the existing measurement methods and better makes up for the blind spots of the application of several methods.

Description

一种基于光透过测量技术的应变测量方法及其装置A strain measurement method and device based on light transmission measurement technology

技术领域 technical field

本发明属于机械领域中的应变测量方法及测量装置,具体为一种基于光透过测量技术的应变测量方法及其装置。The invention belongs to a strain measurement method and a measurement device in the mechanical field, in particular to a strain measurement method and a device based on light transmission measurement technology.

背景技术 Background technique

目前机械领域中的应变测量方法主要有电阻应变法,使用机械式电子引伸计,以及采用激光全息干涉技术等等。但是电阻应变方法中由于受到应变片自身面积的影响,对表面积较小的试样进行测量时往往不适用,而且应变片自身还有强度限制,当需要进行大形变测量时,电阻应变方法往往也不适用;而使用机械式电子引伸计时,需要夹在试样上,被测面太小或太大都不适用,且所测材料的刚度必须足够大,否则材料受引伸计作用产生的应变将影响材料自身的应变;激光全息干涉技术中设备较昂贵,并且在检测时受机械振动、声振动(如环境噪声)以及环境光等的干扰大等等,因此需要在安静、清洁的暗室中进行检测,对环境要求很高。这些方法都不适合应用于小试验面积材料、柔性材料和大形变情况应变的快速方便测量中。At present, the strain measurement methods in the mechanical field mainly include the resistance strain method, the use of mechanical electronic extensometers, and the use of laser holographic interferometry and so on. However, due to the influence of the area of the strain gauge itself, the resistance strain method is often not suitable for measuring samples with a small surface area, and the strain gauge itself has strength limitations. When large deformation measurements are required, the resistance strain method is often not suitable. Not applicable; while using a mechanical electronic extensometer, it needs to be clamped on the sample. It is not applicable if the measured surface is too small or too large, and the stiffness of the material to be measured must be large enough, otherwise the material will be affected by the strain generated by the extensometer. The strain of the material itself; the equipment in laser holographic interferometry technology is relatively expensive, and it is greatly disturbed by mechanical vibration, acoustic vibration (such as environmental noise) and ambient light during detection, etc., so it needs to be detected in a quiet and clean dark room , has high requirements on the environment. These methods are not suitable for fast and convenient measurement of strain in small test area materials, flexible materials and large deformation conditions.

发明内容 Contents of the invention

要解决的技术问题technical problem to be solved

为解决现有方法不适合应用于小试验面积材料、柔性材料和大形变情况应变的快速方便测量中的技术问题,本发明提出一种基于光透过测量技术的应变测量方法及其装置。In order to solve the technical problem that existing methods are not suitable for fast and convenient measurement of strain in small test area materials, flexible materials and large deformation conditions, the present invention proposes a strain measurement method and device based on light transmission measurement technology.

技术方案Technical solutions

所述的一种基于光透过测量技术的应变测量方法,其特征在于:包括以下步骤:The described strain measurement method based on light transmission measurement technology is characterized in that: comprising the following steps:

步骤1、在试样试验段两侧固定两根相互平行的刚性引针,刚性引针与试样试验段拉伸方向的中心轴线垂直,刚性引针长度大于试样试验段的宽度;Step 1. Fix two rigid guide pins parallel to each other on both sides of the sample test section, the rigid guide pins are perpendicular to the central axis of the tensile direction of the sample test section, and the length of the rigid guide pins is greater than the width of the sample test section;

步骤2、采用光透式数字测微计测量两根刚性引针间的距离Sl和Sr,以Sl和Sr的平均距离S=(Sl+Sr)/2作为试样试验段的初始长度S,其中Sl和Sr的测量位置位于试样试验段两侧,且与试样试验段拉伸方向中心轴线的距离相等;Step 2. Measure the distance S l and S r between two rigid guide pins with a light-transmitting digital micrometer, and take the average distance S = (S l + S r )/2 of S l and S r as the sample test The initial length S of the segment, where the measurement positions of S l and S r are located on both sides of the sample test section, and the distance from the central axis of the sample test section in the tensile direction is equal;

步骤3、拉伸试样,采用光透式数字测微计实时测量两根刚性引针间的距离S′l和S′r,测量位置与步骤2中测量位置相同,以S′l和S′r的平均距离S′=(S′l+S′r)/2作为试样试验段的长度S′,通过公式ε′=(S-S′)/S实时得到试样试验段的应变ε′;Step 3, stretching the sample, using a light-transmitting digital micrometer to measure the distance S′ l and S′ r between the two rigid guide pins in real time, the measurement position is the same as that in step 2, and the distance between S′ l and S The average distance S' of ' r = (S' l + S' r )/2 is taken as the length S' of the sample test section, and the strain ε' of the sample test section is obtained in real time by the formula ε'=(SS')/S ;

步骤4、达到设定的拉伸力时,停止拉伸试样,采用光透式数字测微计测量两根刚性引针间的距离S″t和S″r,测量位置与步骤2中测量位置相同,以S″l和S″r的平均距离S″=(S″l+S″r)/2作为试样试验段的最终长度S″,并通过公式ε″=(S-S″)/S得到试样试验段的最终应变ε″。Step 4. When the set tensile force is reached, stop stretching the sample, and use a light-transmitting digital micrometer to measure the distance S″ t and S″ r between the two rigid guide pins. The measurement position is the same as that measured in step 2. The position is the same, the average distance S″=(S″ l + S″ r )/2 between S″ l and S″ r is used as the final length S″ of the sample test section, and the formula ε″=(SS″)/ S obtains the final strain ε" of the test section of the sample.

本发明所述一种基于光透过测量技术的应变测量方法的优选方法,其特征在于:当试样材料为金属材料时,使用锡焊固定刚性引针;当试样材料为非金属材料时,使用粘胶固定刚性引针。A preferred method of the strain measurement method based on light transmission measurement technology in the present invention is characterized in that: when the sample material is a metal material, use soldering to fix the rigid guide pin; when the sample material is a non-metallic material , secure the rigid pins with adhesive.

本发明所述一种基于光透过测量技术的应变测量方法的优选方法,其特征在于:刚性引针为粗细均匀的圆柱引针,且硬度至少达到45HRC。The preferred method of the strain measurement method based on light transmission measurement technology in the present invention is characterized in that: the rigid guide pin is a cylindrical guide pin with uniform thickness, and the hardness reaches at least 45HRC.

一种实现本发明所述一种基于光透过测量技术的应变测量方法的装置,其特征在于:包括金属试验台和光透式数字测微计,金属试验台通过底部的卡孔固定在试验机平台上,金属试验台上部有两个测微计安放槽,两个测微计安放槽之间为对称标记,对称标记上方有对中槽,对中槽与对称标记纵向中心轴线重合;光透式数字测微计放置在测微计安放槽内,且紧贴在对称标记上;当带有刚性引针的试样加装在试验机上时,通过对中槽将试样对中。A device for implementing a strain measurement method based on light transmission measurement technology described in the present invention is characterized in that it includes a metal test bench and a light transmission digital micrometer, and the metal test bench is fixed on the testing machine through a clamping hole at the bottom On the platform, there are two micrometer placement grooves on the upper part of the metal test bench. There is a symmetrical mark between the two micrometer placement grooves. There is a centering groove above the symmetrical mark. The centering groove coincides with the longitudinal central axis of the symmetrical mark; The type digital micrometer is placed in the micrometer placement groove, and it is close to the symmetry mark; when the sample with a rigid guide pin is installed on the testing machine, the sample is centered through the centering groove.

有益效果Beneficial effect

本发明通过光透过测量技术测量刚性引针在拉伸过程中的距离变化,实现了对小试验面积材料和大形变情况应变及应力的快速方便测量。克服了现有测量方法的缺陷,较好地弥补了几种方法应用的盲区。The invention measures the distance change of the rigid guide pin in the stretching process through the light transmission measurement technology, and realizes the rapid and convenient measurement of the strain and stress of materials with a small test area and large deformation conditions. It overcomes the defects of the existing measurement methods and better makes up for the blind spots in the application of several methods.

附图说明 Description of drawings

图1:本发明的结构示意图;Fig. 1: structural representation of the present invention;

图2:金属试验台结构示意图;Figure 2: Schematic diagram of the structure of the metal test bench;

图3:试验机平台示意图;Figure 3: Schematic diagram of the testing machine platform;

图4:光透式数字测微计测量原理图;Figure 4: Schematic diagram of light transmission digital micrometer measurement;

图5:狗骨形试样的示意图;Figure 5: Schematic diagram of a dog-bone-shaped specimen;

其中:1、金属试验台;2、光透式数字测微计;3、试样;4、刚性引针;5、试验机平台;6、测微计安放槽;7、对称标记;8、对中槽;9、减轻孔;10、卡孔;11、试验机平台基座;12、试验机平台安装凸起;13、光透式数字测微计发射端;14、光透式数字测微计接收端。Among them: 1. Metal test bench; 2. Light-transmitting digital micrometer; 3. Sample; 4. Rigid guide pin; 5. Testing machine platform; 6. Micrometer placement groove; 7. Symmetrical mark; 8. Centering groove; 9. Relief hole; 10. Clamping hole; 11. Testing machine platform base; 12. Testing machine platform installation protrusion; micrometer receiver.

具体实施方式 Detailed ways

下面结合实施例具体说明本发明:The present invention is specifically described below in conjunction with embodiment:

参照附图1、附图2和附图3,本发明所述基于光透过测量技术的应变测量装置包括金属试验台1和光透式数字测微计2,金属试验台1通过底部的卡孔10固定在试验机平台5上;金属试验台1上部有两个测微计安放槽6,两个测微计安放槽6之间为对称标记7,对称标记7上方有对中槽8,对中槽8与对称标记7纵向中心轴线重合;光透式数字测微计2放置在测微计安放槽6内,且紧贴在对称标记7上,使用测微计卡具将光透式数字测微计2与金属试验台1固定;带有刚性引针4的试样3加装在试验机上,且试样试验段中心轴线与对中槽8对齐,保证两台光透式数字测微计2的测量位置距试样试验段中心轴线的距离相等。With reference to accompanying drawing 1, accompanying drawing 2 and accompanying drawing 3, the strain measuring device based on light transmission measurement technology of the present invention comprises metal test stand 1 and light-transmitting digital micrometer 2, and metal test stand 1 passes through the stuck hole at the bottom 10 is fixed on the platform 5 of the testing machine; there are two micrometer placement grooves 6 on the upper part of the metal test bench 1, a symmetrical mark 7 is located between the two micrometer placement grooves 6, and a centering groove 8 is arranged above the symmetrical mark 7. The middle groove 8 coincides with the longitudinal central axis of the symmetry mark 7; the light-transmitting digital micrometer 2 is placed in the micrometer placement groove 6, and is closely attached to the symmetry mark 7, and the light-transmitting digital micrometer 2 The micrometer 2 is fixed to the metal test bench 1; the sample 3 with the rigid guide pin 4 is installed on the testing machine, and the central axis of the sample test section is aligned with the centering groove 8 to ensure that the two light-transmitting digital micrometers The distance between the measuring position of gauge 2 and the central axis of the sample test section is equal.

本实施例中,采用上述应变测量装置对矩形纯铜试样和狗骨形纯铜试样(附图5中给出了狗骨形式样的形状图)进行了应变测量,其中使用的光透式数字测微计2的型号为KEYENCE公司生产的LS-7010,矩形纯铜试样尺寸为16×1×9(mm),狗骨形纯铜试样中间试验段段尺寸为6×1×6(mm)。In the present embodiment, the above-mentioned strain measuring device is used to measure the strain of the rectangular pure copper sample and the dog-bone-shaped pure copper sample (the shape diagram of the dog-bone-shaped sample is provided in the accompanying drawing 5). The type of digital micrometer 2 is LS-7010 produced by KEYENCE Company, the size of the rectangular pure copper sample is 16×1×9 (mm), and the size of the middle test section of the dog-bone pure copper sample is 6×1×6 (mm).

首先,在矩形纯铜试样和狗骨形纯铜试样的试验段两侧采用锡焊方法固定两根相互平行的刚性引针4,刚性引针与试样试验段拉伸方向的中心轴线垂直,且刚性引针4的长度大于试样试验段的宽度;使用的刚性引针4为粗细均匀的圆柱型引针,硬度达到45HRC。First, fix two parallel rigid guide pins 4 on both sides of the test section of the rectangular pure copper sample and the dog-bone-shaped pure copper sample by soldering method, the rigid guide pins and the central axis of the tensile direction of the test section of the sample Vertical, and the length of the rigid guide pin 4 is greater than the width of the sample test section; the rigid guide pin 4 used is a cylindrical guide pin with uniform thickness, and the hardness reaches 45HRC.

其次,将固定有刚性引针4的式样3加装在试验机上,且试样试验段中心轴线与对中槽8对齐,保证两台光透式数字测微计2的测量位置距试样试验段中心轴线的距离相等。采用光透式数字测微计2测量两根刚性引针间的距离St和Sr,Sl为试样试验段左侧测量位置测出的距离,Sr为试样试验段右侧测量位置测出的距离,以Sl和Sr的平均距离S=(Sl+Sr)/2作为试样试验段的初始长度S。Secondly, the pattern 3 fixed with the rigid guide pin 4 is installed on the testing machine, and the central axis of the sample test section is aligned with the centering groove 8, so as to ensure that the measurement position of the two light-transmitting digital micrometers 2 is far from the test sample. The distance from the central axis of the segment is equal. Measure the distances S t and S r between the two rigid guide pins with a light-transmitting digital micrometer 2, S l is the distance measured at the left side of the sample test section, and S r is the distance measured at the right side of the sample test section For the distance measured at the position, take the average distance S=(S l +S r )/2 between S l and S r as the initial length S of the test section of the sample.

接下来,启动试验机,拉伸试样,采用光透式数字测微计2实时测量两根刚性引针4间的距离S′l和S′r,以S′l和S′r的平均距离S′=(S′l+S′r)/2作为试样试验段的长度S′,通过公式ε′=(S-S′)/S实时得到试样试验段的应变ε′。而将实时得到的式样应变值与拉伸机提供的应力值相结合,绘制出应力应变曲线。Next, start the testing machine, stretch the sample, and measure the distance S′ l and S′ r between the two rigid guide pins 4 in real time by using the light-transmitting digital micrometer 2, and take the average of S′ l and S′ r The distance S' = (S' l + S' r )/2 is taken as the length S' of the sample test section, and the strain ε' of the sample test section is obtained in real time by the formula ε'=(SS')/S. The stress-strain curve is drawn by combining the sample strain value obtained in real time with the stress value provided by the stretching machine.

最后,当试验机达到设定的拉伸力时,停止拉伸试样,采用光透式数字测微计2测量两根刚性引针4间的距离S″l和S″r,以S″l和S″r的平均距离S″=(S″l+S″r)/2作为试样试验段的最终长度S″,并通过公式ε″=(S-S″)/S得到试样试验段的最终应变ε″。Finally, when the testing machine reaches the set tensile force, the tensile sample is stopped, and the distances S″ l and S″ r between the two rigid guide pins 4 are measured by using the light-transmitting digital micrometer 2, with S″ The average distance between l and S″ r S″=(S″ l +S″ r )/2 is used as the final length S″ of the sample test section, and the sample test section is obtained by the formula ε″=(SS″)/S The final strain ε″.

其中,在获得试样试验段的初始长度S和试样试验段的最终长度S″时,采用了如下处理方法:在静态力下,使用光透式数字测微计2以2400次/秒的频率进行数据采集,持续采集数据10秒,从而得到足够多数据,以测量Sl为例,设采集10秒共取得Sl的24000个数据为χ1~χ24000,得到均值为:Wherein, when obtaining the initial length S of the sample test section and the final length S" of the sample test section, the following processing method is adopted: under static force, use the light-transmitting digital micrometer 2 at 2400 times/second Collect data frequently, and collect data continuously for 10 seconds, so as to obtain enough data. Taking the measurement of S l as an example, assuming that 24,000 data of S l are obtained in 10 seconds of collection, they are χ 124000 , and the average value obtained is:

χχ ‾‾ == 11 2400024000 ΣΣ ii == 11 2400024000 χχ ii

标准差为:The standard deviation is:

σσ == ΣΣ ii == 11 2400024000 (( χχ ii -- χχ ‾‾ )) 22 2399923999

使用拉依达准则,剔除粗大误差,即排除在

Figure BSA00000282644000043
之外的值,用剩余数据再求一次得到均值
Figure BSA00000282644000044
Figure BSA00000282644000045
其余Sr、S″l和S″r以同样方法得到。Use the Raida criterion to eliminate gross errors, that is, exclude the
Figure BSA00000282644000043
For values other than , use the remaining data to find the mean again
Figure BSA00000282644000044
Pick
Figure BSA00000282644000045
The rest of S r , S″ l and S″ r are obtained in the same way.

下面给出了在700N和1400N拉伸力下,本方法的应变测量测量结果与电阻应变法、通过拉伸机测得的总体应变以及理论计算值之间的对比结果。其中由于在1400N拉伸力下,应变片被拉断,所以没有此条件下的电阻应变法结果,而且在1400N拉伸力下,进入塑性变形阶段,也没有理论模型。此外,通过拉伸机测得的总体应变主要用于矩形式样对比,这是因为矩形式样的总体应变应与局部应变相同,狗骨形式样则不然。另外,在理论计算中,由于狗骨型式样形状不规则,无法计算出理论值。The comparison results between the strain measurement results of this method and the resistance strain method, the overall strain measured by the stretching machine and the theoretical calculation value are given below under the tensile force of 700N and 1400N. Among them, since the strain gauge is broken under the tensile force of 1400N, there is no result of the resistance strain method under this condition, and there is no theoretical model when it enters the plastic deformation stage under the tensile force of 1400N. In addition, the global strain measured by the tensile machine is mainly used for comparison of the rectangular specimens, because the global strain should be the same as the local strain for the rectangular specimens, which is not the case for the dog-bone specimens. In addition, in the theoretical calculation, due to the irregular shape of the dog-bone pattern, the theoretical value cannot be calculated.

Figure BSA00000282644000051
Figure BSA00000282644000051

从表中的结果可以看出,对小试验面积和大形变试样,传统的电阻应变法不仅在测量范围上很有局限,在承受范围内的测量结果也存在较大误差;而本系统实测应变得到的结果与理论值和拉伸机测得总体应变都比较接近,且测量范围很大,可实际运用。It can be seen from the results in the table that for small test areas and large deformation samples, the traditional resistance strain method not only has limitations in the measurement range, but also has large errors in the measurement results within the tolerance range; The results obtained by the strain are relatively close to the theoretical value and the overall strain measured by the stretching machine, and the measurement range is large, which can be used in practice.

Claims (4)

1. strain measurement method based on the light transmission measuring technique is characterized in that: may further comprise the steps:
Step 1, fixing two rigidity that are parallel to each other are drawn pin in specimen test section both sides, and it is vertical with the central axis of specimen test section draw direction that rigidity is drawn pin, and rigidity is drawn the width of pin length greater than the specimen test section;
Step 2, adopt light pass through the formula digital micrometer measure two rigidity draw between pin apart from S lAnd S r, S lBe the distance that measure measuring position, specimen test section left side, S rThe distance of measuring for measuring position, specimen test section right side is with S lAnd S rMean distance S=(S l+ S r)/2 are as the initial length S of specimen test section, wherein S lAnd S rThe measuring position be positioned at specimen test section both sides, and equate with the distance of specimen test section draw direction central axis;
Step 3, tensile sample, adopt light pass through the formula digital micrometer measure in real time two rigidity draw between pin apart from S ' lAnd S ' r, the measuring position is identical in measuring position and the step 2, with S ' lAnd S ' rMean distance S '=(S ' l+ S ' r)/2 are as the length S ' of specimen test section, through formula ε '=(S-S ')/S obtain in real time the strain stress of specimen test section ';
Step 4, when reaching the tensile force of setting, stop tensile sample, adopt light pass through the formula digital micrometer measure two rigidity draw between pin apart from S " lAnd S " r, the measuring position is identical in measuring position and the step 2, with S " lAnd S " rMean distance S "=(S " l+ S " r)/2 are as the final lengths S of specimen test section ", and through formula ε "=(S-S ")/S obtain the final strain stress of specimen test section ".
2. a kind of strain measurement method based on the light transmission measuring technique according to claim 1 is characterized in that:
When sample material was metal material, pin was drawn in use soldering fixedly rigidity; When sample material was nonmetallic materials, use viscose glue fixedly rigidity drew pin.
3. a kind of strain measurement method based on the light transmission measuring technique according to claim 1 is characterized in that: it is that the cylinder of even thickness draws pin that rigidity is drawn pin, and hardness reaches 45HRC at least.
4. device of realizing the said strain measurement method based on the light transmission measuring technique of claim 1; It is characterized in that: comprise that metallographictest platform and two light pass through the formula digital micrometer; The metallographictest platform is fixed on the testing machine platform through the hole clipping of bottom, and two micrometer mounting grooves are arranged at metallographictest platform top, is symmetrical mark between two micrometer mounting grooves; There is the centering groove symmetry mark top, and the centering groove overlaps with symmetrical mark longitudinal center axis; Light passes through the formula digital micrometer and is placed in the micrometer mounting groove, and is close on the symmetrical mark; When having rigidity and draw the sample of pin and be installed on the testing machine, through the centering groove with sample centering.
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