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Uncertainty Analysis of Kolsky Bar Strain Gage Output

机译:Kolsky Bar应变计输出的不确定性分析

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An apparatus has been built at the National Institute of Standards and Technology (NIST) to measure the dynamic stress-strain relationships for metals at elevated temperatures. The NIST Pulse Heated Kolsky Bar apparatus has the capability to resistively heat samples to over 1000 C with heating rates of over 10 000 C/s in addition to performing the traditional Kolsky bar impact testing. The traditional Kolsky bar (or Split Hopkinson Pressure Bar) consists of two long hardened steel bars aligned end-to-end with the sample sandwiched in between the bars. A test is carried out by striking the end of the incident bar with a projectile fired from an air gun that sends an elastic wave down the bar, which then rapidly deforms the sample. As the sample is deformed a transmitted wave is started down the second bar. Standard variable resistance metal foil strain gages are mounted in the center of each of the long bars that measure the amplitude of the strain wave as a function of time. The outputs of the strain gages are recorded on a standard digital oscilloscope data acquisition system. Using the strain gage signal recordings a high-strain rate stress-strain curve for the sample material can then be calculated using a well established method. Our Kolsky bar apparatus can test samples at strain rates from about 500 /s to 10 000 /s (normal compression machines in materials test labs operate in the range of 0.01 /s and under special conditions can go as high as 100 /s.) By measuring the temperature of the sample during the deformation (the deformation takes approximately 150 microseconds) the stress-strain curve can be reported for various temperatures. The strain gage measuring system is calibrated by a standard method of shorting a large precision resistor across the gage and recording the output. The uncertainty of the simulated strain in this parallel resistor calibration method depends on the uncertainty of the value of the parallel resistor, the gage resistance, and the manufacturer's gage factor. There is an additional contribution to the uncertainty of the measurement results because of the dynamic effects on the gage factor. To understand the accuracy of the strain gage output the different uncertainties need to be combined in an uncertainty analysis. The uncertainty analysis of the strain gage calibration method presented in this paper uses an approach based on NIST Technical Note 1297. Future papers will address the uncertainty of the temperature measuring methods and some of the effects of the assumptions used in the Kolsky bar simple theory for relating strain in the elastic bars to the stress and strain in the sample.
机译:在国家标准和技术研究所(NIST)建立了一种设备,以测量升高温度下金属的动态应力 - 应变关系。 NIST脉冲加热的KOLSKY BAR设备的能力除了执行传统的KOLSKY BAR冲击试验之外,还具有超过10 000c / s的加热速率的高热样品。传统的Kolsky Bar(或Split Hopkinson压力杆)由两个长的硬化钢筋组成,其端到端对齐,样品夹在杆之间。通过从入射杆的末端撞击从气枪射出的射弹,从而通过向下方发射弹性波,然后快速变形样品来进行测试。当样品变形时,透射波开始第二杆。标准可变电阻金属箔应变计安装在每个长条的中心的中心,该长条测量应变波的振幅作为时间的函数。应变计的输出记录在标准数字示波器数据采集系统上。使用应变计信号记录可以使用良好的方法计算样品材料的高应变率应力 - 应变曲线。我们的Kolsky Bar设备可以以约500 / s的应变速率测试样品,从约500 / s至10 000 / s(材料测试实验室的正常压缩机在0.01 / s的范围内,在特殊条件下可以高达100 / s。)通过在变形期间测量样品的温度(变形需要大约150微秒),可以报告应力 - 应变曲线对于各种温度。应变计测量系统通过跨越测量的大型精密电阻的标准方法校准并记录输出。在该并联电阻校准方法中模拟应变的不确定性取决于并联电阻,量大力和制造商的量因子的值的不确定性。由于对量因子的动态影响,对测量结果的不确定性存在额外的贡献。为了了解应变计的准确性,在不确定分析中需要组合不同的不确定性。本文提出的应变计校准方法的不确定分析采用了一种基于NIST技术说明1297的方法。未来的论文将解决温度测量方法的不确定性以及Kolsky Bar简单理论中使用的假设的一些效果将弹性杆中的应变与样品中的应力和菌株相关联。

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