中子残余应力表征光路对准与样品定位方法

Optical Alignment and Sample Positioning in Neutron Residual Stress Characterization

  • 摘要: 中子残余应力表征通常需分别测试样品的3个主应力方向,而同一测量点在不同方向的中子束取样尺寸不一致将导致测试结果不可靠。因此,在样品台坐标系下精确对准光路和准确定位样品的坐标位置是中子残余应力表征的重要环节,光路对准和样品定位直接影响残余应力测试结果的可靠性。本工作基于实验光路和样品台建立了谱仪的样品台坐标系,以样品台坐标中心定位针的衍射峰累积强度为目标,通过步进扫描依次精确对准了单色器、入射狭缝、衍射狭缝和径向准直器的谱仪光路。在此基础上,根据样品几何特点分别利用全站仪瞄准、入射中子束、衍射中子束和样品轮廓扫描准确定位了典型实验样品的位置坐标,并分析了各定位方法的取样位置精度。其中,通过扫描衍射中子束的衍射峰积分强度与样品平移位置关系获得样品表面的坐标位置,是最准确的定位方法。该工作为指导用户准确可靠地开展中子应力测试奠定了实验基础。

     

    Abstract: Neutron residual stress characterization involves measurement at three principal directions of the sample. However, the measurement of the third principal direction usually requires rotation of sample manually. Inconsistent measurement points in different directions will lead to test failure and wrong result. Accurate optics alignment and precise sample positioning in the coordinate system of the sample stage are important procedures of neutron residual stress characterization, since optics alignment and sample positioning directly affect the reliability of the residual stress test. In this work, the sample stage coordinate system of the diffractometer was established based on the experimental optics and the sample stage. The center of the coordinate system was determined by a positioning hole machined in the center of the sample table and a positioning pin made by martensitic steel, austenitic steel, copper, nickel based high-temperature alloy, aluminum alloy, etc. to satisfy the requirement of conventional metal test. Aimed at the integral intensity of the diffraction peak of the positioning pin, the instrument optics including monochromator, the incident slit, the diffraction slit and the radial collimator was accurately aligned by step scanning. Based on the optics of the neutron residual stress diffractometer and the coordinate system of the sample stage, electronic total station, edge scanning using incident neutron beam and diffraction neutron beam, and sample contour scanning were used to accurately position the sample coordinate. Especially, the position precision was quantitatively analyzed. For samples with regular shapes, the coordinate position of the sample surface could be observed by a total station. According to the attenuation of the sample on incident neutron beam, a low efficient 3He tube detector located at the center of the incident neutron beam was used to record the relationship between neutron intensity and sample translation perpendicular to the incident neutron beam. Neutron intensity of the 3He tube follows a Boltzmann function distribution with the translation position of the sample. The coordinate position of the scanned side of the sample can be obtained through curve fitting. Edge scanning by diffraction beam is the most accurate positioning method. The integral intensity of the diffraction peak is affected by the combined effect of the effective sampling size (contributing diffraction intensity) and the neutron path (attenuating diffraction intensity), while the neutron path and effective sampling size can be obtained by calculating the surface position of the sample. Thus, the relationship between the integral intensity of diffraction peak and the sample translation could be established. The coordinate position of scanning edge can be obtained through curve fitting using transmission scanning optics and reflection scanning optics. For samples with complex shapes, sample contour scanning by coordinate measuring machine or laser scanning arm should be used to obtain the irregular outline drawing. This work will help users understand the optics alignment and sample positioning of neutron residual stress characterization, analyze the error source of residual stress measurement, guide users to accurately and quickly carry out neutron residual stress experiments.

     

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