摘要
按照由刘与郑于1991年所叙述的以直接测量高角区衍射峰为基础的新技术:α_(measure)=[-cot(2θ_1/2)」(2θ_2-2θ_1)/2(t_2-t_1),这里的θ_1与θ_2分别为温度t_1与t_2时所测得的布拉格角,本文逐项地介绍了新技术的实施步骤与注意事项。
The new technique described by Liu and zheng ( 1991) is based on the direct measurement ofhigh-angle diffraction peads:α_(measure)=[-cot(2θ_1/2)](2θ_2-θ_1))/2(t_2-t_1) , where the Braggangles, θ_1 and θ_2 , are measured at t_1 and t_2 respectively. The implementation steps and conditionsfor implementing the new technique are presented term by term in this paper.
出处
《华南师范大学学报(自然科学版)》
CAS
1995年第2期59-62,共4页
Journal of South China Normal University(Natural Science Edition)
基金
广东省自然科学基金
关键词
热膨胀
测量
粉末衍射仪
晶体
X射线衍射
thermal expansion
implementation of the new measuremen technique