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三维时域散斑动态干涉测量系统的集成化设计
引用本文:刘子惠,高瞻,高晨家,王煦,钟楚千,刘宇琛,张园.三维时域散斑动态干涉测量系统的集成化设计[J].应用光学,2020,41(4):829-836.
作者姓名:刘子惠  高瞻  高晨家  王煦  钟楚千  刘宇琛  张园
作者单位:北京交通大学 理学院 发光与光信息技术教育部重点实验室,北京 100044
基金项目:国家自然科学基金(51675038)
摘    要:三维电子散斑干涉技术(3D ESPI)具有非接触、高精度、高灵敏度和全场测量等优点,被广泛应用于许多领域。为了实现非接触动态全场三维测量,设计并建立了一个紧凑、完备的三维测量系统。用一个多波长光纤耦合激光器代替3个独立光源,产生的离面、面内散斑干涉图仅用一台彩色CCD相机就能捕捉和处理;整个测量系统采用笼式结构,具有高度的灵活性和稳定性;对基于小波变换的相位展开算法进行了编程,实现了被测物体三维位移信息的完整提取。实验证明该测量系统可以实时获取被测物体的三维位移,在测量实验中,获得的三维位移值17.68 μm、36.23 μm、13.85 μm,相比于实际位移值18.1 μm、36.4 μm、14.0 μm它们的绝对误差分别为0.42 μm、0.17 μm、0.15 μm,相对误差分别为2.3%、0.5%、1.1%。

关 键 词:光学测量    时域散斑干涉    小波变换    集成化设计
收稿时间:2019-07-17

Integrated design of three-dimensional continuous displacement measurement with temporal speckle interferometry
Affiliation:Key Laboratory of Luminescence and Optical Information Technology ( Ministry of Education), School of Science, Beijing Jiaotong University, Beijing 100044, China
Abstract:The three-dimensional electronic speckle pattern interferometry (3D ESPI) is widely used in many fields due to its ascendancy of non-contact, high precision, high sensitivity and full-field measurement. In order to realize the non-contact dynamic full-field 3D measurement, a compact and complete 3D measurement system was designed and set up. Three independent lasers were replaced by a single multi-wavelength fibre coupling laser to produce the speckle pattern interferograms of out-of-plane and in-plane, which could be captured and processed by only one charge coupled device (CCD) camera. The entire measurement system adopted cage construction with high flexibility and stability. The phase unwrapping algorithm based on the wavelet transform was programmed to realize the complete extraction of 3D displacement information on the measured object. The experimental results show that this measurement system can obtain the 3D displacement of the measured object. The 3D displacement values in the experiments are 17.68 μm, 36.23 μm and 13.85 μm, compared with the actual displacement values of 18.1 μm, 36.4 μm and 14.0 μm, the absolute errors are 0.42 μm, 0.17 μm and 0.15 μm, respectively,and the relative errors are 2.3%, 0.5% and 1.1%.
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