静态和动态3D轮廓使用结构光

R. Rodríguez-Vera, D. Vasquez, K. Genovese, J. Rayas, F. Mendoza-Santoyo
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引用次数: 1

摘要

用于三维形状测量的非破坏性光学技术是科学、工程、医学和工业的基础。这样的3D数据比2D数据有优势:形状数据对光照和物体运动的改变是不变的。获取三维形状的一种主要的、简单的方法是从物体的轮廓出发。轮廓的光学技术有很多种,但最容易实现的是使用线性结构光投影。目前的工作重点是在宏观和微观水平上实现静态和动态3D轮廓的线性结构光投影技术。作为条纹图案的线性结构光被投射到要轮廓的表面上。使用白光和激光照亮塔尔博特图像来投射条纹图案。投影条纹图案由常规或高速CCD相机捕获,用于图像数字化和进一步分析。采用傅里叶变换方法获得了轮廓包覆光学相位图。简单的实验安排适用于表面与轮廓的静态或动态条件。例如,对处于谐波振动条件下的样品,将其振动频率与捕获CCD相机的振动频率进行调谐,从而获得模态振型。在静态情况下,人们可以获得受静载荷作用的表面前后的地形对比,或者简单地比较其地形。在微观和宏观层面上,给出了静态和动态表面条件的例子。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Static and dynamic 3D contouring by using structured light
Non-destructive optical techniques for 3D shape measuring are fundamental in science, engineering, medicine, and industry. Such 3D data offer advantages over 2D data: shape data are invariant against alteration of the illumination and object motion. One of the major and easy methods to obtain 3D shape is from its contours. There exist several optical techniques for contouring, but the easiest to put into operation is by using linear structured light projection. The present work focuses on the implementation of linear structured light projection techniques for static and dynamic 3D contouring at macro- and micro-levels. Linear structured light as a fringe pattern is projected on the surface to be contoured. White light and laser-illuminating Talbot image are used in order to project the fringe pattern. Projected fringe pattern is captured by a conventional or high-speed CCD camera for image digitalizing and further analysis. Fourier transform method is employed as a tool to obtain a contour-wrap optical phase map. The simple experimental arrangement is adapted for static or dynamic conditions of the surface to contour. Samples that are under harmonic vibration conditions, for example, their vibrating frequency is tuned with that of the capture CCD camera to obtain the mode shape. In the static case one can obtain the topographical comparison before and after the surface subject to a static load or simply its topography. Examples, at micro and macro levels, of static and dynamics surface conditions are shown.
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