光的干涉与衍射

O348.1 2004064033 实时确定光弹性参数的积分相移法=Real-time determination of photoelatic parameters by integrated phase-shifting method[刊,中]/雷振坤(天津大学机械学院力学系.天津(300072)),亢一澜…∥光学技术.—2004,30(3).—280-283,288 积分相移法可以实时测量光弹性参数,在光弹性实验的某些变载测试中将有一定的发展潜力。推导了积分     

平面偏振光场光弹性实时相移法

光弹性法可广泛用于二维、三维应力或应变场的研究。根据偏振相移法的原理,提出一种新的积分相移法,并设计了用于全场等倾线和等差线实时分析的光弹性仪。在正交偏振光场下,按一定速度同步旋转起偏镜和分析镜,CCD摄像机可连续获取四幅相移光弹图像,由CCD像敏单元积分获得其光强值,通过所提出的相移法运算,可以迅速地得出全场等倾角和等差线的相位值。该方法和装置不仅可用于光学原件及玻璃制品的高速检测,而且也可用于随时间缓慢变化的光弹性分析中。     

全场数字化测量光弹性等倾角的五步彩色相移法

通过把相移法与光学彩色信息图像处理技术相结合 ,提出了一种确定全场光弹性等倾角的五步彩色相移法。模型置于白光照射下 ,在起偏镜与分析镜不同设置的平面偏振光场中 ,用彩色数码照相机分别采集五幅等色线与等倾线相耦合的条纹图 ,根据相移法基本原理 ,就可以确定在 0～π/2范围内的等倾角。经过对径压缩圆盘的检验 ,实验结果与理论完全相符。该方法改进了单色光相移法的不足 ,对实验应力分析及其在工程结构强度设计中的应用将起积极的促进作用     

数字光弹性中六步混合相移技术

数字光弹性应力分析中常用相移法确定等倾线和等差线,最广泛应用的是十步相移法,针对单色光入射引起的等倾线耦合等差线的问题,增加采集白光入射4幅图像,使用不同光弹图像集分别计算等倾线和等差线,测量精度更高但操作复杂、效率较低。本文提出一种优化的六步混合相移方法,将十步相移法的6+4测量方法缩减为3+3的六步测量方法。用仿真模拟实验对本文方法进行误差分析,验证了其具有良好的抗噪性能和相移误差抗干扰能力。真实实验结果表明：与传统六步相移法相比,本文方法有效解决了等倾线耦合等差线以及波片失配误差的问题;与十步相移法相比,本文方法与其等倾线平均偏差约为0.01 rad,等差线平均偏差约为0.09 rad,在提高40%采集效率的同时保证了测量精度。     

数字光弹性相移法中全场等倾角和等差线相位

以径向受压圆盘为例,从弹性力学的角度详细分析了模型全场等倾角相位的情况,分析第一主应力的方向,在六步相移法的基础上提炼出圆盘全场等倾角相位和等差线的真实相位。采用有限元软件MARC与形函数拟合相结合的方法模拟径向受压圆环六步相移图和等差线相位图,可以推广到没有解析解或者解析解复杂的应力模型的光弹性实验模拟。通过径向受压圆盘实验验证了方法的可行性,实现光弹法中自动提取全场等差线的信息。     

数字光弹性中五步彩色相移法及其应用

把相移法与光学彩色信息图像处理技术相结合,提出全场数字化确定主方向角的光弹性五步彩色相移法。其主要优点是采用最简单的白光平面偏振仪光学系统,由数码照相机采集五幅等色线与等倾线相互耦合的彩色条纹图,经计算机进行处理后,就可以得到[O～π／2]范围内单纯连续的等倾角相图;为了减少测量误差,在相移法中引入背景光强参与运算。对实验中存在的三种主要误差因素进行了定量分析,给出了具体的误差控制指标。用对径压缩圆盘问题的理论仿真模拟结果、基本实验和复杂平面及空间实际问题进行检验和对比,表明本方法是正确可行的。     

多幅图像运算模块的建立及在光弹性图像处理中的应用

介绍光弹性图像处理软件中多幅图像运算模块的建立,该模块具有多幅图像运算,表达式中的图像文件数自动识别,对单个或多个图像文件进行二值化操作,计算结果的拉伸及预览以及结果的显示与保存等功能,该模块在光弹性图像处理中可实现等倾线的分离,等差线的倍增及相移技术等。     

平面偏振光场光弹性实时相移法的误差分析

研究了在获取图像的过程中转角变化、偏振片方位角误差及试件所受的载荷变化对平面偏振光场光弹性实时相移法的影响。通过理论分析与数值模拟,讨论了在不同条件下等倾角相位误差。等倾角相位误差随着每场转角变化的增加而增大;偏振镜方位角误差使等倾角相位产生平移;试件所受的载荷变化会引起所采集的光弹性图像误差,对等倾角的计算结果会产生较大的影响。研究结果对合理设计光弹性实验装置、正确评价和执行实验技术具有积极的指导作用。     

光弹性法中时间边缘效应数学模型和应用研究

在光弹性实验中,模型边缘会产生随时间增长的条纹,它干扰正常的由外载荷引起的应力条纹,给实验带来误差。根据时间边缘效应产生的原因建立了时效数学模型,通过对比根据建立的数学模型模拟的等差线和实验得到的等差线,可以验证所建立的数学模型能够准确地反映出时效的特征,并尝试运用数字光弹性相移法去除时效的影响。     

光强和方位角误差对光弹性五步彩色相移法的影响

为了了解相移法中的各种参数所产生的误差对最终结果的影响 ,对一些主要参数做深入的误差分析是十分必要的。针对五步彩色相移法所用的白光入射平面偏振场的特点 ,只考虑光强、起偏镜和分析镜方位角所引起的误差影响就可以了。提出一个分析和评估这些误差源对五步彩色相移法确定等倾角参数所产生影响的方法 ,这对合理设计实验装置和执行正确的实验条件将起到积极的作用     

Real-time phase-shift ing techniques for determining the photoelastic parameters: a theoretical comparison

Among data acquisition techniques in digital photoelasticity, the integrated phase shifting technique (IPST) can real-time analyze the photoelastic parameters at a video rate of the high speed CCD camera. In this paper, fourteen algorithms are described by different configurations of the rotating an analyzer at a constant rate and an output quarter-wave plate at another constant rate. The theoretical comparisons of the algorithms are given by the simulated phase distributions of the isochromatic and isoclinic parameters of the disk under two cases that the load keeps unchangeable or linearly increasing in exposure time of the camera. Then a guideline is given to alleviate the influence of the load changing with time on the IPST.     

A numerical comparison of real-time phase-shifting algorithms

Among data acquisition techniques in digital photoelasticity, the integrated phase shifting technique (IPST) can real-time analyze the photoelastic parameters at a video rate of the high speed CCD camera. In this paper, fourteen algorithms are described by different configurations of the rotating an analyzer at a constant rate and an output quarter-wave plate at another constant rate. The theoretical comparisons of the algorithms are given by the simulated phase distributions of the isochromatic and isoclinic parameters of the disk under two cases that the load keeps unchangeable or linear increasing in exposure time of the camera. Then a guideline is given to alleviate the influence of the load changing with time on the IPST.     

一种弹光调制器精确定标微系统设计

弹光调制器利用各向同性晶体受迫振动后产生的双折射效应,对入射的偏振光进行相位调制,在偏振调制及测量方面具有重要应用.弹光调制器的相位延迟是其关键指标参数,实际应用时需对驱动电压与相位延迟进行标定.但传统的弹光调制器定标系统中的元件体积较大,且在使用前完成标定,误差大.为了使弹光调制系统能够实现实时定标,达到精确定标的目...     

The influence of the quarter wave plates in automated photoelasticity

During the last decades, several methods have been proposed to automate photoelastic analyses. Some procedures are based on the circularly polarised light by using quarter wave plates. However, quarter wave plates are typically matched for a specific wavelength, and an error is introduced at different wavelengths. The error of quarter wave plates affects the measurement of isochromatic and isoclinic data. In this paper, the influence of the errors of quarter wave plates in some of the most common automated photoelastic methods is reviewed. The errors in the photoelastic data are given and the procedures to reduce, or eliminate, them are also suggested.     

Photoelasticity in polycrystalline aggregates

A theory for the photoelastic behaviour of transparent polycrystalline aggregates consisting of randomly oriented anisotropic crystallites has been developed. Such an aggregate is isotropic but it becomes birefringent under the influence of a uniaxial load. The photoelastic constants of the aggregate are given by the components of the spatial average of the photoelastic tensor of the single crystal, and are worked out by assuming either the strain to be continuous (Voigt approximation) or the stress to be continuous (Reuss approximation). The components of the average photoelastic tensor are very different for these two limits. The elastic and the photoelastic constants of alkali halide aggregates have been evaluated for both the stress continuity and the strain continuity conditions. The maximum variation of the elastic constants in going from the Voigt to the Reuss condition is 50 per cent while the photoelastic birefringence can vary by as much as 300 per cent in alkali halides. In the case of KI and rubidium halides even the sign of the photoelastic birefringence is different for the two limits.     

球壳激光窗口附加相移的分析和计算

分析了球壳激光窗口附加相移产生的原因 :窗口本身光路长度不等、窗口材料的热和弹光效应引起的折射率和应变分布不均。用差分法计算了光波阵面附加相移的分布 ,结果表明 ,窗口参数的选择对光束位相分布影响较大。考虑热和弹光效应 ,依据远场光斑中心峰值的大小 ,得到较佳的窗口参数 ,减小了附加相移对光束质量的影响。     

On photoelastic stress measurements in optically absorbing medium

The effects of optical absorption in a photoelastic medium on the formation of the fringe patterns are studied by taking into account the stress-induced anisotropy of both the refractive index and the absorption coefficient. The propagation of optical waves in a dielectric solid under the influence of stress is formulated by incorporating complex elasto-optical tensor elements in the wave equation. The expression for optical transmission from the plane polariscope configuration consisting of an absorbing photoelastic specimen is derived using the Jones calculus formalism including complex optical retardation terms. It is observed that the photoelastic fringe fields are substantially modified due to these effects which must be considered for accurate interpretation of the experimentally obtained fringes.     

高速动光弹系统及其应用

高速动光弹仪是动态光弹性研究的有效诊断工具,主要用于记录各种结构在动载荷作用下,不同瞬间的应力条纹图像。研究应力波的传播规律,裂纹扩展过程,固体高速变形等。通常的动光弹仪为多火花式动光弹仪。国外也有采用静态光弹仪与转镜式高速分幅相机结合的系统。我们研究调试的动光弹系统,是在高速纹影系统中加入偏振光场,即静态光弹系统、纹影系统与转镜式高速分幅相机结合。在雷管动载荷作用下,应用高压脉冲氙灯光源,单色圆偏振光亮场,获得了不同光弹模型的清晰应力条纹图像。给出应力波的传播过程和孔附近产生的应力集中现象。该系统具有摄影频率高、曝光时间短、测试灵敏度高、适于强载荷、远距离研究大尺寸光弹模型,同时具有透射式和反射式光学系统等特点。从而为动态光。弹性研究提供了有效的测试技术和诊断系统。     

Limitation of carrier fringe methods in digital photoelasticity

The carrier fringes method has been proposed in digital photoelasticity in combination with techniques such as Fourier transform and phase shifting method, without considering the influence of the isoclinics on the isochromatic patterns analysis. Unlike other optical methods as moiré and holographic interferometry, in photoelasticity the light intensity emerging from a circular polariscope is related to both the isochromatic retardation and the isoclinic parameter. As it is shown by the theoretical analysis, owing to the misalignment between the principal stresses in the model and in the carrier, the computed retardation is affected by an error which is the same for all photoelastic methods based on the use of carrier fringes. Consequently, the photoelastic analysis carried out by methods that use carrier fringes cannot be applied as a full-field technique. In detail, numerical simulations show that the retardation error is comparable (less than 0.05 fringe orders) with that of other photoelastic methods provided that the misalignment between the principal stresses in the model and in the carrier is less than 30°. On the contrary, in the model zones where the misalignment is higher than 30°, the retardation measurement can be affected by non negligible errors (up to 0.25 fringe orders).