排序方式: 共有60条查询结果,搜索用时 15 毫秒
21.
22.
建立了紫外波段漫反射板双向反射分布函数的测量装置,研究了在特定接收条件下铝漫反射板双向反射分布函数(BRDF)随入射角的变化,并对测量误差作了相应的分析,漫反射板定标的相对精度小于2.5%。测量了铝漫反射板从250~650 nm的半球反射比。随着波长的增加,铝漫反射板的半球反射比略呈上升趋势,在紫外探测仪的探测波段300~360 nm之间变化约6%。监测了铝漫反射板的半球反射比随时间的长期变化。铝漫反射板在制备一年后,其半球反射比基本保持稳定,在紫外探测仪的探测波段300~360 nm范围内,其半球反射比平均下降约0.9%。 相似文献
23.
为了研制CO2探测仪定标漫反射板,采用物理研磨和化学腐蚀相结合的工艺方法制作了铝漫反射板试验样块,搭建了相对双向反射分布函数和半球反射率的测试装置。在0°和45°入射光的情况下,对可见近红外波段的测试结果表明:表面粗糙度影响铝漫反射板的朗伯特性,240#研磨砂制作的漫射板的朗伯特性最佳;化学腐蚀不仅能提高铝漫反射板的朗伯特性,也能提高铝漫反射板的半球反射率。当选取碱蚀温度为室温20℃、NaOH溶液浓度为52.6 g/L时,最佳腐蚀时间约为4 min;镀膜使铝漫反射板的半球反射率平均提高20%,但会使其朗伯特性稍变差;不同波长处铝漫反射板的相对双向反射分布函数略有不同,但变化趋势相同。实验确定了影响漫反射板漫反射特性的关键参数,并定量优化了这些工艺参数,为进一步研制CO2探测仪星上定标漫反射板提供了依据。 相似文献
24.
Miroslav Pech 《Optik》2010,121(20):1881-1884
Two measuring techniques are presented in this paper. These techniques are able to measure and process the shape of the reflecting surfaces. In the first part of the paper the theory and modifications of the optical, mechanical and software design for the Hartmann wavefront analyzer are described. This new method is applied to the non-contact measurement of concave-mirrors shape and objectively defines the shape and specifies the difference of the segment shape from an ideal surface with micrometer accuracy. This difference determines essentially the mirrors image quality. In the second part of the paper attention is concentrated on the other main factor that affects image quality— surface roughness. Thereinafter, physical background and usage of the measuring system and results are presented. 相似文献
25.
The field of predictive rendering concerns itself with those methods of image synthesis which yield results that do not only
look real, but are also radiometrically correct renditions of nature, i.e., which are accurate predictions of what a real scene would look like under given lighting conditions. A real coating consists
of pigments, effect pigments, clear lacquer and glaze. A novel and unique combination of real parameters that are commonly
measured in the industry and a theoretical reflectance model consisting of measurable parameters is required. Here, the authors
design perception parameters and put them into well known surface reflection functions such as He and Torrance. The original
contributions are the study of the sub-surface scattering of real paint and the prediction of its appearance in rendered images
by the proposed model of light reflection beneath the paint surface.
Presented at 5-th International Conference Solid State Surfaces and Interfaces, November 19–24, 2006, Smolenice Castle, Slovakia 相似文献
26.
27.
K. Stamnes B. Hamre G. Ryzhikov R. Mahoney A. Sei 《Journal of Quantitative Spectroscopy & Radiative Transfer》2011,112(4):714-2442
A radiative transfer model for coupled atmosphere-snow-ice-ocean systems (CASIO-DISORT) is used to develop accurate and efficient tools for computing the bidirectional reflectance distribution function (BRDF) of sea ice for a wide range of situations occurring in nature. These tools include a method to generate sea ice inherent optical properties (IOPs: single-scattering albedo, extinction optical depth, and scattering asymmetry parameter) for any wavelength between 300 and 4000 nm as a function of sea ice physical parameters including real and imaginary parts of the sea ice refractive index, brine pocket concentration and effective brine pocket size, air bubble concentration and effective air bubble size, volume fraction of ice impurities and impurity absorption coefficient, and sea ice thickness. The CASIO-DISORT code was used to compute look-up tables (LUTs) of the Fourier expansion coefficients of the BRDF as a function of angles of illumination and observation, sea ice IOPs, and ocean albedo. By interpolation in the LUTs one efficiently obtains accurate BRDF values. To include snow on the ice we modified DISORT2 to accept Fourier expansion coefficients for the BDRF as input instead of the BRDF itself, thereby reducing the computation time by a factor of about 60. The BRDF computed by CASIO-DISORT or retrieved from the LUTs applies to diffuse light only. To remedy this shortcoming we added a specular Gaussian beam component to the new BRDF tool and verified that it works well for BRDFs for bare and snow-covered sea ice. 相似文献
28.
在偏振光条件下,物体的表面反射受到折射率、表面粗糙度、入射角等多种因素的影响。针对粗糙物体表面在不同波段光照下表现出不同的偏振反射特性,提出一种基于Kirchhof理论的偏振光谱BRDF模型。利用已知材质在不同波长下的复折射率,对其折射率和消光系数部分分别反演出的对应光谱模型,进而得到复折射率的光谱模型;同借鉴经典的表面粗糙度测量方法,结合菲涅耳反射公式,推导出表面粗糙度的光谱模型,将得到的复折射率和粗糙度光谱模型与BRDF模型相结合,推导出偏振光谱BRDF建模。模型分别在折射率随波长变化、粗糙度为常量,折射率、粗糙度均随波长变化以及原模型三种情况下进行仿真对比实验,并将所得到的数据与其他资料进行对比。其结果表明,该模型能够较为准确的反映物体表面的偏振反射特性,并且能够描述偏振度随波长变化趋势的光谱特征,能够为偏振遥感、物质分类等方面的应用提供可靠依据。 相似文献
29.
依据双向反射分布函数理论,推导出散射光谱的加和性原理。散射光谱加和性是指对于材质质点之间无相互作用的平面漫反射体系,在光源与入射面材质不存在干涉、衍射、荧光、光谱上转换和光谱下转换等相互转换作用,且无光化学现象及非线性效应发生的前提下,且符合能量守恒定律的同时,由单光源或多光源照射的材料的散射光谱,等于该材料中每种材质的散射光谱的线性叠加。实验上,以几种材料的散射光谱为例,通过改变探测条件、照明条件和材质比例,进行了散射光谱加和性的实验验证,并且针对实验结果进行了误差分析。单光源条件下的最大实验误差为2.64%,多光源条件下则为2.35%,加和计算偏差均在实验误差允许范围内。由此证明了材料的散射光谱具有加和性,不受组成的材质差异性、材质的面积比例组合多样性、以及实验条件多变性影响。散射光谱加和性的首次提出,不仅为基于散射光谱的复杂结构体的特征提取及识别研究提供了确切的理论依据和有效的分析方法,而且对相关的实验分析和应用研究有着重要的借鉴和参考意义。 相似文献
30.