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    [轉(zhuǎn)載]2010年IODC的照明設(shè)計(jì)問(wèn)題 [復(fù)制鏈接]

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    離線mang2004
     
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    只看樓主 正序閱讀 樓主  發(fā)表于: 2011-05-14
    去年國(guó)際光學(xué)設(shè)計(jì)的照明問(wèn)題。 ;O}%_ef@  
    轉(zhuǎn)載自: http://iodc.info/illumination-design-problem/39-problems/58-2010-illumination-design-problem ;XMbjWc  
    有興趣的同好可以看看。光行壇有人參加嗎? S#8wnHq  
    vRpMZ)e  
    Problem description: I3uaEv7OZc  
    J^R))R=  
    Transfer maximum monochromatic flux from a 1-mm-square Lambertian source in air to an equal-etendue nonimmersed target. The target surface is rectangular with a 16:9 aspect ratio. The surface area of the target must be at least 4 mm². The target is defined such that only rays incident on the target surface at angles of θmax or less, relative to the surface normal, are considered to be within the phase space of the target, where the value of θmax is determined by the equal-étendue requirement. mnzamp  
    Cg |_ ) _w  
    Problem design degrees of freedom: W/<]mm~95  
    Can be any combination of idealized refractive and reflective components.  Jx9S@L`  
    Og4 X3QG  
    Assumptions and constraints vvU;55-  
    The only media allowed are air (index of 1) or dielectrics with refractive index in the range 1.33 - 1.59. "WdGY*r  
    R] tHd=kf  
    The coupling efficiency will be computed in the geometrical optics approximation using 100,000 pseudo-randomly generated rays. Optical losses produced by the following material characteristics will be included in the efficiency computation: r  /63  
    S$HzuK\f  
    Mirror reflectivity = 95% at all angles. E3<jH  
    TIR reflectivity = 100% at all angles. 22"M#:r$  
    Bulk absorption loss for all dielectric materials = 0.5% per cm. ,A[40SZA  
    Fresnel losses at air-dielectric interfaces = 2% at all angles. *]nha1!S  
    Fresnel losses between two different dielectric interfaces = 0.2% at all angles. 0(VH8@h`O  
    No Fresnel losses within a gradient index material. `C%,Nj  
    Minimum size of a component and edge thickness = 0.1 mm. %<6oKE  
    Minimum air space between components (including source) = 0.1 mm 8xJdK'  
    No volume or surface scattering. ^3B{|cqf  
    Light that finds its way back into the source is fully absorbed. FbO-K-  
     
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