照明工程学报
照明工程學報
조명공정학보
CHINA ILLUMINATING ENGINEERING JOURNAL
2015年
2期
83-88
,共6页
几何光学%非成像光学%三维同步多表面
幾何光學%非成像光學%三維同步多錶麵
궤하광학%비성상광학%삼유동보다표면
geometric optics%nonimaging optics%3D-SMS methods
为实现 LED 朗伯光源的矩形配光,提出了一种基于“脊肋”法的三维同步多表面非成像光学设计方法。该方法根据给定的辐照度分布,先由复合抛物面(CPC)完成初级配光,将朗伯光源±90°的发散角缩小到45°,再在二维平面生成一对“脊”线,然后向两侧生长出“肋”线,生成两个曲面框架,最后利用由 NURBS 曲面算法构建出两个自由曲面实现目标配光。两个自由曲面的引入提升了设计的自由度,但也大大增加了设计难度。将该方法应用到矩形均匀配光设计中,仿真结果表明:在远场接收面上得到一个较规则的方形轮廓且光束半发散角约为3.66°,考虑反射损失后其光效仍高达63%以上,平顶均匀度高于0.96。
為實現 LED 朗伯光源的矩形配光,提齣瞭一種基于“脊肋”法的三維同步多錶麵非成像光學設計方法。該方法根據給定的輻照度分佈,先由複閤拋物麵(CPC)完成初級配光,將朗伯光源±90°的髮散角縮小到45°,再在二維平麵生成一對“脊”線,然後嚮兩側生長齣“肋”線,生成兩箇麯麵框架,最後利用由 NURBS 麯麵算法構建齣兩箇自由麯麵實現目標配光。兩箇自由麯麵的引入提升瞭設計的自由度,但也大大增加瞭設計難度。將該方法應用到矩形均勻配光設計中,倣真結果錶明:在遠場接收麵上得到一箇較規則的方形輪廓且光束半髮散角約為3.66°,攷慮反射損失後其光效仍高達63%以上,平頂均勻度高于0.96。
위실현 LED 랑백광원적구형배광,제출료일충기우“척륵”법적삼유동보다표면비성상광학설계방법。해방법근거급정적복조도분포,선유복합포물면(CPC)완성초급배광,장랑백광원±90°적발산각축소도45°,재재이유평면생성일대“척”선,연후향량측생장출“륵”선,생성량개곡면광가,최후이용유 NURBS 곡면산법구건출량개자유곡면실현목표배광。량개자유곡면적인입제승료설계적자유도,단야대대증가료설계난도。장해방법응용도구형균균배광설계중,방진결과표명:재원장접수면상득도일개교규칙적방형륜곽차광속반발산각약위3.66°,고필반사손실후기광효잉고체63%이상,평정균균도고우0.96。
In order to achieve the rectangular irradiance distribution of LED lambertian source , a simultaneously multiple surface nonimaging optical design method is put forward which is called the “spine-rib” method.First it shrinks the divergence of the lambertian source from ±90°to 45°by a CPC, and then a couple of “spine” line is generated according to the prescribed irradiance distribution .Based on these lines there will be “rib” lines grown on to both side to get two surface frameworks .Finally, two freeform surfaces of the optical device are built by NURBS surface algorithm .The introduction of two freeform surfaces enhances the degrees of freedom which also improves the difficulty of design .Applied the method to the rectangular uniform light distribution design , simulation results show that : a square contour will be formed on the far -field receiver and give a 3.66°ray half divergence angle .When the reflection loss is fully considered , the light energy utilization is still more than 63%, the flat-topped uniformity is higher than 0.96.