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简介:本文是以十字元件为背景光源,经过一个透镜元件成像在探测器上,并显示其热成像图。 2CRgOFR Ey&gZ$|& 成像示意图 hQ}y(2A.XI 首先我们建立十字元件命名为Target _F`RwBOjs xM_+vN*( 创建方法: cH`ziZ<&m1 AvcN, 面1 : A>C8whx 面型:plane mJ'5!G 材料:Air RA*W Ys&xb 孔径:X=1.5, Y=6,Z=0.075,形状选择Box t_hr$ { .zo>,*:t ZjveXrx 辅助数据: >JHQA1mX 首先在第一行输入temperature :300K, J3y4D} emissivity:0.1; %b>Ee>rdD Su]p6B &+" )~2
+ 面2 : >{eGSSG0 面型:plane uF\ ;m. 材料:Air }{F1Cr 孔径:X=1.5, Y=6,Z=0.075,形状选择Box CD pLV: pwmH(94$0 Gg3<
}( 位置坐标:绕Z轴旋转90度, wZb77 .9!?vz]1 /JQY_>@W 辅助数据: )KKmV6>b ok/{ w 首先在第一行输入temperature :300K,emissivity: 0.1; Ja{[T .-}F~FES c=<5DC&p Target 元件距离坐标原点-161mm; '5}@#Mi ~#|Pe1Y HG&rE3@ 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 +&.wc;mi %<h+_(\h c52S2f7 探测器参数设定: :ywm 4) dReJ;x4 在菜单栏中选择Create/Element Primitive /plane p* tAwl OFn#C! %ql2 XAY t{Z:N']H 4_d'Uh&] .NT9dX 元件半径为20mm*20,mm,距离坐标原点200mm。 wg=-&- V]P%@<C 光源创建: CYZ0F5+t et}%E9 光源类型选择为任意平面,光源半角设定为15度。 !1xX)XD4y 8}{W.np_ DgKe!w$ 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 4+q3
Kw >tTu1#t 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 e#s-MK-Q M`tNYs]V _qsg2e}n 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 X^)vZL? L[O.]2 创建分析面: D}]u9jS1 0tEe
$9eK@ /s "Lsbe 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 Q3 yW#eD >M^4p [6f(3|" 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 p
#Y2v |6GDIoZ FRED在探测器上穿过多个像素点迭代来创建热图 @q+X:K5b rixt_}aE FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 um*!+Q 将如下的代码放置在树形文件夹 Embedded Scripts, ';3#t(J; o>Q=V0? EJ=ud9 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 ^(~%'f @y(<4kLz 绿色字体为说明文字, C!}t6 67A g.f6- '#Language "WWB-COM" C(}N*e1 'script for calculating thermal image map =jkiM_<h 'edited rnp 4 november 2005 dQJ)0!B i2X%xYv ^ 'declarations `}S;_g! Dim op As T_OPERATION Lb} $)AcC Dim trm As T_TRIMVOLUME pd}Cg'}X Dim irrad(32,32) As Double 'make consistent with sampling WnL7 A:sZ Dim temp As Double N^%7 Dim emiss As Double \JbOT%1 Dim fname As String, fullfilepath As String 1`)e}p& ][ 1
iKT 'Option Explicit R_2T" |:,i Sub Main &sg~owz 'USER INPUTS 0YO/G1O& nx = 31 %JPBD]&M ny = 31 Z\>mAtm numRays = 1000 rObg:(z&\ minWave = 7 'microns LGq
T$ O| maxWave = 11 'microns "I0F"nQ sigma = 5.67e-14 'watts/mm^2/deg k^4 ,dXJCX8so fname = "teapotimage.dat" L&hv:+3N GGez!?E% Print "" pYz\GSd Print "THERMAL IMAGE CALCULATION" )6*)u/x: 1h#e-Oyff detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 U o[\1) wf2v9.;X:< Print "found detector array at node " & detnode >,a$)z \EW<;xq srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点
B6.9hf GUC.t7! Print "found differential detector area at node " & srcnode Hv-f :P O G_S2Q @|Q GetTrimVolume detnode, trm jJyS^*.X detx = trm.xSemiApe MJ<jF(_= dety = trm.ySemiApe w\y) area = 4 * detx * dety b=XXp`h~a Print "detector array semiaperture dimensions are " & detx & " by " & dety $7*@TMX Print "sampling is " & nx & " by " & ny eXi}-~o Ogu";p( 'reset differential detector area dimensions to be consistent with sampling ffR<G&"n~b pixelx = 2 * detx / nx ?H!QV;ku pixely = 2 * dety / ny 2?@Ozr2Uh SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False L~E|c/ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 _*++xF1 ou=33}uO 'reset the source power a/xnf<(H SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) #vzt6x@* Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" yb) a w+gPU1|(r 'zero out irradiance array GDYFhH7H For i = 0 To ny - 1 R5=M{ For j = 0 To nx - 1 v(;n|=O irrad(i,j) = 0.0 ,c|Ai(U Next j [:8+ +#KD Next i q9(Z9$a(\ DFp">1@`PR 'main loop v+C%t!dx EnableTextPrinting( False ) RV),E:? x:+]^?}r ypos = dety + pixely / 2 ^/)%s 3 For i = 0 To ny - 1 gWfMUl xpos = -detx - pixelx / 2 u1`JvfLrL ypos = ypos - pixely ^00C"58A 10CRgrZ EnableTextPrinting( True ) o]<J&<WM Print i aSIoq}c( EnableTextPrinting( False ) R%6KxN)+@ dH)\zCt |LirjC4 For j = 0 To nx - 1 Z@0IvI $:D\yZ, xpos = xpos + pixelx byPqPSY K{0 gkORF 'shift source Bi7&yS5V LockOperationUpdates srcnode, True FiKGB\_] GetOperation srcnode, 1, op ]QJ7q} op.val1 = xpos [JKLlR op.val2 = ypos Q-KBQc SetOperation srcnode, 1, op G%>M@nYUE LockOperationUpdates srcnode, False ^bECX<,H x#fv<Cj4 raytrace krRnE7\m DeleteRays 3cc;BWvM CreateSource srcnode J7wIA3.O TraceExisting 'draw \S>GtlQbn NXOcsdcZu 'radiometry JZ/T:Hsh4 For k = 0 To GetEntityCount()-1 zT ")!Df>' If IsSurface( k ) Then hfpis== temp = AuxDataGetData( k, "temperature" ) W4=A.2[q emiss = AuxDataGetData( k, "emissivity" ) :XB^IyO-A If ( temp <> 0 And emiss <> 0 ) Then aa}U87]k ProjSolidAngleByPi = GetSurfIncidentPower( k ) P>'29$1' frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) ~)*uJ wW/a irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi ?N&s. End If !ezy
v` 4jW <*jM End If
pzb`M'Z?C Y?:"nhN Next k T>w;M?`9K d'[q2y?6N Next j lS?#(}a1) P?Kg7m W Next i E+J +fi EnableTextPrinting( True ) ]>[0DX]j _gQ_ixu 'write out file >^D5D%" fullfilepath = CurDir() & "\" & fname ,3Nna:~f Open fullfilepath For Output As #1 y<PQ$D) Print #1, "GRID " & nx & " " & ny lqvP
Dz Print #1, "1e+308" 0B"_St}3D Print #1, pixelx & " " & pixely <GSp%r Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 eE@7AM r ?z}TtDp maxRow = nx - 1 "p[3^<~uQ maxCol = ny - 1 OV`li#H For rowNum = 0 To maxRow ' begin loop over rows (constant X) ?L6wky{ row = "" XoGOY|2`6 For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) ie7P^:T|+ row = row & irrad(colNum,rowNum) & " " ' append column data to row string yh{U!hG Next colNum ' end loop over columns S2EV[K8# k=9k4l Print #1, row L$ZsNs+ \zhCGDm1_ Next rowNum ' end loop over rows 68~5Dx Close #1 f/U~X; R| XD#bG Print "File written: " & fullfilepath FBa-gm<9 Print "All done!!" >J{e_C2ZS End Sub 0@&/W-VXg A@e!~ 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: j|@8VxZ #I#_gjJkx NT{'BJ 找到Tools工具,点击Open plot files in 3D chart并找到该文件 g`4WisL1n |][PbN
D I(<Trn 打开后,选择二维平面图: L;fz7?_j $F6GCM3Cx
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