infotek |
2020-11-18 10:58 |
十字元件热成像分析
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。 x+y!P Ma=6kX]
成像示意图 PUjoi@] 首先我们建立十字元件命名为Target `KJYm|@i +fP/|A8P 创建方法: l^UJes! <r+!hJ[s' 面1 : '0_j{ig 面型:plane q]i(CaKh 材料:Air hi3sOK*r;< 孔径:X=1.5, Y=6,Z=0.075,形状选择Box <K#'3&*$s V)1:LLRW
,8=`* 辅助数据: <f.>jjwFE 首先在第一行输入temperature :300K, [71#@^ye emissivity:0.1; jq("D, NrJ_6sjF0g gF,[u 面2 : yXTK(<' 面型:plane OSa}8rlr' 材料:Air I)XOAf$6 孔径:X=1.5, Y=6,Z=0.075,形状选择Box EAD0<I<>
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JQaHL! 位置坐标:绕Z轴旋转90度, /K,|k
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QlRoe|{ 辅助数据: O@r.> ,5\2C{ 首先在第一行输入temperature :300K,emissivity: 0.1; t8DL9RW' AvrL9D ~3'RW0 Target 元件距离坐标原点-161mm; (zs4#ja2, YXX36
:>P4L,Da] 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 mWli}j# Q&Z4r9+Z \]T=j#.S$ 探测器参数设定: *gd?>P7\0 crJ7pe9 在菜单栏中选择Create/Element Primitive /plane e8AjO$49 L$29L:
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fO^e+Mz 元件半径为20mm*20,mm,距离坐标原点200mm。 TvunjTpaj }XX~
W}M(\ 光源创建: M&qh]v gC n5Nan
光源类型选择为任意平面,光源半角设定为15度。 8_a$kJJ2 3XeXzPj I*A0?{ 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。 f0uUbJ5
<+AIt 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。 pg~zUOY aO.\Qe+j R^J.?>0 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。 7P<r`,~k- [G{rHSK5tQ 创建分析面: M.ZEqV+k {OB-J\7Y 2;r]gT~ 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。 qwq/Xcv lx\qp`w
?HrK\f3wWO 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。 b8J@K" RAIVdQ}.Z FRED在探测器上穿过多个像素点迭代来创建热图 -VS9`7k ,CJAzGBS 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。 ]g{hhP3> 将如下的代码放置在树形文件夹 Embedded Scripts, Jy \2I{I' Z?m
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LnP3z5d( 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。 0B=[80K;8 \Sg<='/{L; 绿色字体为说明文字, ;mEwQ Dc08D4
'#Language "WWB-COM" IQ ){(Y 'script for calculating thermal image map t?gJNOV 'edited rnp 4 november 2005 YiD-F7hf.* <&4nOt 'declarations B\\6# Dim op As T_OPERATION z< z*Wz Dim trm As T_TRIMVOLUME EQ4#fAM) Dim irrad(32,32) As Double 'make consistent with sampling ,zQo {. Dim temp As Double KX!i\NHz Dim emiss As Double l^.K'Q1~a Dim fname As String, fullfilepath As String ^NXcLEaP*< ujU=JlJ7dl 'Option Explicit !RS9%ES_? Bd{4Ae\_+g Sub Main _w5RK( 'USER INPUTS _@Y"$V]=Vt nx = 31 !)N|J$FU ny = 31 p8Iw!HE numRays = 1000 yQ9ZhdQS minWave = 7 'microns j`O7=- maxWave = 11 'microns !lAD
q|$ sigma = 5.67e-14 'watts/mm^2/deg k^4 }^9]jSq5 fname = "teapotimage.dat" #?dUv# P''X_1oMC Print "" O`WIkBV! Print "THERMAL IMAGE CALCULATION" blGf!4H Cezh l detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 d{f@K71* ^(ScgoXva Print "found detector array at node " & detnode Z%m-HE:k -_NC%iN#C srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 "
Ya9~6 EeB ]X24 Print "found differential detector area at node " & srcnode Ur^j$B} 2#3^skj GetTrimVolume detnode, trm 9}5K6aQ detx = trm.xSemiApe 1~J5uB4 dety = trm.ySemiApe ZPHXzi3j area = 4 * detx * dety P-CB;\ Print "detector array semiaperture dimensions are " & detx & " by " & dety I^D0<lHl~ Print "sampling is " & nx & " by " & ny Zk&h:c BYi)j6" 'reset differential detector area dimensions to be consistent with sampling 1j0-9Kg' pixelx = 2 * detx / nx G/vC~6x pixely = 2 * dety / ny 9AHSs,.t SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False t|V0x3X Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 *:_P8G; a8$kNtA 'reset the source power ubYG SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) ;
dd Q/ Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" JqCc;Cbd :~zv t 'zero out irradiance array 0)|Q6*E> For i = 0 To ny - 1 8!mc@$Z For j = 0 To nx - 1 WA$JI@g irrad(i,j) = 0.0 O oSb>Y/4 Next j -kpswP Next i 1zftrX~v!X -h#mn2U~3r 'main loop #?[.JD51l EnableTextPrinting( False ) |>2FRPK <?h%k"5 ypos = dety + pixely / 2 :!fG; )= For i = 0 To ny - 1 cCY/gEv xpos = -detx - pixelx / 2 Q7gY3flg ypos = ypos - pixely TeQNFo^_8 l&$$w!n0w EnableTextPrinting( True ) j>Ag\@2ME Print i w,1Ii}d9 EnableTextPrinting( False ) 9bJQT'<R 93O;+Z5J 9}29&O For j = 0 To nx - 1 ] asBd" pV(lhDNoQ xpos = xpos + pixelx re &E{ ZJ,cQ+fn 'shift source l4y{m#/ LockOperationUpdates srcnode, True CO?Xt+1hR GetOperation srcnode, 1, op 2;`=P5V op.val1 = xpos QHt4",Ij op.val2 = ypos AeuX Qt SetOperation srcnode, 1, op WO</Mw LockOperationUpdates srcnode, False 3WY$WRv ^Q+i=y{W 'raytrace SC &~s$P; DeleteRays :_kAl? eJ CreateSource srcnode :-`7Q\c} TraceExisting 'draw ]bi)$j.9s S8,Z;y 'radiometry q2rUbU_A( For k = 0 To GetEntityCount()-1 o4b~4h{% If IsSurface( k ) Then X"fh@. temp = AuxDataGetData( k, "temperature" ) ul f2vD emiss = AuxDataGetData( k, "emissivity" ) =*vMA#e If ( temp <> 0 And emiss <> 0 ) Then (Y%Q|u ProjSolidAngleByPi = GetSurfIncidentPower( k ) 9#d+RT frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 6
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irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi qU6nJi+-I End If ;Lm=dd@S: mqff]m End If @4$\
5%j X|D!VX>#! Next k W5L iXM Z?Hs@j Next j mo{MR:>) F}GPZ=T; Next i P^`duZ{T EnableTextPrinting( True ) OS|>t./U YW@#91. 'write out file ?E%ELs_Dl fullfilepath = CurDir() & "\" & fname [+m?G4[ Open fullfilepath For Output As #1 G`fC/Le Print #1, "GRID " & nx & " " & ny ph>7?3;t Print #1, "1e+308" 0[?ny`Y Print #1, pixelx & " " & pixely hN2:d1f0 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 73#x|lY E{^XlY maxRow = nx - 1 )}vNOE?X~ maxCol = ny - 1 jn >d*9u For rowNum = 0 To maxRow ' begin loop over rows (constant X) $;M:TpX row = "" h7*W*Bd For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y)
~=<}\a~ row = row & irrad(colNum,rowNum) & " " ' append column data to row string /2EHv.e` Next colNum ' end loop over columns vx_o(wof 8}X5o]Mv Print #1, row km^^T_ M/ W>VP'vn} Next rowNum ' end loop over rows mbnV[ Close #1 {!|}=45Z rqPFU6 Print "File written: " & fullfilepath r:&`$8$ Print "All done!!" OouPj@r End Sub P`s kg@>;(V& 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: *BuUHjTv XU/QA
[K w.,Q1\*rPp 找到Tools工具,点击Open plot files in 3D chart并找到该文件 YEkh3FrbwH 7\*FEjRM] %AOja+ 打开后,选择二维平面图: E0%~!b E9?phD
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