| infotek |
2022-01-24 09:30 |
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。 p%j@2U 78 3a Z8
成像示意图 ]jM D'vg^b 首先我们建立十字元件命名为Target SR8[
7MU igz&7U8gg 创建方法: v3`J~,V< F[~qgS*; 面1 : 6~D:O?2 面型:plane Xr':/Qjf 材料:Air BhNwC[G?m 孔径:X=1.5, Y=6,Z=0.075,形状选择Box W;j*lII 1q/z&@+B
Qza[~6 辅助数据: p61"a,Xc 首先在第一行输入temperature :300K, "%0RR? emissivity:0.1; i"_JF-IbN en#W<"_" N[=nh)m7b 面2 : )v'3pTs2 面型:plane Vd|/]Zj 材料:Air w6Ue5Ix,! 孔径:X=1.5, Y=6,Z=0.075,形状选择Box +)ro
EJ_ ?jb7Oq#[ ?ILNp`k 位置坐标:绕Z轴旋转90度, R:OoQ^c 8CMI\yk
g"<kj" 辅助数据: Hs2L$TX 'L= g( 首先在第一行输入temperature :300K,emissivity: 0.1; BXLhi(.s $8X?|fV) Z;lE-`Z*(F Target 元件距离坐标原点-161mm; ISOPKZ#F *FOTq'%i
]}C#"Xt 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 OB5{EILej 'gQm%:qU3r %_}#IS1 探测器参数设定: 2{ }5WH -3haLdRk6 在菜单栏中选择Create/Element Primitive /plane Qb9) 1 _es>G'S
NOo&5@z;H Bxz{rR0XV &zUo", }9 {}vW= 元件半径为20mm*20,mm,距离坐标原点200mm。 DR^mT$ (S1$g ~t; 光源创建: i_f"?X;D babDLaC@ 光源类型选择为任意平面,光源半角设定为15度。 )HR'FlxOd awo=%vJ& ^> ZQ:xs@( 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 '[:].?M hg=\L5R 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 Y`\zLX"_m (#7pGGp*E nn5S 7! 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 oa47TqFt >0B[ 创建分析面: r=8]Ub[ pLrNYo*d V/J[~mN9 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 \-`L}$ QMHeU>
9sJbz=o]r 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。 6 3Kec pO=bcs8Z FRED在探测器上穿过多个像素点迭代来创建热图 C[ <&%=
G74<sD 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。 v]Pw]m5=U 将如下的代码放置在树形文件夹 Embedded Scripts, K\=bpc"Fy Ab8~'<F$B
F1gDeLmJ 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。 Cg8{NNeD W=PDOzB>K 绿色字体为说明文字, ';zLh $F;$-2 '#Language "WWB-COM" bAt!9uFn 'script for calculating thermal image map >PL/>
'edited rnp 4 november 2005 024*IoVZ 0Rrz
'declarations 5as';1^P&* Dim op As T_OPERATION +xFtGF) Dim trm As T_TRIMVOLUME l&U3jeW-o Dim irrad(32,32) As Double 'make consistent with sampling E8#y9q Dim temp As Double >p2v"X X Dim emiss As Double 3l<)|!f]g Dim fname As String, fullfilepath As String &A=d7ASN= &> }MoB 'Option Explicit vWjK[5
M% /O/u5P{J Sub Main iTqv= 'USER INPUTS LP#CA^*S nx = 31
p^\>{ ny = 31 plb'EP>e numRays = 1000 z&cfFx#h) minWave = 7 'microns 75I*&Wl maxWave = 11 'microns D;d'ss; sigma = 5.67e-14 'watts/mm^2/deg k^4 +-
c#UO> fname = "teapotimage.dat" y#YCc{K
[ K31Fp;K Print "" E5-8tHV Print "THERMAL IMAGE CALCULATION" 7o0ej# *l_1T4]S detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 \'BKI; (J$JIPF Print "found detector array at node " & detnode q35%t61Lc ax'Dp{Q srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 aH,0+ | };29'_.."x Print "found differential detector area at node " & srcnode nb(#;3DQ x\I9J4Q GetTrimVolume detnode, trm q\d'}:kfu detx = trm.xSemiApe "2Js[uf dety = trm.ySemiApe _aa3Qwx area = 4 * detx * dety )<-kS Print "detector array semiaperture dimensions are " & detx & " by " & dety ;)cSdA9 Print "sampling is " & nx & " by " & ny #^xiv/sV $o{f)'.>n 'reset differential detector area dimensions to be consistent with sampling Lr40rLx;u pixelx = 2 * detx / nx W53i5u( pixely = 2 * dety / ny |hOqz2| SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False ;l}TUo Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 q^O{LGN PM o>J|^ 'reset the source power DV{Qbe#In SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 7QQ1oPV Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" 6i=m1Yk r|?2 @VE 'zero out irradiance array &eK8v]|"W For i = 0 To ny - 1 kw}J~f2 For j = 0 To nx - 1 b3y@!_'c irrad(i,j) = 0.0 6i{W=$RQ Next j yBs Next i Jq/([
{jggiMwo.v 'main loop !{r Gt`y EnableTextPrinting( False ) 4+ yd/^S A%%WPBk{O ypos = dety + pixely / 2
7&l For i = 0 To ny - 1 }g>&l.2X xpos = -detx - pixelx / 2 GJ{]}fl ypos = ypos - pixely 7NoB ]U'KYrh EnableTextPrinting( True ) 1mf|:2, Print i oy/#,R_n% EnableTextPrinting( False ) Ur]5AJ U2@?!B[\d` H[!by)H For j = 0 To nx - 1 -DU[dU*~ +}X@{DB xpos = xpos + pixelx T9N /;3 spd>.Cm` 'shift source 0'VwObq LockOperationUpdates srcnode, True jJ|O]v$N GetOperation srcnode, 1, op 9J0m op.val1 = xpos C!~&c7 op.val2 = ypos O8 k$Uc SetOperation srcnode, 1, op WAkKbqJV LockOperationUpdates srcnode, False :;)K>g,b RUSBJsMB raytrace 8[2^`g DeleteRays ;`s/|v CreateSource srcnode [ V/*{Z TraceExisting 'draw Ko2{[%
4K)P Yk 'radiometry !XzRV?Ih; For k = 0 To GetEntityCount()-1 X;ijCZb3b If IsSurface( k ) Then a|lcOU temp = AuxDataGetData( k, "temperature" ) vKol@7%N emiss = AuxDataGetData( k, "emissivity" ) v34XcA If ( temp <> 0 And emiss <> 0 ) Then /m.6NVu7 ProjSolidAngleByPi = GetSurfIncidentPower( k ) ),dXaP[ frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) Fag%#jxI irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi O62H4oT End If VmV/~- <Z fZT=q^26 End If Pou`PNvH T+N%KRl Next k rjx6Ad/\ iI&J_Y{1a_ Next j +hV7o!WxC |f?tyQ Next i X0Xs"--} EnableTextPrinting( True ) 9.D'! K7U` 'write out file vX/~34o]\ fullfilepath = CurDir() & "\" & fname *siS4RX2 Open fullfilepath For Output As #1 :74)nbS Print #1, "GRID " & nx & " " & ny $iupzVrro Print #1, "1e+308" Abd&p N Print #1, pixelx & " " & pixely `=vL?w^QS Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 G8Ns? _l{GHz
maxRow = nx - 1 e>z3\4 maxCol = ny - 1 /i"L@t)\t For rowNum = 0 To maxRow ' begin loop over rows (constant X) FF)F%o+:w row = "" oCXBek?\ For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) 1^b-J0 row = row & irrad(colNum,rowNum) & " " ' append column data to row string egK,e?~ Next colNum ' end loop over columns mJ)o-BV ]fnc.^{ Print #1, row [8(e`6xePb `N]!-=o Next rowNum ' end loop over rows Ca0~K42~ Close #1 ^<.mUaP pg [F{T< Print "File written: " & fullfilepath gj0gs Print "All done!!" CES^
c-. k End Sub gH(,>}{^K t+|c)"\5h 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: `Q' 0l}, E#Smi507p fnN"a Z 找到Tools工具,点击Open plot files in 3D chart并找到该文件 {I&>`?7. )F8G q, 1I<D
`H% 打开后,选择二维平面图: &CV%+ j7?53e
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