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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。 VpkkiN PG/xX
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成像示意图 ~<#!yRy>r 首先我们建立十字元件命名为Target RZ&T\;m,7 T"$yh2tSY 创建方法: ww"HV;i nZ2mY!* 面1 : 2oFHP_HVfu 面型:plane 9Iod[ x 材料:Air V<;w 孔径:X=1.5, Y=6,Z=0.075,形状选择Box mxV0"$'Fm _7"G&nZ0
AGxG*KuZ 辅助数据: zLiFk<G@Xi 首先在第一行输入temperature :300K, n++L
=&Wd emissivity:0.1; nZ 0rxx[V? ?xuhN
G@ !h0#es\ 面2 : JW4~Qwx 面型:plane IPhV|7 材料:Air 80M"`6 孔径:X=1.5, Y=6,Z=0.075,形状选择Box o4"7i 9+g gOA =i/7&gC 位置坐标:绕Z轴旋转90度, $*`=sV!r }G#TYF}
f|f9[h' 辅助数据: u!As?AD. Ok=RhoZZ 首先在第一行输入temperature :300K,emissivity: 0.1; $i+
1a0%n (*Jcx:rH .'y]Ea Target 元件距离坐标原点-161mm; (gv1f f@%H"8w!
<d GGH 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 VE<&0d< t@TBx=16 xi.L?"^/! 探测器参数设定: MW^,l=kqW) SG{> t*E 在菜单栏中选择Create/Element Primitive /plane #mNM5(o h$Z_r($b
f<V#Yc(U} 8T:|~%Sw ,&;#$ b5 ]F5qXF5 元件半径为20mm*20,mm,距离坐标原点200mm。 a+TlZE>8 8v},&rhPQq 光源创建: <wt#m`Za 8Q&hhmOnz 光源类型选择为任意平面,光源半角设定为15度。 v(?^#C>6W R)AFaP | `[<j5(T 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。 5h9`lS2 Lzzf`jN] 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。 n1n1} 3McBTa! W2VH? -Gw 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。 h\k!X/ D6trqB 创建分析面: Kf<-PA p!MOp-;- 2,c{Z$\kn 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 h2 2-vX xF'9`y^]!@
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(b2b 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 }+KSZ, ^mLZT* FRED在探测器上穿过多个像素点迭代来创建热图 #2thg{5 Ctpr. FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 .z
u0GsU= 将如下的代码放置在树形文件夹 Embedded Scripts, yIBT*,4 gdupG
aVI/x5p~ 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 ^zv0hGk 2 KLW#+vZ 绿色字体为说明文字, sgdxr!1?y -hav/7g '#Language "WWB-COM" \$Xo5f< 'script for calculating thermal image map cD&53FPXC 'edited rnp 4 november 2005 /
AFn8=9'^ PN ,pEk| 'declarations b
!FX]d1~k Dim op As T_OPERATION c <8s\2 Dim trm As T_TRIMVOLUME @EZ@X/8{& Dim irrad(32,32) As Double 'make consistent with sampling 3 8>?Z]V Dim temp As Double f>k<I[C< Dim emiss As Double c:0nOP Dim fname As String, fullfilepath As String kB-%T66\ T^3_d93}d 'Option Explicit MA\"JAP/ (9r\YNK Sub Main 8X":,s! 'USER INPUTS JivkY"= F nx = 31 .4c* _$ ny = 31 R[Q`2ggG numRays = 1000 (H/JB\~r minWave = 7 'microns 3+mC96wN maxWave = 11 'microns )UA$."~O sigma = 5.67e-14 'watts/mm^2/deg k^4 Ek|#P{! fname = "teapotimage.dat" LAG*H o2e aSG Print "" 6/^$SWd2 Print "THERMAL IMAGE CALCULATION" n?vw|'(} +cQGX5 K detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 }gQ FWT Z?k4Kb Print "found detector array at node " & detnode $]IX11.m vzl+0" srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 %n-:mSus MP/6AAt7=| Print "found differential detector area at node " & srcnode (uV~1 M{gtu'. GetTrimVolume detnode, trm /QDlm>FM4 detx = trm.xSemiApe 9%e&Z'l dety = trm.ySemiApe 2P9gS[Ub area = 4 * detx * dety &z[39Q{~ Print "detector array semiaperture dimensions are " & detx & " by " & dety 0j*-ZvE)30 Print "sampling is " & nx & " by " & ny %[(DFutJY+ >Q&E4j C 'reset differential detector area dimensions to be consistent with sampling _"
0VM> pixelx = 2 * detx / nx EgO=7?(pW pixely = 2 * dety / ny N1rBpt SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False Fy!uxT-\ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 qMT7g LB'1 OZ\ ]6]L 'reset the source power e573UB SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) iXN"M` nhm Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" jj^{^,z\ :7ej6 'zero out irradiance array >5C|i-HX For i = 0 To ny - 1 | k"?I For j = 0 To nx - 1 '`g#Zo irrad(i,j) = 0.0 JBa( O-T Next j b~?FV>gl Next i >SO !{ Sc
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-y_ 'main loop [iE% P^ EnableTextPrinting( False ) n_5m+
1N w'[lIEP 2$ ypos = dety + pixely / 2 Dohq@+] O For i = 0 To ny - 1 ;O=tSEe xpos = -detx - pixelx / 2 H\]ZtSw8- ypos = ypos - pixely S;DqM;Q \tf \fa EnableTextPrinting( True ) VfAC&3%M Print i tRU+6D
<w EnableTextPrinting( False ) P_11N9C vZj:\geV *,g|I8?%VD For j = 0 To nx - 1 g.yr)
LHt0 28qTC? xpos = xpos + pixelx F9rxm 7PG&G5 'shift source {@K>oaZ LockOperationUpdates srcnode, True K=x>%6W7b GetOperation srcnode, 1, op (.~#bl op.val1 = xpos 6t9Q,+nJ op.val2 = ypos wi'CBfr'z SetOperation srcnode, 1, op 0M^7#), LockOperationUpdates srcnode, False e|x1Dq 5Ug.J{d 'raytrace ^|yw)N]Q/ DeleteRays L{y%\:] CreateSource srcnode [DS.@97n TraceExisting 'draw k<p$BZ <SeK3@Gi 'radiometry h}PeXnRU For k = 0 To GetEntityCount()-1
;0G+>&C8 If IsSurface( k ) Then e>`+Vk^Jc temp = AuxDataGetData( k, "temperature" ) y8"8QH emiss = AuxDataGetData( k, "emissivity" ) >-EJLa If ( temp <> 0 And emiss <> 0 ) Then e1$T%?(&[ ProjSolidAngleByPi = GetSurfIncidentPower( k ) 5yPw[
EY frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) ,PH ;j_ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi ``*iK End If 0mcZe5RS Jq0aDf
f End If C3EQzr` "G. L)oD Next k zu8 J3Ipk-'lx Next j chw6_ctR> K
q;X(&Z Next i DC?U+ EnableTextPrinting( True ) I8*_\Ez z ((Y \vP 'write out file mx`QBJ fullfilepath = CurDir() & "\" & fname vv0A5p8H Open fullfilepath For Output As #1 bCWSh~ Print #1, "GRID " & nx & " " & ny -/ 5" Py Print #1, "1e+308" 9H^$cM9C Print #1, pixelx & " " & pixely ^0oOiZs Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 #mhR^60, \@")2o+ maxRow = nx - 1
DZPg|*KT maxCol = ny - 1 ^{f^%)X For rowNum = 0 To maxRow ' begin loop over rows (constant X) WdQR^'b$ row = "" 7p"4rL For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) y5>X0tT row = row & irrad(colNum,rowNum) & " " ' append column data to row string 0hJ,l. Next colNum ' end loop over columns .gZ1}2GF= 3zC<k2B Print #1, row ~kHWh8\b: =$kSvCjP Next rowNum ' end loop over rows 6ZvGD}/ Close #1 F3)w('h9c be^+X[ Print "File written: " & fullfilepath ,O`a_b] Print "All done!!" 2c)Ez? End Sub mKTE%lsH JU>F&g/| 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: l~",<bTc sVT:1 kI 4%refqWK 找到Tools工具,点击Open plot files in 3D chart并找到该文件 ,>
%=,x mz-sazgV l~mC$>f 打开后,选择二维平面图: 86 $88`/2 :'6vIPN5
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