| infotek |
2023-04-06 08:38 |
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。 Q0!gTV U#+S9jWe
成像示意图 r`i<XGPJ% 首先我们建立十字元件命名为Target ss% ahs G|Ic6Sd 创建方法: _C&2-tnp DL|,:2` 面1 : f$iv+7<B^ 面型:plane U{RW=sYB~9 材料:Air ;)5d
wq 孔径:X=1.5, Y=6,Z=0.075,形状选择Box b3MgJT"mN >yg mE`g
/P5w}n 辅助数据: D.j'n-yw 首先在第一行输入temperature :300K, fg%I?ou emissivity:0.1; {~k/xM.- {IYfq)c y;yXOE_ 面2 : ]P(:z 面型:plane 8}\VlH] 材料:Air ?2%d;tW 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ._~_OVU K!5QFO4 R?(0:f 位置坐标:绕Z轴旋转90度, e4y dn C&,&~^_F
c#$B;? 辅助数据: 5iz]3]}%
b~Op1p 首先在第一行输入temperature :300K,emissivity: 0.1; 4g b2$" ! g6IG>) xSs);XO, Target 元件距离坐标原点-161mm; V2,54YE 1<fS&)^W
=;7gxV3; 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 n%"q> ixw3Z D(>+ M3o dyO( 探测器参数设定: wXMKQ)$( Ha1E /b]K
在菜单栏中选择Create/Element Primitive /plane f/~"_O% *j?tcxq
,@tkL!"9q <h4"^9hL /WRS6n r )ZUeHt}w 元件半径为20mm*20,mm,距离坐标原点200mm。 zu5'Ex`gQa sNc(aGvy 光源创建: ]{{A/ j\ d=o|)kV 光源类型选择为任意平面,光源半角设定为15度。 ^ ~:f02[D =MEv{9_ Yc3\NqQM 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。 G+stt(k: Y;8Y s&/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。 mTz %;+|L "^F#oo%L J0*hJ-/u 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。 J 05@SG': XAW$"^p 创建分析面: Ve*NM|jg t.$3?"60~ "~(qp_AI 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 btHN 'iA#lKG
&PVos|G 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 %@#+Xpa+ n0F.Um FRED在探测器上穿过多个像素点迭代来创建热图 &lbxmUeU V>ML-s9 FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 Xf!@uS6<X 将如下的代码放置在树形文件夹 Embedded Scripts, SNV~;@(h ( NWT/yBx
^e:C{]S= 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 v".q578
0B #no~g(!o 绿色字体为说明文字, 1rKKp h eQu%TZ(x-$ '#Language "WWB-COM" N-`Vb0;N 'script for calculating thermal image map dE19_KPm[j 'edited rnp 4 november 2005 h6<abT@I {*,~,iq 'declarations 6zh<PETa03 Dim op As T_OPERATION |x@)%QeC Dim trm As T_TRIMVOLUME mbB,j~;^6H Dim irrad(32,32) As Double 'make consistent with sampling uPKq<hBI Dim temp As Double 4)0 %^\p Dim emiss As Double r8g4NsRVtv Dim fname As String, fullfilepath As String pd{W(M78g 2_ M+akqy^ 'Option Explicit J ^gtSn^ =+5z;3 Sub Main oFM\L^Y?$$ 'USER INPUTS 7ksh%eV nx = 31 wmKM:`&[5 ny = 31 5I/wP qR[ numRays = 1000 JYuI~<: minWave = 7 'microns OzY55 maxWave = 11 'microns B?Ac sigma = 5.67e-14 'watts/mm^2/deg k^4 Py7!_TX fname = "teapotimage.dat" 6hDK;J J& @)s;u}H Print "" QR4rQu Print "THERMAL IMAGE CALCULATION" uw! h07Z.q ; detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 ]@X5'r" Vcn04j#Q Print "found detector array at node " & detnode F x,08 CvfXm srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 Rs_0xh ah<1&UG, Print "found differential detector area at node " & srcnode rMXIw 9ZvBsG) GetTrimVolume detnode, trm h/~:}Bof detx = trm.xSemiApe 5tPBTS<<"L dety = trm.ySemiApe U
|I>CDp area = 4 * detx * dety ?_mcg8A@@* Print "detector array semiaperture dimensions are " & detx & " by " & dety wKF #8Y Print "sampling is " & nx & " by " & ny piYv}4;:( Td#D\d\R 'reset differential detector area dimensions to be consistent with sampling 3jF#f'* pixelx = 2 * detx / nx }$M 2XF pixely = 2 * dety / ny 79 zFF SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False O@JgVdgf Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 P^m+SAAB u8ofgcFYE 'reset the source power Y `4AML SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) n\d`Fk Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" *Q2;bmIc .5Y%I;~v 'zero out irradiance array *9:oTN For i = 0 To ny - 1 [ZwZGAP For j = 0 To nx - 1 +mRFHZG irrad(i,j) = 0.0 V]b1cDx{ Next j (vte8uQe Next i _&S?uz m iku8T*&uc 'main loop xml@]N*D#E EnableTextPrinting( False ) 4d&#NP :}d`$2Dz ypos = dety + pixely / 2 JFaxxW For i = 0 To ny - 1 z0J$9hEg89 xpos = -detx - pixelx / 2 p.KX[I ypos = ypos - pixely d,=Kv rkhQoYZ[ EnableTextPrinting( True ) 8
v NgePn Print i 5,=Yi$x EnableTextPrinting( False ) [?3*/*V (]wi^dE B5J!&suX For j = 0 To nx - 1 WelB+P2 (H *-b4]/ xpos = xpos + pixelx DO<eBq\O g*b
4N_ 'shift source *]2LN$ LockOperationUpdates srcnode, True KDwz!:ye GetOperation srcnode, 1, op ?f v?6r op.val1 = xpos f.V;Hl, op.val2 = ypos gyH'92ck SetOperation srcnode, 1, op kN uDoo]z LockOperationUpdates srcnode, False 1|Y(XB^os( 6cof Zc$ 'raytrace }*Qd]\fy DeleteRays A.7:.5Cx' CreateSource srcnode 'B}pIx6k~ TraceExisting 'draw y7SOz'd jB }O6u[% 'radiometry CG'NC\x5 For k = 0 To GetEntityCount()-1 QFoZv+| If IsSurface( k ) Then G)gf +)W temp = AuxDataGetData( k, "temperature" ) 'G6TSl emiss = AuxDataGetData( k, "emissivity" ) 70_T;K6 If ( temp <> 0 And emiss <> 0 ) Then f uojf+i ProjSolidAngleByPi = GetSurfIncidentPower( k ) Vzy]N6QT{ frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) xO'I*) irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi sh.xp8^)^> End If JV'd!5P 1"46OCu{ End If o
D; \3K 6NA!L Next k KtJE 5A 1oZ+C# Next j T#Pz_
hAu }]vj"!?a Next i O;M_?^'W EnableTextPrinting( True ) KsYT3 l|`FW 'write out file FtN1ZZ"<* fullfilepath = CurDir() & "\" & fname j)\g0u6 Open fullfilepath For Output As #1 ~Wu Elns Print #1, "GRID " & nx & " " & ny Qu]0BVIe Print #1, "1e+308" 475yX-A Print #1, pixelx & " " & pixely Ku LZg Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 b{)('C$ Ff>Y<7CQ
v maxRow = nx - 1 x( w <U1 maxCol = ny - 1 jIE>t5 fy For rowNum = 0 To maxRow ' begin loop over rows (constant X) Wq)'0U;{$ row = "" ~J2-B2S! For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) DGY#pnCu row = row & irrad(colNum,rowNum) & " " ' append column data to row string L*tXy>&b. Next colNum ' end loop over columns ?>MD /l(l uZZ[`PA( Print #1, row e<5+&Cj Bir}X Next rowNum ' end loop over rows d;S:<]l' Close #1 6bnAVTL5 yP0P-8 Print "File written: " & fullfilepath F$r8hj` Print "All done!!" /og}e~q End Sub wI>JOV7 E E?v~6"& 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: ,2JqX>On>Y ;0E"4(S.q1 qh$D;t1= 找到Tools工具,点击Open plot files in 3D chart并找到该文件 =khjD[muC q<>2}[W *"
<tFQ 打开后,选择二维平面图: jbIWdHZ/US NOyLZa'
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