| 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。 o0 Ae*Y0 Gsb]e
成像示意图 PsLCO(26 首先我们建立十字元件命名为Target p.G7Cs B !XT:.+ 创建方法: _3hEYeh `d8TA#|` 面1 : _PIk,!< 面型:plane ZU`"^FQ3A 材料:Air D)Zv 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ;>~iCFk]? L-XTIL$$
4t":WutC 辅助数据: %^S1 fUwT 首先在第一行输入temperature :300K, LE;c+(CAU emissivity:0.1; ,0~=9dR 2,+H;Ypi! \m<*3eS 面2 : &\LbajP:+ 面型:plane wNlp4Z'[ 材料:Air >_@J&vC 孔径:X=1.5, Y=6,Z=0.075,形状选择Box [(C lvGx ?^dyQhb >(3y(1; 位置坐标:绕Z轴旋转90度, [lf[J&}X v[m>;Ubg&
VD4( 辅助数据: ]?^mb n ^#nAS2w7U 首先在第一行输入temperature :300K,emissivity: 0.1; 0:XmReO+k ||hd(_W8 b{A#P? Target 元件距离坐标原点-161mm; J? C"be= d/MMPge3
2n\EZ 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 O?@AnkOhn j9%=^ZoQj u!O)\m- 探测器参数设定: "zugnim r;-\z(h 在菜单栏中选择Create/Element Primitive /plane }q^CR(h (R
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\{( i9d.Ls 0VPa=AW N)QW$iw9 元件半径为20mm*20,mm,距离坐标原点200mm。 >6c{CYuT MZ0 J/@( 光源创建: )Ipa5i>t Lx.X#n.]T 光源类型选择为任意平面,光源半角设定为15度。 8IO4>CMkv 0ZO!_3m$r [l0>pHl@ 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。 ,a}+Jj{ YQ]W<0( 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。 \j4TDCs_[ &U:;jlST9 A," u~6Bn 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。 %k9GoX_ Ay[6rUO 创建分析面: [5H#ay LqNsQu"; U2;_{n*g% 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。 {D$+~lO Pwf":U)
EsdA%` 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 ?e0ljx; svN&~@l FRED在探测器上穿过多个像素点迭代来创建热图 #}o*1 G#UO>i0jy FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 i6aM}p< 将如下的代码放置在树形文件夹 Embedded Scripts, ^)TZHc2a[ A\LMmg
I=0`xF|4K- 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 5LR
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`ml '#Language "WWB-COM" BKi@c\Wb 'script for calculating thermal image map 1GE[*$vuq 'edited rnp 4 november 2005 wZ0RI{)s' a0~LZQ? 'declarations FG/1!8F Dim op As T_OPERATION )1N~-VuT Dim trm As T_TRIMVOLUME PY[nnoF"| Dim irrad(32,32) As Double 'make consistent with sampling Ejmpg_kux Dim temp As Double <v%Q|r Dim emiss As Double ''tCtG"
Xi Dim fname As String, fullfilepath As String "\3C)Nz? 6o6I]QL 'Option Explicit ;0FfP *mby fu0q Sub Main e w?4; 'USER INPUTS yvv]iRk< nx = 31 6/6M.p ny = 31 ^VOFkUp) numRays = 1000 =bgWUu\F minWave = 7 'microns ]lqLC maxWave = 11 'microns Ir#]p9:x sigma = 5.67e-14 'watts/mm^2/deg k^4 0~4Ww=# fname = "teapotimage.dat" Y7BmW+ 7H.3.j(L Print "" 6+!$x?5|NP Print "THERMAL IMAGE CALCULATION" 0fu*}v" @Z.BYC detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 x n?$@ 0Xb,ne
7 Print "found detector array at node " & detnode bI+/0Xx 2ca#@??R srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 7vTzY%v [n4nnmM Print "found differential detector area at node " & srcnode B`|f"+. A*G ~#v^ GetTrimVolume detnode, trm zG{P5@:.R detx = trm.xSemiApe xqs ,4bcbY dety = trm.ySemiApe M0yv=g area = 4 * detx * dety sKCYGt$ Print "detector array semiaperture dimensions are " & detx & " by " & dety ml@;ngmp. Print "sampling is " & nx & " by " & ny =WT&unw} bFjH*~
P 'reset differential detector area dimensions to be consistent with sampling ,oykOda:| pixelx = 2 * detx / nx ncqAof(/ pixely = 2 * dety / ny PriLV4? SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False t W+"/<U Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 /yHjds ":0u%E?s 'reset the source power }ZK%@b> SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) Bv<aB(c Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" tk]D)+{u&c 4C/G &w& 'zero out irradiance array ?r0rY? For i = 0 To ny - 1 !wN2BCSY@ For j = 0 To nx - 1 z%S$~^=b irrad(i,j) = 0.0 C~egF=w Next j P -NR]f Next i `;Ho<26 #9gx4U 'main loop FQJiLb._Z EnableTextPrinting( False ) ?a#Gn2 .W^B(y(tA ypos = dety + pixely / 2 9}%$j For i = 0 To ny - 1 Qo)Da}uo20 xpos = -detx - pixelx / 2 6se8`[ ypos = ypos - pixely GF6 o u?"="-^ EnableTextPrinting( True ) -'Ay(h Print i \_WR:?l EnableTextPrinting( False ) EjL]#,QR ^R=`<jx vhPlH0 For j = 0 To nx - 1 {.542}A >ei~:z]R xpos = xpos + pixelx Lo3N)~5 OHi.5 ( 'shift source _aR{B-E LockOperationUpdates srcnode, True 9wZ?")2 GetOperation srcnode, 1, op g3].STz6w op.val1 = xpos u"q56}Q?] op.val2 = ypos ||JUP}eP SetOperation srcnode, 1, op E/g"}yR LockOperationUpdates srcnode, False Asv]2> x Z/%FQ raytrace QuqznYSY{ DeleteRays OL>)SJj5 CreateSource srcnode M#;
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}8y For k = 0 To GetEntityCount()-1 T/\RViG3 If IsSurface( k ) Then n9xP8<w8
temp = AuxDataGetData( k, "temperature" ) JD#x+~pb,8 emiss = AuxDataGetData( k, "emissivity" ) iP0m1 If ( temp <> 0 And emiss <> 0 ) Then >*RU:X ProjSolidAngleByPi = GetSurfIncidentPower( k ) d!E_EoOi frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) ?D6uviQg irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi JcWp14~e End If Ww,\s5Uw Hl,{4%] End If )[ A-d(y= Yy88 5 Next k .Q%Hi7JMi lG)wa Next j *Jgi=,!m y6nP=g|')> Next i <%m YsaM EnableTextPrinting( True ) eCYPd-d "iA0hA 'write out file iX$G($[l( fullfilepath = CurDir() & "\" & fname {1)A"lQu Open fullfilepath For Output As #1 rW)h?, b Print #1, "GRID " & nx & " " & ny ,B[j{sE Print #1, "1e+308" -B;#pTG Print #1, pixelx & " " & pixely I.n,TJoz4J Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 Y~AjcqS %rylmioW> maxRow = nx - 1 =#2c
r:1 maxCol = ny - 1 j|t=%* For rowNum = 0 To maxRow ' begin loop over rows (constant X) qD{1X25O row = "" XVqOiv) For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) HU'Mi8xxy row = row & irrad(colNum,rowNum) & " " ' append column data to row string `gX|q3K\s Next colNum ' end loop over columns CIx(SeEF hZx&j{ Print #1, row 8M99cx*K ,AP0*Ln Next rowNum ' end loop over rows fzIs^(:fl Close #1 krUtOVI B&]`OO>O Print "File written: " & fullfilepath ij
?7MP Print "All done!!" 0
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:% End Sub #7]Jz.S 4yyw:" 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: z&6_}{2,] zMsup4cl =Kd'(ct 找到Tools工具,点击Open plot files in 3D chart并找到该文件 AELj"=RA "'U^8NA2 cUY- 打开后,选择二维平面图: jH<
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