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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。 Bvt@X N$[$;Fm: 成像示意图 -uh(?])H 首先我们建立十字元件命名为Target XhsTT2B KN"S?i]X 创建方法: Blq8H"3!: X,8<oX1r 面1 : Z0De!?ALV\ 面型:plane sE{ pzPq! 材料:Air 5'a3huRtV 孔径:X=1.5, Y=6,Z=0.075,形状选择Box mZIoaF>t "n:{!1VGw 2BCtJ`S` 辅助数据: ET];%~ ^ 首先在第一行输入temperature :300K, OGiV{9U emissivity:0.1; %zU`XVNN+ mJB2)^33a 0q\7C[R_ 面2 : c#N<"cy> 面型:plane 1009ES7* 材料:Air oUQ07z\C 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 5X.e*; ob_I]~^I?| |#l= 位置坐标:绕Z轴旋转90度, e"r)R8 fFjH "2WD d3^OEwe 辅助数据: jEXW HyiFy7j 首先在第一行输入temperature :300K,emissivity: 0.1; aQ j*KMc )EyI0R] 5 [#YE^[*qK Target 元件距离坐标原点-161mm; kqG0%WtQ CXtU"X H;aYiy 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 e4OeoQ@ > qW 1V85FG W(fr<<hL 探测器参数设定: J/);"bg_O QCPID: 在菜单栏中选择Create/Element Primitive /plane KNgH|5Pb '2zL.:~ ~](fFa{ fQ>4MKLw=d :T3/yd62N 0:KE@= 元件半径为20mm*20,mm,距离坐标原点200mm。 j<%])
,a?\MM9$ 光源创建: ]<DNo&fw %=j3jj[ 光源类型选择为任意平面,光源半角设定为15度。 <*H^(0 iAMtejw 8
6QE/M 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。 f^e6<5gdf t"j|nz{m 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。 /\mKY%kyh *s}|Hy ea=83 Zj 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。 CLKov\U\ 04!(okubyp 创建分析面: {+zJI-XN/ nA>sHy \F, DA"K_ 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。 !\[+99F# I>h<b_y gJ2
H=#M 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 3-40'$lE RANPi\] FRED在探测器上穿过多个像素点迭代来创建热图 <I;*[;AK vjViX<#(V 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。 !}3,B28 将如下的代码放置在树形文件夹 Embedded Scripts, gM;}#>6 f7}"lG]q h$C@j~ 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 NCA{H^CL
!a1i Un9 绿色字体为说明文字, PM$Ee #62R (g :p5Rl '#Language "WWB-COM" 4aZCFdc 'script for calculating thermal image map ?3sT"r_d@ 'edited rnp 4 november 2005 $7I]`Jt B'>*[!A 'declarations Oi:JiD= Dim op As T_OPERATION *.y' (tj[ Dim trm As T_TRIMVOLUME IKvBf'%- Dim irrad(32,32) As Double 'make consistent with sampling %IpSK 0<Sp Dim temp As Double D_|B2gdZY Dim emiss As Double (U.**9b; Dim fname As String, fullfilepath As String Wf02$c0#K {7Cx#Ewd 'Option Explicit ^>~dlS `!\ivIi^ Sub Main d+z[\i 'USER INPUTS ^[h2% c$ nx = 31 h\,5/ )Y ny = 31 X<Za9 numRays = 1000 ^6 /j_G minWave = 7 'microns <D /a l9 maxWave = 11 'microns [ET6(_=b sigma = 5.67e-14 'watts/mm^2/deg k^4 1JTbCS fname = "teapotimage.dat" m>Ux`Gp+ sz09+4h# Print "" % mn /> Print "THERMAL IMAGE CALCULATION" Ph7pd 9rj('F&1 detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 }(i(Ar- }F{=#Kqn^ Print "found detector array at node " & detnode vrcE]5(:s FuP}Kec srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 M1=_^f=&. Md(JIlh3 Print "found differential detector area at node " & srcnode *M!kA65' <A~GW
'HB GetTrimVolume detnode, trm m^$5K's& detx = trm.xSemiApe I{n;4? dety = trm.ySemiApe cIw
eBDl area = 4 * detx * dety #MTj)P, Print "detector array semiaperture dimensions are " & detx & " by " & dety o<4D=.g7D Print "sampling is " & nx & " by " & ny \ZnN D1A _%IqjJO{=r 'reset differential detector area dimensions to be consistent with sampling Fn,k!q pixelx = 2 * detx / nx :4;S"p pixely = 2 * dety / ny wkT;a&_ SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False ?R?Grw)`H Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 7~.ZE 2,AaP*, 'reset the source power gg8c7d:Q SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) G*\sdBW!k Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" jKt-~: F!CAitxd 'zero out irradiance array @%B4;c For i = 0 To ny - 1 Ex,JB + For j = 0 To nx - 1 ,+-? Zv 2 irrad(i,j) = 0.0 '0Zm#g Next j fNxw&ke8& Next i B
T7Id hPPB45^ 'main loop V<-htV EnableTextPrinting( False ) 6GOg_P aY j%w ypos = dety + pixely / 2 "]<}Hy For i = 0 To ny - 1 _<u;4RO(s xpos = -detx - pixelx / 2 .}p|`3$P ypos = ypos - pixely )VY10R)$ !QTPWA EnableTextPrinting( True ) LVmY=d> Print i D Q 5W6W EnableTextPrinting( False ) @KJV1t` &|z|SY]DL #NJ<[Gew For j = 0 To nx - 1 ?waebuj> e?vj+ZlS$f xpos = xpos + pixelx \1{_lynD PSEWL6=]N 'shift source V2QW\2@$ LockOperationUpdates srcnode, True 86{ZFtv GetOperation srcnode, 1, op ^N{X " op.val1 = xpos "3ug}k op.val2 = ypos YE_6OLW SetOperation srcnode, 1, op \4@a LockOperationUpdates srcnode, False EP0a1.C [)iN)$Mv raytrace +U=KXv DeleteRays \d5}5J]a&n CreateSource srcnode 5*XH6g F TraceExisting 'draw }#|2z}! H` Lu"EK 'radiometry Xr2 Wa For k = 0 To GetEntityCount()-1 `OLB';D If IsSurface( k ) Then fU`T\ temp = AuxDataGetData( k, "temperature" ) C,3T!\ emiss = AuxDataGetData( k, "emissivity" ) 6>lW5U^yA\ If ( temp <> 0 And emiss <> 0 ) Then XJ\_V[WA ProjSolidAngleByPi = GetSurfIncidentPower( k ) "Y(%oJS]D frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) No~6s.H irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi p`LL End If sOC|
B _]_L F[ End If d~,n_E$q; kw;wlFU; Next k v'$ykZ!Z XJ
_%! Next j @M9_j{A ? 9qAe Next i |/t K-c6J EnableTextPrinting( True ) @@; 1%z J:[3;Z 'write out file hN}5u"pS fullfilepath = CurDir() & "\" & fname Mi;Tn;3er Open fullfilepath For Output As #1 #-A5Z;TD. Print #1, "GRID " & nx & " " & ny }Uq/kei^P Print #1, "1e+308" .$OjUlzr-H Print #1, pixelx & " " & pixely ELD
+:b Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 ?SB5b , JfR kp maxRow = nx - 1 ={OCa1 maxCol = ny - 1 :
qr}M For rowNum = 0 To maxRow ' begin loop over rows (constant X) zcZ^s v> row = "" m/cx|b3hqv For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) Mru~<:9 row = row & irrad(colNum,rowNum) & " " ' append column data to row string J511AoQ{R Next colNum ' end loop over columns 3!1&DII4 cFe V?a Print #1, row qP@L(_=g p~ mN2x ] Next rowNum ' end loop over rows &(GopWR`e Close #1 yM W'-\ D_zcOq9 Print "File written: " & fullfilepath #dL5x{gV= Print "All done!!" K T%i,T End Sub P:jDB{ hLCsQYNDU 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: 9{T 8M aS2a_!f rE9Ta8j6 找到Tools工具,点击Open plot files in 3D chart并找到该文件
uT#Acg iz,]%<_PE #vnefIcBf 打开后,选择二维平面图: o$*bm6o Bi %Z2/
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