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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。 s~6?p%
2] 8;5 UO,`T 成像示意图 Aq^1(-g 首先我们建立十字元件命名为Target 5$`i)}:s PxM]3Aoa 创建方法: 9} :n A%Pjg1(uX 面1 : l-Xxur5M' 面型:plane 17a'C 材料:Air 8*V3g_z 孔径:X=1.5, Y=6,Z=0.075,形状选择Box $-|`#|CBd '{5|[ t9Ht
54 辅助数据: J)6RXt*! 首先在第一行输入temperature :300K, +`r;3kH .. emissivity:0.1; ZL:nohB .8<bz4 ]uI#4t~ 面2 : t,]r% 面型:plane 1 xm8w$% 材料:Air 0V
uG(O 孔径:X=1.5, Y=6,Z=0.075,形状选择Box nr
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4N[8LC;MH 位置坐标:绕Z轴旋转90度, 7H:1c=U u}W R1u[ 2ro4{^(_ 辅助数据: qt=gz6! 'JsP9>) 首先在第一行输入temperature :300K,emissivity: 0.1; w^s|YF=c x=pq-&9>B p~Fc*g[! Target 元件距离坐标原点-161mm; JK4vQWy Smzy EMT h2#G 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 X-|Lg.s oyZ}JTl(Q Ob$|IH8. 探测器参数设定: 3R1v0 4eMNKIsvY$ 在菜单栏中选择Create/Element Primitive /plane Bd*:y qi ?B.>VnYZ/a /~yk cY
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F] 元件半径为20mm*20,mm,距离坐标原点200mm。 J+r\EN^9 MKq:=^ w 光源创建: p}$VBl$' ;i\m:8!; 光源类型选择为任意平面,光源半角设定为15度。 "a
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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。 AP&mr1_ h W\q 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。 tn&~~G~# [1K\
_ Lgw!S~0 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,bYzWsrPo
pbM~T(Y8 创建分析面: &sleV5V I]t ",s/j $Zf hQ5bat 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 99j^<) 6}zargu(; V+j58Wuf 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。
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FRED在探测器上穿过多个像素点迭代来创建热图 @}k5rcQ*/ ltRvNXx+] FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 Qxr&zT7f 将如下的代码放置在树形文件夹 Embedded Scripts, ^EY^.?Mg T<1*R>el ~ HFDX@m* 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 :!H]gC
4 h8OmO5/H 绿色字体为说明文字, Gxx:<`[ON YTP6m9hA+ '#Language "WWB-COM" s|L}wtc 'script for calculating thermal image map !cS
A|C 'edited rnp 4 november 2005 ,)-7f| '}3@D$YiM% 'declarations faH113nc Dim op As T_OPERATION yzJ
VU0s Dim trm As T_TRIMVOLUME Ni"n_Yun Dim irrad(32,32) As Double 'make consistent with sampling hZ6CiEJB Dim temp As Double 1Z-f@PoM Dim emiss As Double >(nb8T| Dim fname As String, fullfilepath As String JtA
tG% ]@YBa4}w 'Option Explicit $KDH"J P(B:tg Sub Main uXD?s3Wv 'USER INPUTS [AgS@^"sf5 nx = 31 /sHWJ?`&/, ny = 31 )w\E^ numRays = 1000 it?l! ~ minWave = 7 'microns 7S+_eL^ maxWave = 11 'microns B"sQ\gb%Q sigma = 5.67e-14 'watts/mm^2/deg k^4 Y v22,|: fname = "teapotimage.dat" o9&&u1`M/ rZ}y'A Print "" b3Nr>(Z<} Print "THERMAL IMAGE CALCULATION" 2 VgFP3 lxsBXX Zg detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 ,
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:7A Print "found detector array at node " & detnode Dxj&9Ra h,QC#Ak o srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 [wKnJu -U'3kaX5< Print "found differential detector area at node " & srcnode <*O~?=6p !@2L g GetTrimVolume detnode, trm ,D#ssxV detx = trm.xSemiApe -n.ltgW@ dety = trm.ySemiApe ~%)ug3%e area = 4 * detx * dety t\&u Print "detector array semiaperture dimensions are " & detx & " by " & dety E=PmOw7b Print "sampling is " & nx & " by " & ny sJA` A .7lDJ2 'reset differential detector area dimensions to be consistent with sampling }@VdtH pixelx = 2 * detx / nx jN.'%5Q?H pixely = 2 * dety / ny %=C49(/K_ SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False 2|Of$oMc Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 oUXi4lsSc -44{b<:D 'reset the source power RE*;_DF SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) u/W Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" 2|2'? ,LD[R1TU8 'zero out irradiance array
v E4ce For i = 0 To ny - 1 >\J({/ #O For j = 0 To nx - 1 WKjE^u irrad(i,j) = 0.0 TCb 7-s Next j 8HL$y-F Next i ?f}lYQzM S(bYN[U 'main loop s+9q`k^ EnableTextPrinting( False ) W+F{!dW f9R~RRz ypos = dety + pixely / 2 x}acxu 2H7 For i = 0 To ny - 1 AHg:`Wjv- xpos = -detx - pixelx / 2 }a=<Gl|I;w ypos = ypos - pixely T~=r*4 ui_nvD: EnableTextPrinting( True ) j%7N\Vb Print i P;B<R" EnableTextPrinting( False ) -1~-uE.~4d |s<IZ2z]}R ED0Vlw+1 For j = 0 To nx - 1 2;!,:bFb "t[9EbFL xpos = xpos + pixelx B;k3YOg B;[ai?@c(_ 'shift source ]Tv0+ Ao LockOperationUpdates srcnode, True :[hZn/ GetOperation srcnode, 1, op =IbDGw( op.val1 = xpos O7]p `Xi8 op.val2 = ypos j=&]=0F SetOperation srcnode, 1, op Rv-`6eyAA LockOperationUpdates srcnode, False 2h_XfY'3pX \w;d4r8x raytrace 25:[VH$:4 DeleteRays UaW,#P CreateSource srcnode >v
sy P TraceExisting 'draw j<BW/ p }p@])}8 'radiometry mgODJ For k = 0 To GetEntityCount()-1
>M2~BDZ If IsSurface( k ) Then 2 %`~DVo temp = AuxDataGetData( k, "temperature" ) ^(w%m# emiss = AuxDataGetData( k, "emissivity" ) 3I}(as{Rp If ( temp <> 0 And emiss <> 0 ) Then mNc?`G_R ProjSolidAngleByPi = GetSurfIncidentPower( k ) pJnT \~o frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) [i"6\p& irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi %3Ba9Nmid End If @ )bCh(u n5Coxvy1 End If <%_7% 5ov F$qn Next k 7?1[sPM *-.{->#Y Next j V8C62X HITw{RPrW Next i QsXy(w#F EnableTextPrinting( True ) X-lB1uq^ bi@z<Xm% 'write out file l0
Eh? fullfilepath = CurDir() & "\" & fname BXzn-S Open fullfilepath For Output As #1 4V6^@ Print #1, "GRID " & nx & " " & ny ApT8;F B Print #1, "1e+308" @k|V4 Print #1, pixelx & " " & pixely &d%0[Ui` Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 5]c\{G /i[1$/* maxRow = nx - 1 >TKl`O maxCol = ny - 1 [|5gw3y For rowNum = 0 To maxRow ' begin loop over rows (constant X) cs-wqxTX[$ row = "" B'AU~#d For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) Ad:}i9-x row = row & irrad(colNum,rowNum) & " " ' append column data to row string gpvzOW/ Next colNum ' end loop over columns =ws iC' k <EzYh Print #1, row g,k} nkIT VR'R7 Next rowNum ' end loop over rows t.s;dlx[@ Close #1 l KdY!j" _nn\O3TB Print "File written: " & fullfilepath z1AYXW6F Print "All done!!" -ff@W m End Sub K6z)&< ]%Db %A 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: KUE}^/%z iXgy/>qgT lTR/o 找到Tools工具,点击Open plot files in 3D chart并找到该文件 +";<Kd - MEI.wJZ aioN)V 打开后,选择二维平面图: Z=I+_p_G =O.%)|
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