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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。 'kYV}rq;l F,4Q 成像示意图 6
rmK_Y 首先我们建立十字元件命名为Target *Z{W,8h*s XFd[>U<X 创建方法: BHU(Hd 1R,n[`}h 面1 : Tk+\Biq
面型:plane 7E|0'PPR 材料:Air (|bht 0 孔径:X=1.5, Y=6,Z=0.075,形状选择Box o#w6]Fmc 8/=[mYn`-
!y*V;J 辅助数据: m#8KCZS 首先在第一行输入temperature :300K, 1w\Y._jK emissivity:0.1; <pi q?:ac I,?bZ&@8 ZZlR:D 面2 : ~ocd4,d= 面型:plane E1VCm[j2 材料:Air $\a;?>WA" 孔径:X=1.5, Y=6,Z=0.075,形状选择Box n>iPAD #=$4U!yL Z$[A.gD4 位置坐标:绕Z轴旋转90度, xaSkn 8t6h^uQ .# M5L 辅助数据: >A1Yn]k 0.+iVOz+Y 首先在第一行输入temperature :300K,emissivity: 0.1; 6`+DBr oWJ}]ip s
fti[ Target 元件距离坐标原点-161mm; J-X5n 3I& t`DUY3>36 Y}|78|q* 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 <{cPa\ $_)f|\s %%-kUe 探测器参数设定: [N$@nA-d OTV)#,occ 在菜单栏中选择Create/Element Primitive /plane 89 SsS b }1$8)zH WG^D$L: zV2c`he%z FyY;F;4P wOa_" 元件半径为20mm*20,mm,距离坐标原点200mm。 33u7 }D=h"\_= 光源创建: f[ER`! -7+Fb^"L 光源类型选择为任意平面,光源半角设定为15度。 i!Ne<Q h@Hmo^!9J Lnj5EY er 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。 5hDE&hp 0,/[r/=jT 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。 {O"dj;RU c=Z#7?k=Uz /\\C&Px 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。 (d!vm\-PH ^Cak/5^K 创建分析面: q?t>!1c ''WX kW(8i}bg 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。
9PR&/Q
F5 +B&FZ4' @B[=`9KF[ 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。 XM_S" f|apk,o_ FRED在探测器上穿过多个像素点迭代来创建热图 <4>6k7W 5N[Y2 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。 )c!f J7o: 将如下的代码放置在树形文件夹 Embedded Scripts, B$lbp03z dA_s7), =lffr?#&B 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。 I4");T3 Nls|R 绿色字体为说明文字, @cXY"hP` +q2l,{|? '#Language "WWB-COM" 8EP^M~rv 'script for calculating thermal image map ?Dfgyz 'edited rnp 4 november 2005 a-kU?&*
y LAvAjvRc 'declarations T&{EqsI=B Dim op As T_OPERATION I)sCWC:Mq~ Dim trm As T_TRIMVOLUME )qxL@w. Dim irrad(32,32) As Double 'make consistent with sampling \C>I6{ Dim temp As Double ukPV nk Dim emiss As Double .vb*|So Dim fname As String, fullfilepath As String }2{%V^D)r aFbA=6 'Option Explicit 'DKP-R" R!- RSkB Sub Main !!P)r1=g 'USER INPUTS 3<'n>' nx = 31 ABx0IdOcI ny = 31 `zTVup& numRays = 1000 T}zOM%]] minWave = 7 'microns '\\J95*` maxWave = 11 'microns udw5A*Ls sigma = 5.67e-14 'watts/mm^2/deg k^4 v/(< fI^ fname = "teapotimage.dat" sbG3,'i) NL~} Print "" l3.HL> o Print "THERMAL IMAGE CALCULATION" :r!nz\%WW <oO^w&G detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 (m@({ wG-X833\( Print "found detector array at node " & detnode obY5taOw {E>kFeg srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 )5p0fw "S*lI^8Z! Print "found differential detector area at node " & srcnode l'mgjv~ {PdyKgM GetTrimVolume detnode, trm @VVBl I detx = trm.xSemiApe ;}1*M ! dety = trm.ySemiApe Gi?" area = 4 * detx * dety #6@7XC Print "detector array semiaperture dimensions are " & detx & " by " & dety ~
/]u72?rP Print "sampling is " & nx & " by " & ny UoBmS5 MejM(o_kk 'reset differential detector area dimensions to be consistent with sampling F0])g pixelx = 2 * detx / nx l3rr2t pixely = 2 * dety / ny <4D.P2ct SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False &n91f Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 ms`R^6Ra 0%#ZupN 'reset the source power
5Ta<$t SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) E.zY(# S Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" p0>W}+8fF ,_F@9Up 'zero out irradiance array (V!:6 For i = 0 To ny - 1 }f?$QSF For j = 0 To nx - 1 8t25wPlx irrad(i,j) = 0.0 bXmX@A$#Io Next j $oDc Next i )7f;FWI }(FF^Mh 'main loop DI"KH)XD EnableTextPrinting( False ) $3psSQQo z10J8Ms' ypos = dety + pixely / 2 1wAD_PI|BH For i = 0 To ny - 1 mmRxs1 0$ xpos = -detx - pixelx / 2 +#ufW%ZG ypos = ypos - pixely ObnQ,x( b\^X1eo
EnableTextPrinting( True ) ~XU%_Hz Print i ktF\f[ EnableTextPrinting( False ) ||yx?q6\h ^__';! e =[5F~--Tf For j = 0 To nx - 1 #$n >+lc Wz{,N07Q#{ xpos = xpos + pixelx _Fe%Ek1Yy 1zIX
$A 'shift source `-Y8T\ LockOperationUpdates srcnode, True HD%n'@E GetOperation srcnode, 1, op W=G8l% op.val1 = xpos OKi}aQ2R* op.val2 = ypos <DR$WsDG SetOperation srcnode, 1, op pgUp1goAU LockOperationUpdates srcnode, False wHuz~y6 E5iNuJj=f raytrace MxLg8,M DeleteRays F%< ZEVm CreateSource srcnode ^tFlA) TraceExisting 'draw 3QhQpPk), #IvHxSo& 'radiometry nixIKOnjC For k = 0 To GetEntityCount()-1 D]=V6l= If IsSurface( k ) Then PRal>s&f temp = AuxDataGetData( k, "temperature" ) `a6AES'w$ emiss = AuxDataGetData( k, "emissivity" ) 4|/}~9/ If ( temp <> 0 And emiss <> 0 ) Then <s=i5t
My5 ProjSolidAngleByPi = GetSurfIncidentPower( k )
%w#z frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 7u`:e,' irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi ~F"w End If &|fPskpy j4wsDtmAU End If I]ZksC 50e
vWD Next k ku)/
8Z`$ bfq%.<W Next j |R;` z2iWr Next i Nd
He:: EnableTextPrinting( True ) .6c
Bx {)I&&fSz 'write out file t>vr3)W fullfilepath = CurDir() & "\" & fname u
p zBd] Open fullfilepath For Output As #1 0DaKd<Scv Print #1, "GRID " & nx & " " & ny D}rnpwp{ Print #1, "1e+308" A;TNR Print #1, pixelx & " " & pixely ky{@*fg. Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 iU|X/>k? 4D[(X=FSU maxRow = nx - 1 p'kB1)~| maxCol = ny - 1 S;SI#Vg@ For rowNum = 0 To maxRow ' begin loop over rows (constant X) /~{fPS row = "" ~
Ofn&[G For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) xUPg~c0 row = row & irrad(colNum,rowNum) & " " ' append column data to row string 4|hfzCjMI Next colNum ' end loop over columns * Na8w'Q &<Fw Print #1, row bwK1XlfD.s g6h=Q3@ Next rowNum ' end loop over rows ,_bG'Hmt Close #1 L4<=,}KS Dc3bG@K*G Print "File written: " & fullfilepath \98|.EG Print "All done!!" pYj} End Sub ~Efi|A/ SQ`KR'E 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: ^x_+& } DjbVYH AQs_(LR 找到Tools工具,点击Open plot files in 3D chart并找到该文件 T9AFL;1 /<\do 1 H,)2Ou-Wn 打开后,选择二维平面图: Lmc"qFzK 6z5?9I4[
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