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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。 ,p{naT%R k3K*{"z 成像示意图 O uNPD q% 首先我们建立十字元件命名为Target s]]lB018O\ ,Qx]_gZ` 创建方法: ; [G: -L+kt_> 面1 : 7Xx3s@ 面型:plane f0vO(@I 材料:Air .fbY2b([ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box !(
>U3N )$RV) )X?oBNsj 辅助数据: !KMl'kswe: 首先在第一行输入temperature :300K, }f;WYz 5 emissivity:0.1; /5)*epF+ ^3[_4av }4p)UX>aWT 面2 : fX]`vjM{ 面型:plane b"uO BB 材料:Air MA,*$BgZ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box PChe w3 .u>[m. rCwE$5
b 位置坐标:绕Z轴旋转90度, hs[x\:})/ d\uN Q66 + 辅助数据: ?TeozhUY 5mQ@&E~#W 首先在第一行输入temperature :300K,emissivity: 0.1; pJx7S sW -=nk,cYn ffG<hclk Target 元件距离坐标原点-161mm; +@=V}IO ?V,q&=9 E{EO9EI 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 VxBBZsZO~ /i3JP} qmFG 探测器参数设定: -Y@tx fu- a;t}'GQGk 在菜单栏中选择Create/Element Primitive /plane Bhxs(NO &nP0T-T5y &EqLF Sp492W+ ka~_iUU4 (B>/LsTu 元件半径为20mm*20,mm,距离坐标原点200mm。 lhKn&U d!E_EoOi 光源创建: HD^#" |]4!WBK 光源类型选择为任意平面,光源半角设定为15度。 rz@qW2 }9+;-*m/ >=[uLY[aK 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 (iX8YP$ % Q]YB.n3 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。 ,c4HicRJ# QQBh)5F 8
MQq3 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。 0n{.96r0R H:@hCO[a 创建分析面: 7pm'b,J< xIGq+yd( 8cG?p 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.FU))lmD >\d&LLAe -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。 /?eVWCR 6;Z-Y>\c FRED在探测器上穿过多个像素点迭代来创建热图 BM<q;;pO 053bM)qW 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。 23wztEp{a 将如下的代码放置在树形文件夹 Embedded Scripts, 6nZ]y&$G-k e0TYHr)X>3 C(ij_> 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。 UGSZg|&6#* &"^F;z/ 绿色字体为说明文字, hZx&j{ p?i.<Z '#Language "WWB-COM" L}`/v]E"eU 'script for calculating thermal image map t(u2%R4<d 'edited rnp 4 november 2005 B?! L~J@p U?UU]>Q 'declarations M]s\F(*ib Dim op As T_OPERATION J!2Z9<q5 Dim trm As T_TRIMVOLUME $fmTa02q> Dim irrad(32,32) As Double 'make consistent with sampling e$Ksn_wEq Dim temp As Double P.y +jyu Dim emiss As Double F\ B/q Dim fname As String, fullfilepath As String w:t~M[kTW XwY,xg&o 'Option Explicit G-d7}Uz? 'z ?Hv Sub Main N d].(_ 'USER INPUTS >Zb!?ntN`t nx = 31 lU{)%4e` ny = 31 q&25,zWD numRays = 1000 Xs~'M/>
O minWave = 7 'microns QTy=VLk43 maxWave = 11 'microns l7|z]v- sigma = 5.67e-14 'watts/mm^2/deg k^4 ^%r6+ey fname = "teapotimage.dat" V&*IZt& ;|q<t Print "" w"j>^#8 Print "THERMAL IMAGE CALCULATION" %e~xO x #AJW-+1g.= detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 |Xt.[1 E_
wVAz3 Print "found detector array at node " & detnode y
bhFDx Sq5,}oT_{j srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点
@ap!3o8,9 ui%#f1Iq Print "found differential detector area at node " & srcnode $
VT) ]l,D,d81 GetTrimVolume detnode, trm EtcT:k?y detx = trm.xSemiApe 1SExlU dety = trm.ySemiApe Bgxk>Y area = 4 * detx * dety $e\s8$EO Print "detector array semiaperture dimensions are " & detx & " by " & dety g88k@<Y Print "sampling is " & nx & " by " & ny 7m2iL#5[ c,a8#Og 'reset differential detector area dimensions to be consistent with sampling 0Y8gUpe3P6 pixelx = 2 * detx / nx t\M6 d6 pixely = 2 * dety / ny &W45.2 SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False \lbH
Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 Ok!P~2J 1CC0]pyHX 'reset the source power //&3{B SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) }F>RIjj Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" i]ZGq7YJ% _}F&^ 'zero out irradiance array k8s)PN For i = 0 To ny - 1 evyjHc Cx For j = 0 To nx - 1 &]TniQH irrad(i,j) = 0.0 Ue}1(2.v Next j QRju9x Next i %r^tZ ;;l hkPMu@BI 'main loop zK6w0 EnableTextPrinting( False ) ^(q .f=I!a wq?"NQ?O< ypos = dety + pixely / 2 /4;mjE For i = 0 To ny - 1 && ]ix3 xpos = -detx - pixelx / 2 E-WpsNJ)X ypos = ypos - pixely RvR.t"8 :W)lt28_ EnableTextPrinting( True ) "09v6Tx Print i [A~?V.G EnableTextPrinting( False ) kXL0 -
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L =X'[r For j = 0 To nx - 1 k+"]; oXZWg~&l^ xpos = xpos + pixelx o(tJc}Mh+( vv)q&,<c 'shift source LVUA"'6V LockOperationUpdates srcnode, True t^&hG7L_m, GetOperation srcnode, 1, op .s\lfBo9 op.val1 = xpos H^'%$F?Ss op.val2 = ypos 1tY+0R SetOperation srcnode, 1, op 2sGKn
a LockOperationUpdates srcnode, False uihH")Mo eBa#Z1Z raytrace ]a IHd]B DeleteRays o}=*E CreateSource srcnode -3ePCAtXbe TraceExisting 'draw |OLXb+7X ;=joQWNDm 'radiometry XVNJK-B For k = 0 To GetEntityCount()-1 {>km]CG If IsSurface( k ) Then O1\4WG% temp = AuxDataGetData( k, "temperature" ) <oXBkCi0r emiss = AuxDataGetData( k, "emissivity" ) Ys.GBSlHG If ( temp <> 0 And emiss <> 0 ) Then 1V]ws}XW ProjSolidAngleByPi = GetSurfIncidentPower( k ) Fug4u?-n frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) B*:I-5 irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi f@`|2wG End If *SJ[~ o~'p&f End If zHKP$k8 1Xi>&;], Next k jOCV)V9} m=n79]b:N Next j $%$zZJ@/ j=pg5T Next i ]-t>F EnableTextPrinting( True ) NU_^*@k " O
r1 fC 'write out file |*48J1:1y fullfilepath = CurDir() & "\" & fname mxEe
-q Open fullfilepath For Output As #1 &IXmy-w Print #1, "GRID " & nx & " " & ny .(/HU Qn Print #1, "1e+308" E-^(VZ_Xj Print #1, pixelx & " " & pixely +\["HS7+'0 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 @_t=0Rc 0e&&k maxRow = nx - 1 ];CIo>
b_( maxCol = ny - 1 oAifM1*0 For rowNum = 0 To maxRow ' begin loop over rows (constant X) 'C}ku>B_r row = "" 7:g_:}m For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) G(?1 Urxi row = row & irrad(colNum,rowNum) & " " ' append column data to row string :ek^M ( Next colNum ' end loop over columns -uN{28;@ }Tk:?U{ Print #1, row 8a)4>B I~6(>Z{ Next rowNum ' end loop over rows ;HAvor=? Close #1 i`52tH y_ dLGHbeZ[( Print "File written: " & fullfilepath ogSDV Print "All done!!" .h4NG4FIF End Sub O`Qke
Z} f"gYXaVF+ 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: 4<tbZP3/6) EKO'S+~ tBkgn3w 找到Tools工具,点击Open plot files in 3D chart并找到该文件 CT_tJ &u^]YE{ |%5pzYe 打开后,选择二维平面图: /tG as +5I5
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