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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。
TY#pj bsWDjV~ 成像示意图 xtS0D^ 首先我们建立十字元件命名为Target =-uk7uZM FefS]G 创建方法: }?d
l.=eq w`Z@|A 面1 : rI]n4>k{ 面型:plane aj]%c_])( 材料:Air ;Uj=rS`Q 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 4d]T` j98>Jr\ s9YP
=)I 辅助数据: m}-~VYDj 首先在第一行输入temperature :300K, Dmk~t="Y emissivity:0.1; X@7e7 j0K}nS\ P V V~Kgy 面2 : 8:UV; 5@ 面型:plane !7kca#,X 材料:Air "(y| iS$^T 孔径:X=1.5, Y=6,Z=0.075,形状选择Box }qdGS<{ T EqCoeR h3L{zOff 位置坐标:绕Z轴旋转90度, D\GP+Ota Y]1b39O r \]iw v 辅助数据: 3Q(#2tL= R<-( 首先在第一行输入temperature :300K,emissivity: 0.1; 9k!#5_ M >/F,Z%!&q bQ2 '*T Target 元件距离坐标原点-161mm; {-Y% wM8<i t[cZ|+^] jJCd2O] 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 W 7Y5~%@ > jvi7 7L&=z$U@m 探测器参数设定: |Gh~Zup .B9rG~ 在菜单栏中选择Create/Element Primitive /plane 8MPXrc,9- k
GzosUt 7w{>bYP ~nG?> s|Acv4| V sIh,@b 元件半径为20mm*20,mm,距离坐标原点200mm。 !j?2HlIK+ {wx!~K 光源创建: ]\<^rEU M7;P)da 光源类型选择为任意平面,光源半角设定为15度。 !'^gqaF+ }-R|f_2Hp thjCfP 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。 Cuq=>J Rc H",*U 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。 $k|k 5cP8x />zE$)'M >;.'$- 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 e " f/ Q}M%
\v 创建分析面: |Tp>,\:5 G-]ndrTn Em8C +EM 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 kN*,3)T;} q8{)27f, +Q3i&"QB. 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 2\M^_x$N }Q?,O FRED在探测器上穿过多个像素点迭代来创建热图 /8i3 I5* W7lR54%| 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。 Kuz
/ 将如下的代码放置在树形文件夹 Embedded Scripts, 6WQT,@? kw>W5tNpf: #?Z>o16,u 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。 lV-b [Az<E3H" 绿色字体为说明文字, XP"lqyAi [wJM=`!W '#Language "WWB-COM" e:E:"elr] 'script for calculating thermal image map ZzNp#FrX" 'edited rnp 4 november 2005 a'zf8id oZkjg3 'declarations db%o3>>e Dim op As T_OPERATION w]hs1vch Dim trm As T_TRIMVOLUME 0?KY9 Dim irrad(32,32) As Double 'make consistent with sampling 9H9 P'lx9 Dim temp As Double WKib$(%f6 Dim emiss As Double #MbkU]) Dim fname As String, fullfilepath As String F(J6 XnQ Qx-/t 9`!Z 'Option Explicit |^^'GZ%a TzT(aWP" Sub Main XjL)WgQ{i 'USER INPUTS K]{Y >w nx = 31 '`#sOH ny = 31 t%$> numRays = 1000 ]3xb Q1 minWave = 7 'microns 59;p| maxWave = 11 'microns owDp?Sy}E sigma = 5.67e-14 'watts/mm^2/deg k^4 ~ [k0ay fname = "teapotimage.dat" #d,+87]\= b!C\J Print "" 1&JPyW Print "THERMAL IMAGE CALCULATION" 1PD{m{ ztcV[{[g detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 uOzol~TU) 50#iC@1 Print "found detector array at node " & detnode ;x/do?FbT i^9 ,. $<1 srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 !7C[\No( X}@^$'W Print "found differential detector area at node " & srcnode SJg4P4| &M p??{g GetTrimVolume detnode, trm hXBAs*4DV8 detx = trm.xSemiApe jlvh'y` dety = trm.ySemiApe V2As 5 area = 4 * detx * dety I!FIV^}Z( Print "detector array semiaperture dimensions are " & detx & " by " & dety eD4D<\* Print "sampling is " & nx & " by " & ny AgEX,SPP 0!<qfT
a 'reset differential detector area dimensions to be consistent with sampling )k)HQcfjD pixelx = 2 * detx / nx pZo:\n5o pixely = 2 * dety / ny 3q'["SS SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False >|{n";n& Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 hk6(y?# *3.K; Ic; 'reset the source power ZqtL4M~9 SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) z TYHwx Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" rC`pTN K/xn4N_UX 'zero out irradiance array muh[wo For i = 0 To ny - 1 &8p]yo2zO For j = 0 To nx - 1 =35g:fL irrad(i,j) = 0.0
Iw)}YZmn Next j H7{)"P]{f Next i Z3C]n,I .|\}]O` 'main loop /\L-y,>X EnableTextPrinting( False ) PHQ7 z$64Ep# ypos = dety + pixely / 2 /g/]Q^ For i = 0 To ny - 1 pco:]3BF6 xpos = -detx - pixelx / 2 6,wi81F,} ypos = ypos - pixely p.wed%O. #mT\B[4h EnableTextPrinting( True ) %y96]e1 Print i /thFs4 EnableTextPrinting( False ) 8jBrD1 `O+}$wP _3Kow{y\ For j = 0 To nx - 1 Q$Q>pV;uH VQ}N&H)` xpos = xpos + pixelx 4d x4hBd ]|m?pt 'shift source 5#275Hyv LockOperationUpdates srcnode, True 91f{qq=#J{ GetOperation srcnode, 1, op t=l@(%O 0_ op.val1 = xpos .(J~:U op.val2 = ypos 0r_3:#Nn SetOperation srcnode, 1, op $jkzm8{W LockOperationUpdates srcnode, False #%9t- 84f(B E raytrace
Z;ze{Vb DeleteRays NqlU? CreateSource srcnode 8}M-b6RV TraceExisting 'draw !n`9V^` ?^3Y+)} 'radiometry L`2(u!i J For k = 0 To GetEntityCount()-1 dI(1L~ If IsSurface( k ) Then nyoLrTs{ temp = AuxDataGetData( k, "temperature" )
9q/k,g emiss = AuxDataGetData( k, "emissivity" ) ,kQCCn] If ( temp <> 0 And emiss <> 0 ) Then (Sv=R(_s ProjSolidAngleByPi = GetSurfIncidentPower( k ) @vc9L frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) /wi*OZ7R irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi y&n-8L_ End If V3S"LJ a
S;z
YD End If
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?_o{ Next k <`V_H~Z $x/VO\Z{- Next j 6:Hd ` rff_=(?i Next i Od("tLIO}I EnableTextPrinting( True ) Y=?Tm,z4 ]."t 'write out file {i<L<Y(3 fullfilepath = CurDir() & "\" & fname *b4W+E Open fullfilepath For Output As #1 RRb>]oD Print #1, "GRID " & nx & " " & ny 2RU/oqmR Print #1, "1e+308" J4]tT pu"K Print #1, pixelx & " " & pixely 79z/(T+ Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 V8O-|7H$v *snY|hF maxRow = nx - 1 {zI>"%$u maxCol = ny - 1 N0pA ,& For rowNum = 0 To maxRow ' begin loop over rows (constant X) %oOSmt row = "" 3dx.%~c For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) n v
?u row = row & irrad(colNum,rowNum) & " " ' append column data to row string Ofc
u4pi Next colNum ' end loop over columns w5+(A_ !lL~#l:F Print #1, row gXj3=N(l OI,F,4e Next rowNum ' end loop over rows s-4qK(ml- Close #1 U6F7dT 2"QcjFW% Print "File written: " & fullfilepath l(pP*2 Print "All done!!" (sW$2a End Sub 7/HX!y{WP 8]i7wq#= 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: M_O) w^
' $WiUoS )+Yu7=S 找到Tools工具,点击Open plot files in 3D chart并找到该文件 Y%!k'\n[2 <M,<|Y*) ,z01*Yx 打开后,选择二维平面图: uf1s}/M k]9y+WC2
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