| infotek |
2022-01-24 09:30 |
十字元件热成像分析
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。
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成像示意图 ?MgUY)X 首先我们建立十字元件命名为Target tm#nU w enSXP~9w 创建方法: OeS\7 (}EB2V9Hh 面1 : eFL=G% 面型:plane /p+>NZ"b 材料:Air PGLplXb#[S 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 2IKnhBSV3 }L# _\
/qy-qUh3h 辅助数据: I~Zh@d% 首先在第一行输入temperature :300K, ;I}kQ!q emissivity:0.1; y6[If cN a6WI170^1 /q5v"iX]T 面2 :
SVB \ 面型:plane k|lcc^[0 材料:Air s1h/} 孔径:X=1.5, Y=6,Z=0.075,形状选择Box PSZL2iGj9V yl1gx lMg+R<$~I 位置坐标:绕Z轴旋转90度, Zy(W^~NT lJis~JLd`
4bw4cqY; 辅助数据: Db1pW=66: /5:bvg+ 首先在第一行输入temperature :300K,emissivity: 0.1; l33Pm/V2? Y!gCMLL ]A<~XIu Target 元件距离坐标原点-161mm; 6T#+V37 i* NH'o/
HY%i`]4X 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 w6W}"Uw kT'u1q$3Vo Gq }U|Z 探测器参数设定: N,;5{y1;J #~l(]h@
) 在菜单栏中选择Create/Element Primitive /plane "huFA|` >w^YO25q
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'j NwG= <U* R]btAu;Z 元件半径为20mm*20,mm,距离坐标原点200mm。 |]ZYa.+: :"IE 光源创建: 5yiK+-iTs -QmO1U 光源类型选择为任意平面,光源半角设定为15度。 y10h#&k X7i/fm{l' YGPy@-,E 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 \DD0s8 {'2@(^3 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 nC}6B).el x`dHJq`_g *]VFvh 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 6N;wqn '_/Bp4i 创建分析面: .b-f9qc= Bxfc}vC. d~`x )B( 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 XoCC/ Tp_L%F
9=V:&.L 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 Ffv`kn@ 6^"=dn6K FRED在探测器上穿过多个像素点迭代来创建热图 846$x$G4 ulkJR-""& FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 n>^Y$yy}! 将如下的代码放置在树形文件夹 Embedded Scripts, PV/77{' 43Qtj$F
%JHGiCv| 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。 ?$6Y2 X'`~s}vGO 绿色字体为说明文字, Tp-l^?O-p Yl#Rib '#Language "WWB-COM" kMOpi =Z1 'script for calculating thermal image map G1"zElug 'edited rnp 4 november 2005 >9(hUH LjUy*mxw 'declarations aP8H`^DFX> Dim op As T_OPERATION Rx);7j/5 Dim trm As T_TRIMVOLUME (
|PAx( Dim irrad(32,32) As Double 'make consistent with sampling LK, bO| Dim temp As Double 5KDGSo Dim emiss As Double HaYE9/xS Dim fname As String, fullfilepath As String
}f8Uc+ 00SbH$SU 'Option Explicit vt;{9\Y ALNc'MW! Sub Main '`XX
"_k3 'USER INPUTS M5*{ nx = 31 C_n9T{k ny = 31 u9}1)9 numRays = 1000 t0nI ('LX, minWave = 7 'microns 6C-/`>m maxWave = 11 'microns D!.+Y-+Xzu sigma = 5.67e-14 'watts/mm^2/deg k^4 z[cyA. fname = "teapotimage.dat" Ircp``g |/2y-[;: Print "" |iR T!
] Print "THERMAL IMAGE CALCULATION" }p!HT6 tZ hlJq-*6' detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 N^pJS6cJkl 9P~\Mpk Print "found detector array at node " & detnode Q`rF&)Q5 &%s8L\? srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 HE'2"t[a -Y*bSP)\ Print "found differential detector area at node " & srcnode Xy@7y[s] n< ud> JIb GetTrimVolume detnode, trm GF>'\@Th detx = trm.xSemiApe 9(5OeH6o? dety = trm.ySemiApe 't_[dSO area = 4 * detx * dety wmTq` XH) Print "detector array semiaperture dimensions are " & detx & " by " & dety Q"t<3-" Print "sampling is " & nx & " by " & ny z j/!In $zyIuJN# 'reset differential detector area dimensions to be consistent with sampling XvE9b5} pixelx = 2 * detx / nx B7]C]=${m pixely = 2 * dety / ny ;Wl+zw SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False aS pWsT Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 u6_@.a} @EDs~ lPv 'reset the source power RgGyoZ SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) qqu.EE Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" o.'g]Q<}UB GD:4"$)[o 'zero out irradiance array n#:N;T;\a For i = 0 To ny - 1 5e}A@GyC For j = 0 To nx - 1 CXO2N1~(J irrad(i,j) = 0.0 x)JOClLr Next j H.WE6 Next i .%^]9/4 ]_8qn'7 'main loop ph_4q@ EnableTextPrinting( False ) Cz W:L&t gt ";2,;X ypos = dety + pixely / 2 *0}3t<5 For i = 0 To ny - 1 ;?6No(/ xpos = -detx - pixelx / 2 hTM[8 ~<^ ypos = ypos - pixely Xu>r~^w=S 4<?8M vF EnableTextPrinting( True ) `KCh*i Print i c=
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" EnableTextPrinting( False ) |0\0a&tkPl ,i0b)=!o A^RR@D For j = 0 To nx - 1 p<&Xd}]"^W \/SQ,*O xpos = xpos + pixelx }?@rO`:EF+ K3' niGT 'shift source tBm_YP[ LockOperationUpdates srcnode, True NO0"* c ; GetOperation srcnode, 1, op |8.(XsN op.val1 = xpos DwV4o^J:l op.val2 = ypos HoLv`JA SetOperation srcnode, 1, op 8UMFq LockOperationUpdates srcnode, False ^47PLLRP >rP#ukr5 raytrace [F*4EGB DeleteRays q\q=PB6r CreateSource srcnode oP2fX_v1x TraceExisting 'draw ] )"u+ /\w)>0 'radiometry 3GmeD/6 For k = 0 To GetEntityCount()-1 TP}h~8 /; If IsSurface( k ) Then _6k*'aT~FK temp = AuxDataGetData( k, "temperature" ) ~-#yOu
,w emiss = AuxDataGetData( k, "emissivity" ) /Ux*u# If ( temp <> 0 And emiss <> 0 ) Then 1N\D5g3 ProjSolidAngleByPi = GetSurfIncidentPower( k ) ~+H"
-+ frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) bO;(bE m@ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi -@F fU2 End If Y9=(zOqv P1U*g! End If >F@qpjoQE Pa^A$fy\ Next k bC^(U`y 32 _oB_YL;,* Next j DS2)@ pCu!l#J Next i Ln.ZVMZ; EnableTextPrinting( True ) m$LVCB MzYavg` 'write out file 7JDN{!jT fullfilepath = CurDir() & "\" & fname S|zW^|YU Open fullfilepath For Output As #1 tURc bwV Print #1, "GRID " & nx & " " & ny BT_tOEL# Print #1, "1e+308" axk"^gps Print #1, pixelx & " " & pixely ]}mxY
vu_i Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 id?#TqD ow/57P maxRow = nx - 1 npDIX maxCol = ny - 1 #n For rowNum = 0 To maxRow ' begin loop over rows (constant X) phYDs9-K row = "" OI0B:() For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) k{AyD`'Q row = row & irrad(colNum,rowNum) & " " ' append column data to row string !$g+F(:(c Next colNum ' end loop over columns f&x0@Q/eON
I<=Df5M Print #1, row m7%C#+67 .la&P,j_L Next rowNum ' end loop over rows o+?rI
p Close #1 +zkm( 8yWoPm<A Print "File written: " & fullfilepath dp5f7>]:( Print "All done!!" >~\w+^2f8 End Sub l+wc'=] .9|uQEL 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: l+y}4k=/ nPkZHIxuD tVqmn 找到Tools工具,点击Open plot files in 3D chart并找到该文件 quo^fqS&a (vJ2z
=z 8V$3b?] 打开后,选择二维平面图: ~SjZk| fA! 6sB
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