| infotek |
2023-04-06 08:38 |
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。 hUO&rov3@ C<u<:4^H
成像示意图 -lDAxp6p 首先我们建立十字元件命名为Target J_ y+.p-
5 iwS55o 创建方法: #yi&-9B @kmOz( 面1 : Exu>% 面型:plane 6<>T{2b:(p 材料:Air >Ndck2@ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box nlsif 6L4<c+v_
*%;+3SV 辅助数据: :,[=g$CT: 首先在第一行输入temperature :300K, IqrT@jgN- emissivity:0.1; ~&\} qz3 io^L[ RjW<
H6a"K 面2 : DJ.n8hne 面型:plane SG@-b( 材料:Air |jT^[q(z 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ' En|-M5 &K@ RTgb 3d81]!n 位置坐标:绕Z轴旋转90度, X+LG Z4]D Fh0cOp(
BfOQ/k)) 辅助数据: H68~5lJY^] o{r<=X ysM 首先在第一行输入temperature :300K,emissivity: 0.1; |'ML
)`c[ 5N.-m;s %f'mW2 Target 元件距离坐标原点-161mm; ) u
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3I):W9$Qp 单透镜参数设定:F=100, bend=0, 位置位于坐标原点
o.|P7{v} @B#\3WNt ExKjH*gn 探测器参数设定: O~~WP*N
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M 在菜单栏中选择Create/Element Primitive /plane qGVf!R Nt'6Y;m!
":!7R<t g*]/HS>e<G ;:DDz 6#gS`X23Y 元件半径为20mm*20,mm,距离坐标原点200mm。 ]q pLaBD lNRGlTD% 光源创建: 8;\ 6>=yX6U1q^ 光源类型选择为任意平面,光源半角设定为15度。 F)n^pT HY!R | p()#+Xy 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。 9S_PZH (2uF<$7( 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。 eg Xbe)ld hI>vz"J =9yh<'583 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。 u/_TR;u=q {i#z<ttu 创建分析面: hteAuz4H w_ONy9 z&KrG 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。 v1O 1-aM ` G-V
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ATzFs]~K; 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。 *'to#_n&W
9,c_(%C FRED在探测器上穿过多个像素点迭代来创建热图 ?[VL
2dP0 X%rsa7H3J 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。 P+:DLex 将如下的代码放置在树形文件夹 Embedded Scripts, `~k`m{4.a PX/7 :D?
N(Sc!rX 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>)z]RB )eD9H*mq 绿色字体为说明文字, J:Idt}@z FKBI.}A?!' '#Language "WWB-COM" sOqT*gwr: 'script for calculating thermal image map G0~6A@> 'edited rnp 4 november 2005 38E
%]*5F l9t|@9 'declarations q,m+W='
Dim op As T_OPERATION B?
Z_~Bf& Dim trm As T_TRIMVOLUME q>rDxmP< Dim irrad(32,32) As Double 'make consistent with sampling Ms
3Sri Dim temp As Double bYUG4+rD Dim emiss As Double 6^e}^~| Dim fname As String, fullfilepath As String dt|| nF aY-7K._</ 'Option Explicit [9^lAhX %k'>bmJ Sub Main aqEmF 'USER INPUTS Jo''yrJpB nx = 31 /b7]NC% ny = 31 cDIZkni= numRays = 1000 FDal;T
minWave = 7 'microns U'aJCM maxWave = 11 'microns U#Wg"W{ sigma = 5.67e-14 'watts/mm^2/deg k^4 46##(4RF fname = "teapotimage.dat" =Hbf()cN) NHiac(&* Print "" xn=#4:f Print "THERMAL IMAGE CALCULATION" 7epil -v! ; detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 _#K?yP? R-YNg Print "found detector array at node " & detnode }qT{" *SC \ `;1[m srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 Tq?7-_MLC$ k+BY 3a Print "found differential detector area at node " & srcnode *,|x
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GetTrimVolume detnode, trm )FN\jo!!. detx = trm.xSemiApe 9ZNzC
i! dety = trm.ySemiApe ot0g@q[3 area = 4 * detx * dety lVCnu>8 Print "detector array semiaperture dimensions are " & detx & " by " & dety q|V|Jl Print "sampling is " & nx & " by " & ny UD=[::## 2HO2 'reset differential detector area dimensions to be consistent with sampling [y~kF?a pixelx = 2 * detx / nx {53|X=D64 pixely = 2 * dety / ny p:V1VHT, SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False (&SPMhs_|( Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 ~b@"ir+g4 tOX-vQ 'reset the source power _Q 'f^Kj SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) K~4bT= Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" +%H=+fJ2} #jJ0Mxg 'zero out irradiance array MOPHu
O{^ For i = 0 To ny - 1 jx{
fel For j = 0 To nx - 1 $_3)m irrad(i,j) = 0.0 :k-@w5( Next j +p[O|[z Next i x2TE[#>< "~S2XcR[ E 'main loop BiDyr EnableTextPrinting( False ) E
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|bu= T ypos = dety + pixely / 2 B}nT>Ub For i = 0 To ny - 1 P_5 G'[ xpos = -detx - pixelx / 2 l$[,V:N ypos = ypos - pixely Sk:x.oOZ 0"Euf41 EnableTextPrinting( True ) R;pIi/yDRe Print i TqSjL{l% EnableTextPrinting( False ) I:w+lchAMe ayh235>a( F|cli
< For j = 0 To nx - 1 )3 R5cq 65nK1W`i xpos = xpos + pixelx -?l`LbD C\Z5%2<Z 'shift source =J"c'Z>. LockOperationUpdates srcnode, True 6J_$dzw GetOperation srcnode, 1, op &O#1*y
Z op.val1 = xpos byTHSRt op.val2 = ypos q&}+O SetOperation srcnode, 1, op @^J>. g LockOperationUpdates srcnode, False jcjl q-x Q+/P>5O/ 'raytrace Z
+O<IF% DeleteRays Ms5R7<O.7 CreateSource srcnode uH(M@7"6_! TraceExisting 'draw _0ZU I^# }#2(WHf=< 'radiometry F(ZczwvR For k = 0 To GetEntityCount()-1 u/NcX If IsSurface( k ) Then +~*e B temp = AuxDataGetData( k, "temperature" ) F>5b[q6~4 emiss = AuxDataGetData( k, "emissivity" ) fQwLx
If ( temp <> 0 And emiss <> 0 ) Then $Yp.BE<} ProjSolidAngleByPi = GetSurfIncidentPower( k ) $e{[fmx frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) fdHFSnQ g irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi
^w&!}f+ End If 2kk; z0f o?cNH End If &;`E3$> R,BINp Next k <>Ha<4A
=E dPxJ`8 Next j g3yZi7b5FU MttFB;Tp Next i uRYq.`v, EnableTextPrinting( True ) 2[j`bYNe 4@Z!?QzW 'write out file gIIF17|Z fullfilepath = CurDir() & "\" & fname (9=E5n6o Open fullfilepath For Output As #1 3.g 4X?=zd Print #1, "GRID " & nx & " " & ny 6.$z!~8 Print #1, "1e+308" 0P{8s Print #1, pixelx & " " & pixely Rlm28 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 [@B!N+P5; `Q/\w1-Q maxRow = nx - 1 .JJ50p maxCol = ny - 1 f! )yE`4- For rowNum = 0 To maxRow ' begin loop over rows (constant X) ]m7x&N2 row = "" ie>mOsz For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) F- M)6&T row = row & irrad(colNum,rowNum) & " " ' append column data to row string 9'e<{mlM Next colNum ' end loop over columns CN}0( 2n J\p-5[E Print #1, row R3LIN-g( :XoR~syT Next rowNum ' end loop over rows sY?wQ: Close #1 Z}Q/u^Z Sfp-ns32%A Print "File written: " & fullfilepath fZLAZMrM Print "All done!!" ts("(zI1E End Sub (ip3{d{CT] ${}9/(x/^ 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: 1'iQlnMO@ }RY Pr J83C]2~7 找到Tools工具,点击Open plot files in 3D chart并找到该文件 `*`ZgTV GU 9p'E S v#,L8f 打开后,选择二维平面图: o>T+fBHE QFoCi&
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