| 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。 wu
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成像示意图 Xs03..S 首先我们建立十字元件命名为Target dwO fEYC %~rEJB@{ 创建方法: oD)x\ )t8 n,N->t$i 面1 : v{u3[c
面型:plane fSo8O 材料:Air ]OAU&t{ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 5Rbl.5.A >xWS>
73Dxf - 辅助数据: T:^.; ZY 首先在第一行输入temperature :300K, {X!vb emissivity:0.1; AHf 9H? _c5@)I~ }%g[1
#%( 面2 : ysaRH3M 面型:plane g2OnLEF]s 材料:Air pF;.nt) 孔径:X=1.5, Y=6,Z=0.075,形状选择Box u[a-9^&g E-A9lJWr &RR;'wLoQT 位置坐标:绕Z轴旋转90度, K\xz|Gq
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*5'8jC"2g 辅助数据: }7PJr/IuF `?VK(<w0q 首先在第一行输入temperature :300K,emissivity: 0.1; K,4Ig! 0'sZ7f<e7 YwVA].p@TI Target 元件距离坐标原点-161mm; \f,<\mJ#
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3u@,OE 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 $tlBI:ay1 :ez76oGyc Ey@^gHku\ 探测器参数设定: KOixFn1 2> a&m> 在菜单栏中选择Create/Element Primitive /plane *|&Y ,H? FPc`J
[Rj4=qq= bTs2$81[ c |0p'EQ &A:&2sP8 元件半径为20mm*20,mm,距离坐标原点200mm。 It*U"4lgi ju2H0AQ 光源创建: rCJ$Pl9R yY]x''K 光源类型选择为任意平面,光源半角设定为15度。 r^k+D<k[7 f2.=1)u. FM]clC;X? 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。 :7{GOx WUS%4LL( 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。 [3dGHf;miw m2SJ\1 J= 9>{fsy 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。 'IU3Xu[-. 4KH'S'eR 创建分析面: ^"Bhp:o2 r'noB<|e O%%Q./oh 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。 fhi}x( QRQ{Bq}#
&D<6Go/)_* 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。 NXD- bAlty}U FRED在探测器上穿过多个像素点迭代来创建热图 vhZXgp0X c{^1`(#? 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。 Boj R" 将如下的代码放置在树形文件夹 Embedded Scripts, oVK?lQ~y CUDA<Fm
olv&K(-ccI 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。 0 Rb3|te Q7amp:JFb 绿色字体为说明文字, (jKqwVs.: M|nLD+d~8 '#Language "WWB-COM" X$xf@|<a 'script for calculating thermal image map o^@#pU < 'edited rnp 4 november 2005 'qV lq5. ESviWCh0Fl 'declarations Cuylozj$& Dim op As T_OPERATION y/@Bhzc Dim trm As T_TRIMVOLUME 5H'Iul<Os Dim irrad(32,32) As Double 'make consistent with sampling S))B^).0- Dim temp As Double :TVo2Zm[@ Dim emiss As Double $c*fbBM(&n Dim fname As String, fullfilepath As String z<Z0/a2'1 wsdZwik 'Option Explicit E2l"e?AN~ ,7$&gx>2& Sub Main q AVypP?J 'USER INPUTS pZ $>Hh# nx = 31 YdV.+v(30 ny = 31 I!b"Rv=Nf- numRays = 1000 XN-1`5:4I minWave = 7 'microns _9-;35D_ maxWave = 11 'microns :xg
J2 sigma = 5.67e-14 'watts/mm^2/deg k^4 Cw^iA
U fname = "teapotimage.dat" 'h ? ,&Zp^ Print "" I3Co Print "THERMAL IMAGE CALCULATION" krGIE}5 CUB;0J( detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 J3+qnT8X ((?"2 }1r Print "found detector array at node " & detnode 1/bTwzR.g nls$
wE srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 2K3j3 |T gWro])3 Print "found differential detector area at node " & srcnode DI/d(oFv` Z9H2! Cp GetTrimVolume detnode, trm ZC$u8$+P detx = trm.xSemiApe uih8ZmRt dety = trm.ySemiApe Z$i?p;HnW area = 4 * detx * dety QP"5A7=m Print "detector array semiaperture dimensions are " & detx & " by " & dety 5k=04=Iyh# Print "sampling is " & nx & " by " & ny V6>{k_0{V pVl7]_=m 'reset differential detector area dimensions to be consistent with sampling 2./z6jXW_ pixelx = 2 * detx / nx zp4@T) pixely = 2 * dety / ny (7_ezWSl> SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False }.u[';q]S Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 (^T}6t3+4 I 8
? 'reset the source power RYl{89 SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) \k$cg~ Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" o8g]ho n\7>_ 'zero out irradiance array 8\)4waz$ For i = 0 To ny - 1 !#1UTa For j = 0 To nx - 1 l d%#.~Q irrad(i,j) = 0.0 >!PM5%G Next j qU&v50n Next i 8eCh5*_$ Oo!]{[}7 'main loop .|:(VG$MfI EnableTextPrinting( False ) D41.$t[ >7?Lq<H ypos = dety + pixely / 2 yqJ>Z%)hf For i = 0 To ny - 1 e*<pO@Uy xpos = -detx - pixelx / 2 Ug[0l) ypos = ypos - pixely x wfdJ(& K-(C5 "j_ EnableTextPrinting( True ) ](+u'8 Print i JBV
06T_4o EnableTextPrinting( False ) u3 X!O mmC MsBfL Q>z(!'dw For j = 0 To nx - 1 SbtZhg=S_ QVb{+`.7 xpos = xpos + pixelx '\pSUp dphWxB 'shift source Kk%
IN9 LockOperationUpdates srcnode, True 98|1K>C GetOperation srcnode, 1, op 80U(q/H%9 op.val1 = xpos 3! KyO)8 op.val2 = ypos HT_nxe`E SetOperation srcnode, 1, op I'J-)D` LockOperationUpdates srcnode, False |>JRJ"CFE REOWSs$' raytrace .%\R L/ DeleteRays h?QGJ^#8 CreateSource srcnode Vvn~G.&) TraceExisting 'draw ?+] %u?A>$Jn 'radiometry CT.hBz
-S For k = 0 To GetEntityCount()-1 yTWicW7i If IsSurface( k ) Then |UQGZ temp = AuxDataGetData( k, "temperature" ) rB =c emiss = AuxDataGetData( k, "emissivity" ) R|\kk?,u If ( temp <> 0 And emiss <> 0 ) Then m*AiP]Qu ProjSolidAngleByPi = GetSurfIncidentPower( k ) oC TSV frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) }F_=.w0 irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi Jk`0yJi$q End If C9%A?'` RHI?_gf& End If 5n=~l[O SQdK`]4 Next k Xq$9H@. tY`%vI [ Next j o3:h!(#G ZyrVv\' Next i #!jwn^yq EnableTextPrinting( True ) `$] ZT>& 8$ _8Yva"e 'write out file 7]
>z e fullfilepath = CurDir() & "\" & fname hIo^/_K Open fullfilepath For Output As #1 c*V/2"
5 Print #1, "GRID " & nx & " " & ny ?[8s`caK. Print #1, "1e+308" <[z9*Tm Print #1, pixelx & " " & pixely )4FW~o<i Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 kybDw{(}gc qD(dAU maxRow = nx - 1 k|rbh.Q maxCol = ny - 1 fp$U%uj For rowNum = 0 To maxRow ' begin loop over rows (constant X) 5Noy~; row = "" Ix.Y_} For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) $btk48a 7 row = row & irrad(colNum,rowNum) & " " ' append column data to row string )Q~K\bJf Next colNum ' end loop over columns \~:_h#bW ?fvK<0S` Print #1, row Gr|102 j'LO'&sQ( Next rowNum ' end loop over rows zRA,Yi4;+ Close #1 ^4
~ V/ 6$5SS# Print "File written: " & fullfilepath Z7=k$e Print "All done!!" o+T, O+i End Sub (+.R8 M~*o =t 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: 10..<v7 3W@ta1 4u]>$?X1_ 找到Tools工具,点击Open plot files in 3D chart并找到该文件 I*=
=I4qx &BRi& &f ,M9Hdm 打开后,选择二维平面图: q4KYC!b xY`$j'u
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