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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。 n)?F
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#L 首先我们建立十字元件命名为Target o-i.'L)X +so o2cb 创建方法: D~ `YRbv =z/mI y< 面1 : q@"4Rbu6 面型:plane }lvP|6Y: y 材料:Air n,'AFb4AF 孔径:X=1.5, Y=6,Z=0.075,形状选择Box &I'F-F; (pxz#B4
(i~%4w= 辅助数据: $bC!T 首先在第一行输入temperature :300K, 2iINQK$ emissivity:0.1; ,`2xfVa- zs^\zCb8 qmeEUch` 面2 : NU\t3JaR 面型:plane $gtT5{"PN( 材料:Air Uz8C!L ">C 孔径:X=1.5, Y=6,Z=0.075,形状选择Box GKDG5u; c+M@{EbuN ]mU*Y:< 位置坐标:绕Z轴旋转90度, a}]@o" ^?VT y5yp
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f6uIF 辅助数据: /OtQk-E w8@|b} 首先在第一行输入temperature :300K,emissivity: 0.1; Oua/NF) {7s zo`U2 WW/m
/+ Target 元件距离坐标原点-161mm; O6 J<Lqgh (I 0t*Se
!Yi<h/: 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 5DBd
[u3 AhZ 8[p6C Jl) 探测器参数设定: J)&+y;. O g~"+IGp 在菜单栏中选择Create/Element Primitive /plane pKlT.<X7 '(:J|DN
KT?s\w QlXF:Gx"= R20GjWy= bL[W.O0 元件半径为20mm*20,mm,距离坐标原点200mm。 IY6S\Gn /[T8/7;_l 光源创建: cuk}VZ )_ u'k / 光源类型选择为任意平面,光源半角设定为15度。 pjn%CR`; w~-d4M NM zNs8\ 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 z,P7b]KVe wZb@VG}% 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 hfc!M2/w k/Ro74f= fJV VW 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 "Y0[rSz,UW >k-poBw 创建分析面: 'gH#\he[Dh 73`UTXvWU b=l}|)a 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 C#0Wo ^}L$[P
AVZ@?aJgF 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。 " <AljgF [uHI
6Q# FRED在探测器上穿过多个像素点迭代来创建热图 Xy<KvFy =w>QG{-N 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。 /_(Dq8^g@ 将如下的代码放置在树形文件夹 Embedded Scripts, ylJlICK gf>5xf{M
}y/t~f+ 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。 *?'T8yf^ S>Y?QQ3#wp 绿色字体为说明文字, ~h.B\Sc]Q 5+Ut]AL5 '#Language "WWB-COM" S22 ;g 'script for calculating thermal image map :b-(@a7> 'edited rnp 4 november 2005 ~?r6Ax-R 9-SXu lgu 'declarations ,{at?y* Dim op As T_OPERATION O}V2>W$ Dim trm As T_TRIMVOLUME mqw.v$> Dim irrad(32,32) As Double 'make consistent with sampling `#bcoK5 Dim temp As Double J-c7ZcTt Dim emiss As Double hT#mM*` Dim fname As String, fullfilepath As String F6/bq/s CcQ|0 'Option Explicit Hua8/:![+ x.RZ!V- Sub Main 6qf`P!7d]M 'USER INPUTS /-lmfpT nx = 31 ,sK-gw ny = 31 ?`$4ZDM numRays = 1000 tWuQKN`_ minWave = 7 'microns =t2epIr5 maxWave = 11 'microns E*vi@aI sigma = 5.67e-14 'watts/mm^2/deg k^4 hZy*E [i fname = "teapotimage.dat" /_8V+@im #s%$kYp 1 Print "" xuF_^ Print "THERMAL IMAGE CALCULATION" "mA/:8` Q 2~ a4ib detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 JI(|sAH [cq>QMW Print "found detector array at node " & detnode uwJkqlUOz <U*d
srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 Y/gCtSF paY%pU Print "found differential detector area at node " & srcnode >e%Po,Fg$ Cpl)byb GetTrimVolume detnode, trm s0CRrMk detx = trm.xSemiApe joq
;N]S dety = trm.ySemiApe y- YYDEl area = 4 * detx * dety .jU9{;[ Print "detector array semiaperture dimensions are " & detx & " by " & dety tp7fmn* Print "sampling is " & nx & " by " & ny BKk*<WMD 9z#IdY$a 'reset differential detector area dimensions to be consistent with sampling i2DR}%U pixelx = 2 * detx / nx 'J}lnt[V pixely = 2 * dety / ny `S|gfJ SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False N~Gh>{N Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 4p]Y`];U O7W}Z1G 'reset the source power 'CvZiW[_r SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) !jm
a -- Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" 4b)xW&K{ @)}U\= 'zero out irradiance array `#hy'S:e
For i = 0 To ny - 1 1EN5ZN, For j = 0 To nx - 1 ,=FYf|Z irrad(i,j) = 0.0 +_<#8v Next j R)v`ZF,/b Next i {221@ zcCq v'uQ'CiH 'main loop a[/p(O EnableTextPrinting( False ) K vgZx(. 2-]m#}zbP ypos = dety + pixely / 2 m~v
Ie c For i = 0 To ny - 1 -M4#dHR_! xpos = -detx - pixelx / 2 ${?Px
c{- ypos = ypos - pixely xucV$[f #Xc~3rg9 EnableTextPrinting( True ) "H({kmR Print i |laqy`D EnableTextPrinting( False ) ^m~=<4eX Rj8l]m6U9 V1+IqOXAIp For j = 0 To nx - 1 +1rJ ;G g$+3IVq& xpos = xpos + pixelx E'C[+iK6, (mzyA%;W 'shift source 4#o` -vcW LockOperationUpdates srcnode, True fRbVc GetOperation srcnode, 1, op N7[~Y2i op.val1 = xpos a P`;Nr= op.val2 = ypos BjShK+Y SetOperation srcnode, 1, op Lczcz"t LockOperationUpdates srcnode, False {*: C$"L giPyo"SD raytrace f"[C3o2P DeleteRays >uVG] CreateSource srcnode d00r&Mc TraceExisting 'draw u+]zi"k^s 4:K9FqU 'radiometry L
U7. For k = 0 To GetEntityCount()-1 rC'97`!K If IsSurface( k ) Then 2Bx\nLf/
K temp = AuxDataGetData( k, "temperature" ) 6K,AQ.=V2 emiss = AuxDataGetData( k, "emissivity" ) p4/D%*G^` If ( temp <> 0 And emiss <> 0 ) Then ]WS 7l@ ProjSolidAngleByPi = GetSurfIncidentPower( k ) ^*ZO@GNL frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) (LnKaf8 irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi
5!wa\)wY End If rtPQ:CaA)? ZqSczS7uf End If Alrk3I3{ P:Bg() Next k XX+4X*(o ?O28Q DUI Next j Q ml<JF rx%lL Next i (*#S%4(YX EnableTextPrinting( True ) Z/%>/ &n['#7 <(! 'write out file lLnD%*03 fullfilepath = CurDir() & "\" & fname rUlXx5f Open fullfilepath For Output As #1 /:B!hvpw Print #1, "GRID " & nx & " " & ny $[H3O(B0* Print #1, "1e+308" R+P1 +5 Print #1, pixelx & " " & pixely 0PZpE
"$X Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 xw`Pq6 7%C6gU!r maxRow = nx - 1 59GS: maxCol = ny - 1 hivWQ$6% For rowNum = 0 To maxRow ' begin loop over rows (constant X) }LOAT$]XI row = "" E<0Y;tR For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) -_B*~M/vV` row = row & irrad(colNum,rowNum) & " " ' append column data to row string cZA l.}/ Next colNum ' end loop over columns *!vwW
T oPl^tzO Print #1, row oH$4K8j @2V#bK Next rowNum ' end loop over rows "1Vuf<?C Close #1 1a`dB
~> G8j$&1`: Print "File written: " & fullfilepath T$!.
:v Print "All done!!" A3MVNz$wo" End Sub jruwdm^ 4/cUd=>Z 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: Ju#
- >] i,ga2{GnM NsPt1_Y8 找到Tools工具,点击Open plot files in 3D chart并找到该文件 mqQN*.8* h<JV6h :8 x= X"4Mj0) 打开后,选择二维平面图: -uX): h! icH\(
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