| 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。 72sD0)?A ]sz3]"2
成像示意图 )&era` e[ 首先我们建立十字元件命名为Target JGC=(; Zh5RwQNE~ 创建方法: B63pgPX _|72r}j 面1 : `28};B> 面型:plane |/gW_;( 材料:Air ELh8ltLY 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ;})5:\h r1ws1 rr=
J--m[X 辅助数据: $Vc~/> 首先在第一行输入temperature :300K, 7nbB^2 emissivity:0.1; s5RjIa0$7 K"<PGOF oG$)UTzGc 面2 : \#68;)+= 面型:plane pV6d
Id 材料:Air "cTncL 孔径:X=1.5, Y=6,Z=0.075,形状选择Box tbnH,* LZ@|9!KDw `mye}L2I 位置坐标:绕Z轴旋转90度, 0&ByEN99 DK0.R]&4(
o]IjK 辅助数据: mDh1>>K'~ E~<`/s 首先在第一行输入temperature :300K,emissivity: 0.1; !_2n dD<fn9t
8 6f2'o+ Target 元件距离坐标原点-161mm; 6<0n *& Y!6/[<r$~k
N_L,]QT? 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 vIvVq:6_3 c*d9'}E j@Qg0F 探测器参数设定: EBtLzbj Pmi#TW3X 在菜单栏中选择Create/Element Primitive /plane q9"=mO0J+ >:=|L%]s;\
?S?2 0 >zkRcm iut`7 Y32O-I!9u 元件半径为20mm*20,mm,距离坐标原点200mm。 ^$%Z!uz "uLjIIl 光源创建: ]a2W e` Q4t(@0e} 光源类型选择为任意平面,光源半角设定为15度。 %AF5= R{,ooxH\J .kTG[)F0b 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。 m~Ld~I" Gamr6I"K 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。 w@2Vts o`khz{SU: y80ykGPT\& 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。 zU6a'tP iAY!oZR(WT 创建分析面: :hGPTf W:i?t8y\y SM[Bv9|0 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。 `"vZ);i< TI y&&_p
8#R?]Uwq 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。 G0n'KB =Cqv= FRED在探测器上穿过多个像素点迭代来创建热图 ,n2i@?NHZ 4!`bZ`_Bw 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。 #G9 adK5 将如下的代码放置在树形文件夹 Embedded Scripts, Z?MoJ{.!?R DOm[*1@^
`ir3YnT+ 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。 n$m"]inX !BU)K'mj 绿色字体为说明文字, 0ZAj=u@O 89o)M5KQ '#Language "WWB-COM" h%d^Gq~ 'script for calculating thermal image map Fb2%!0i 'edited rnp 4 november 2005 ~
aZedQc $#o1MX 'declarations vUQFQ Dim op As T_OPERATION 3l!NG=R Dim trm As T_TRIMVOLUME 8OWmzY_= Dim irrad(32,32) As Double 'make consistent with sampling oFg5aey4 Dim temp As Double E]^5I3=O Dim emiss As Double _17|U K|N Dim fname As String, fullfilepath As String Bp AB5=M0 lp&!lb` 'Option Explicit
1S%k @^nu#R Sub Main bv?0.{Z 'USER INPUTS { }e^eJ nx = 31 ed~R>F> ny = 31 r$)$n&j numRays = 1000 ?`sy%G minWave = 7 'microns ph30'"[Z} maxWave = 11 'microns '|K.k6 sigma = 5.67e-14 'watts/mm^2/deg k^4 2V#6q,2 fname = "teapotimage.dat" vM0_>1nN gqiXmMm:9 Print "" gzfb zt}? Print "THERMAL IMAGE CALCULATION" Z-Wfcnk vx 0UoKX detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 a#(U2OP \d68-JS@~ Print "found detector array at node " & detnode .Oo/y0E^ =:$) Z srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 8Pmwzpk02 UOI^c Print "found differential detector area at node " & srcnode =t+ (' O8 RzUg& GetTrimVolume detnode, trm ??xlA-E detx = trm.xSemiApe )h"Fla dety = trm.ySemiApe c8Pb area = 4 * detx * dety 9]~PCZ2j Print "detector array semiaperture dimensions are " & detx & " by " & dety #tz8{o?ebN Print "sampling is " & nx & " by " & ny fGO*%)
$[e%&h@JR 'reset differential detector area dimensions to be consistent with sampling JLW$+62 pixelx = 2 * detx / nx Q]i[.ME pixely = 2 * dety / ny wixD\t59X SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False ZrcPgcF Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 ~= 9Vv twbcuaCTW 'reset the source power vl~%o@*_ SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) )kA2vX^=Z Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" s>J3\PC Gc}0]!nrW9 'zero out irradiance array c%yh(g For i = 0 To ny - 1 *^6k[3VY For j = 0 To nx - 1 XPVV+. irrad(i,j) = 0.0 =#'+"+lQ } Next j 5=.7\#D Next i z@n+7p`w VVN#
$ 'main loop aKOf;^@ EnableTextPrinting( False ) V%o#AfMI_ r'PE5xqF ypos = dety + pixely / 2 :7k`R62{ For i = 0 To ny - 1 QS%,7'EG xpos = -detx - pixelx / 2 =%)}) ypos = ypos - pixely kFnUJM$r c}8 -/P= EnableTextPrinting( True ) ?9,YVylg Print i jiOf')d5 EnableTextPrinting( False ) 6|i`@|# v(k*A: @Z,qu2~|! For j = 0 To nx - 1 BMe72 T+3k$G[e/ xpos = xpos + pixelx $<14JEU AwA1&mh 'shift source vr<)Ay LockOperationUpdates srcnode, True 7kOE/>P? GetOperation srcnode, 1, op w# xncH:1 op.val1 = xpos =CGD
~p` op.val2 = ypos !;ZBL;qY9 SetOperation srcnode, 1, op NH<Y1t LockOperationUpdates srcnode, False *C
tsFS~ qW+=g]x\ raytrace '"'D.,[W2 DeleteRays 6MrZ6dz^ CreateSource srcnode ZKZl>dDuh TraceExisting 'draw HIQ]"Hl :Xh_$4~^Y 'radiometry #IH<HL)t%e For k = 0 To GetEntityCount()-1 $(Z]TS$M& If IsSurface( k ) Then cA2^5'$$ temp = AuxDataGetData( k, "temperature" ) ab8oMi`z
emiss = AuxDataGetData( k, "emissivity" ) ce 7Yr*ZB If ( temp <> 0 And emiss <> 0 ) Then o",f(v&u% ProjSolidAngleByPi = GetSurfIncidentPower( k ) "u .)X3 frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) LuQ"E4;nY% irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi nNd`]F^U End If Kx(76_XD D|u^8\'. End If +,ZUTG V)_H E Next k !:]s M-cCt qAS70XjOF Next j >C*?17\ J3]qg.B%z Next i z v L>(R EnableTextPrinting( True ) <M5{.`o /Bg6z m 'write out file &hSnB~hi fullfilepath = CurDir() & "\" & fname ,(;p(#F> Open fullfilepath For Output As #1 yDu
yMt# Print #1, "GRID " & nx & " " & ny /8P4%[\ Print #1, "1e+308" -dc"N|. Print #1, pixelx & " " & pixely 2XETQ; 9 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 -z>Z0viA )V9Mcr*Ce6 maxRow = nx - 1 <Y}"D Yt maxCol = ny - 1 p[af[! For rowNum = 0 To maxRow ' begin loop over rows (constant X) %~~z9 6( row = "" iECC@g@a For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) :uU]rBMo row = row & irrad(colNum,rowNum) & " " ' append column data to row string 1{\,5U& Next colNum ' end loop over columns {LMS~nx X1
0"G~0 Print #1, row ,\m;DR1 ]sm0E@ 1 Next rowNum ' end loop over rows F=*BvI"+ Close #1 \U<F\i )"i>R
~* Print "File written: " & fullfilepath YQB]t=Ha Print "All done!!"
yv8dfl End Sub 5w,YBUp 9>.<+b(>!' 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: RB$ 8^# k?|zIu a dz;N;rIY 找到Tools工具,点击Open plot files in 3D chart并找到该文件 33v%e gne#v O+8ApicjTc 打开后,选择二维平面图: [r~rIb%Zj z}b U\3!
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