| 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。 RF6]_-
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成像示意图 MW^FY4V1m 首先我们建立十字元件命名为Target aVVE2:M SK/}bZ;f 创建方法: cuG;1,?b sX>|Y3S\U 面1 : 8Dxg6> 面型:plane p}GTOJT} 材料:Air P*Jk 8MK#G 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ^cW{%R>XY /;Cx|\
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I# 辅助数据: ;CL^2{ 首先在第一行输入temperature :300K, uVZm9Sp emissivity:0.1; +LWgby4q N8r+Q%ov FDFVhcr 面2 : P:'y}a- 面型:plane Tnf&32IA 材料:Air e6gj'GmY 孔径:X=1.5, Y=6,Z=0.075,形状选择Box -jTK3&5 o'P[uB/ XxB% 位置坐标:绕Z轴旋转90度, 8BS$6Pa \q-["W34
+C`vO5\0 辅助数据: Y'6P ~C;v ONcS,oHW 首先在第一行输入temperature :300K,emissivity: 0.1; j\.pS^+ JKXIxw>q kc2E4i Target 元件距离坐标原点-161mm; ER]C;DYX b;mpZ|T.
3@;24X 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 qP%[nY a 6fH *2E <&M5#:u 探测器参数设定: 9fSX=PVRmQ l`K5fk 在菜单栏中选择Create/Element Primitive /plane .W-=V zWX "Jyb?5
#DTBdBh?I "0"8Rp&V| BxxqzN+ 5i3nz=~o 元件半径为20mm*20,mm,距离坐标原点200mm。 ybm&g( -\ H&ZsMML/% 光源创建: f7]C1!] ##NowO 光源类型选择为任意平面,光源半角设定为15度。 0ipYXbC !jJH}o/KW lFM'F [-?- 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 %eqL)pC] Q#$dp 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。 YC~kq? (e{pAm 1T7;=<g` 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。 \?.M1a[ N(&/ Ud 创建分析面: nr9cG/" ;,_c1x/F ]
i\a[3 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。 m`ab5<%Gn t3$+;K(
=gr3a,2 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。 &5wM` )/<\|mR FRED在探测器上穿过多个像素点迭代来创建热图 *(@[E b<rJ@1qtJ 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。 v:]
AS: 将如下的代码放置在树形文件夹 Embedded Scripts, =l9H]`T/ 80ms7 B
vV9q5Bj: 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。 SA$1rqU= cS1BB#N0 绿色字体为说明文字, wq&TU'O lN^} qg>< '#Language "WWB-COM" [HhdeLOX 'script for calculating thermal image map rRZ ,X% 'edited rnp 4 november 2005 6|:]2S mI~k@ !3 'declarations mM7S9^<UH Dim op As T_OPERATION ^Ru/7pw5 Dim trm As T_TRIMVOLUME ztS'Dp}q< Dim irrad(32,32) As Double 'make consistent with sampling G" Fd]' Dim temp As Double GzUgzj|BN~ Dim emiss As Double ^m:?6y_uw Dim fname As String, fullfilepath As String BqKh&m \YBY"J 'Option Explicit uB:utg 4RqOg1 Sub Main uU]4)Hp 'USER INPUTS x~tG[Y2F? nx = 31 OC]_b36v ny = 31 ^25[%aJI numRays = 1000 ~T[m{8uh minWave = 7 'microns [
Q6v #I maxWave = 11 'microns `QlChxd sigma = 5.67e-14 'watts/mm^2/deg k^4 b|*A%?m fname = "teapotimage.dat" BI] %$rq Ot]PH[+ Print "" g.N~81A Print "THERMAL IMAGE CALCULATION" vF K&.J n'JwT!
A detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 q<b;xx pFg9-xd% Print "found detector array at node " & detnode *qE[Y0Cd xla9:*pPn srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 p'
FYK| Hdh'!|w Print "found differential detector area at node " & srcnode /tf}8d h30~2]hH GetTrimVolume detnode, trm '7{0k{ detx = trm.xSemiApe }IGr%C(3% dety = trm.ySemiApe +S:(cz80V area = 4 * detx * dety $vdGkz@6 Print "detector array semiaperture dimensions are " & detx & " by " & dety >w?O?&Q$ Print "sampling is " & nx & " by " & ny SA|f1R2uS 4
|N&Y 'reset differential detector area dimensions to be consistent with sampling )A['+s pixelx = 2 * detx / nx _Ucj)Ud k pixely = 2 * dety / ny m4*Rr SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False (yAQm pp Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 LRv-q{jP; HQ+:0"B 'reset the source power w8(qiU SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) ]v 6u Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" s"G6aM n5%rsNxg 'zero out irradiance array d7u"Z5t For i = 0 To ny - 1 #uT-_L}sw For j = 0 To nx - 1 l\*} irrad(i,j) = 0.0 '@Y@H, Next j gRKmfJ*u Next i [Qv% y2^r.6"O 'main loop Xt /muV EnableTextPrinting( False ) Z|
+/Wl-h xk}YeNVj ypos = dety + pixely / 2 l9q
ygh For i = 0 To ny - 1 bI=\n)sEz xpos = -detx - pixelx / 2 "S^;X
@#v ypos = ypos - pixely 8Hs>+Udl s&M6DFlA EnableTextPrinting( True ) q'M-a tE. Print i VD.p"F(] EnableTextPrinting( False ) j+J)S1 Sz"J-3b^ r 06}@ 7 For j = 0 To nx - 1 w=3@IW M>0=A xpos = xpos + pixelx ^C@uP9g 7Z"mVh} 'shift source W<B8P S$ LockOperationUpdates srcnode, True 4fZ$&)0& GetOperation srcnode, 1, op Cfb/f]*M op.val1 = xpos -";'l@D= op.val2 = ypos z(3mhMJY SetOperation srcnode, 1, op #=b_!~:% LockOperationUpdates srcnode, False sN7I~ .7Ys@;>B 'raytrace Y1Bj++?2 DeleteRays Uz\B^"i| CreateSource srcnode )AqM?FE4R TraceExisting 'draw ,ibI@8;#~' g^^%4Y 'radiometry EUe2<G For k = 0 To GetEntityCount()-1 `t: 7&$>T If IsSurface( k ) Then PQXyu1 temp = AuxDataGetData( k, "temperature" ) ~7b'4\ emiss = AuxDataGetData( k, "emissivity" ) U{LDtn%@h6 If ( temp <> 0 And emiss <> 0 ) Then ]^&DEj{ ProjSolidAngleByPi = GetSurfIncidentPower( k ) rr*",a"}m frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 23y7l=.b/ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi ,u{d@U^)3@ End If [={pFq` nV
McHN End If zV4%F"- |I7P0JqP Next k g 6>RyjN Q9 kKk Next j +yS"pOT Nt&}T Next i -deY,% EnableTextPrinting( True ) PFG):i-? /+sn-$/"i 'write out file NV*aHci fullfilepath = CurDir() & "\" & fname +sE8 1B Open fullfilepath For Output As #1 >?b/_O Print #1, "GRID " & nx & " " & ny E`iT>+LG< Print #1, "1e+308" 5 &-fX:/ Print #1, pixelx & " " & pixely /zuU Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 _xAdvr' W 8:$kFy\A' maxRow = nx - 1 phl5E:fIKx maxCol = ny - 1 `\q4z-<- For rowNum = 0 To maxRow ' begin loop over rows (constant X) EiP_V&\ row = "" v=i[s For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) T
{(6*^g<B row = row & irrad(colNum,rowNum) & " " ' append column data to row string EZIMp8^ Next colNum ' end loop over columns d~S.PRg= QCa$<~c Print #1, row 6O$OM }N2T/U Next rowNum ' end loop over rows Kdx?s;i Close #1 ECg/ge2 6peO9]Zy Print "File written: " & fullfilepath _9#4 Print "All done!!" z:RwCd1\ End Sub 2y
~]Uo rA8neO) 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: xlgN}M =o{zw+|% % h k(2,z 找到Tools工具,点击Open plot files in 3D chart并找到该文件 @w,-T@nAW ub+>i !7AW_l9`i 打开后,选择二维平面图: M `Y~IG} 1-r1hZ-
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