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。 4(,.<# $l)RMP}
成像示意图 !9gpuS[ 首先我们建立十字元件命名为Target ~
tR!hc} @|\;#$?XW3 创建方法: ty!DMg# hg12NzbK 面1 : ]|F`;} 7 面型:plane .;31G0<w2 材料:Air ,w "cY?~< 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 4r;le5@ iM!V4Wih6
kPOk.F%) 辅助数据: ZWGelZP~ 首先在第一行输入temperature :300K, H`<u2fo|p emissivity:0.1; Z3o HOy G l/3*J s]yZ<uA 面2 : euY+jc% 面型:plane !rgXB( 材料:Air v$` 3}<3- 孔径:X=1.5, Y=6,Z=0.075,形状选择Box "LYhYkI s
j-oaWt 8Ud.t=2 位置坐标:绕Z轴旋转90度, YeJTB} y< gRl/e
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q 辅助数据: a%y*e+oM D7R;IA-w 首先在第一行输入temperature :300K,emissivity: 0.1; Bph(\=
W ?`vGpi~ Z3zD4-p$_ Target 元件距离坐标原点-161mm; Q$Qr)mcC &: LE]w
eOVln1a 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 |1kA6/ p8]X Ne Q_/UC#I8 探测器参数设定: DM6(8df( Y)8 Py1} 在菜单栏中选择Create/Element Primitive /plane r,|}^u8` z xgDaT
e}gGl<((g U0|wC,7" &iuMB0rbu 3-y2i/4}$ 元件半径为20mm*20,mm,距离坐标原点200mm。 H5vg s2R H(?+-72KX 光源创建: (CAVOed `j2|aX
%Z* 光源类型选择为任意平面,光源半角设定为15度。 CC6]AM(i /L`qOr2E )fuAdG 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\k6."e_& }lkU3Pf1U 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。 &mJm'Ks \Vj7%ph 4\U"e* 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。 22d>\u+c mst;q@ 创建分析面: W'zI~'K d^Cv9%X 7
A{R0@ 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。 ^6UE/4x!y d<_IC7$u>
R-Tf9?) 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 Np
opg1Gv> IjPtJwW`A FRED在探测器上穿过多个像素点迭代来创建热图 1OFrxSg uq!d8{IMu FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 ~c,+)69"T 将如下的代码放置在树形文件夹 Embedded Scripts, V'N]u(^ b5
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:Mu]*N 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 30cb+)h( U4NA'1yo 绿色字体为说明文字, Y0Rk:Njc r*Z p-} '#Language "WWB-COM" R4f_Kio 'script for calculating thermal image map F @!9rl' 'edited rnp 4 november 2005 f2P2wt.$ AbMf8$$3SH 'declarations tiic>j\D Dim op As T_OPERATION G{'`L)~3N Dim trm As T_TRIMVOLUME v00w
GOpW Dim irrad(32,32) As Double 'make consistent with sampling eeUEqM$7EX Dim temp As Double l5Q-M{w0x Dim emiss As Double 7@!ne&8Z? Dim fname As String, fullfilepath As String 3r2e_?m ?&XpwJw:~ 'Option Explicit r[&/*~xL V*+Z=Y' Sub Main ]#O~lq 'USER INPUTS KupQtT< nx = 31 mk`#\=GE ny = 31 $gcC}tX numRays = 1000 Q$S|L C minWave = 7 'microns eBlB0P
maxWave = 11 'microns m@`
NN sigma = 5.67e-14 'watts/mm^2/deg k^4 -H](2} fname = "teapotimage.dat" WD'[|s\ $@ZrGT Print "" tc<HA7vpt~ Print "THERMAL IMAGE CALCULATION" =(as{,j k
3oR: detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 $s9YU" Xa=oEG Print "found detector array at node " & detnode AI*1kxR uRRp8hht srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 5l
/EZ\q cY%6+uJ1 Print "found differential detector area at node " & srcnode Pu0O6@Rg OR-fC GetTrimVolume detnode, trm FP h1 }qS detx = trm.xSemiApe sy+tLDMd dety = trm.ySemiApe >}!})]Xw9 area = 4 * detx * dety r=^? Print "detector array semiaperture dimensions are " & detx & " by " & dety +m1y#|08 Print "sampling is " & nx & " by " & ny $r/tVu2!W :)Z.! 'reset differential detector area dimensions to be consistent with sampling 5|bc*iqU pixelx = 2 * detx / nx +FlO_=Bu pixely = 2 * dety / ny 0r'<aA`=I SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False k|F TT Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 #bdSH)V 0X4%Ccs 'reset the source power >_LZD4v!< SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) ZE0D= Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" ^@n?& z+qrsT/?L 'zero out irradiance array LIMPW w g For i = 0 To ny - 1 Qj',&b For j = 0 To nx - 1 .0u@PcE:O irrad(i,j) = 0.0 `@Tl7I\ Next j Ld:U~M- Next i s&~i S[ M"<B@p]rk: 'main loop :]k`;;vh EnableTextPrinting( False ) $Z{Xt*
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ypos = dety + pixely / 2 -k"5GUc| For i = 0 To ny - 1 o[E|xw xpos = -detx - pixelx / 2 &Uu8wFbIJ ypos = ypos - pixely ubQZTA x We*&\e+"T EnableTextPrinting( True ) zTvGku[3 Print i q[MZSg EnableTextPrinting( False ) k_hs g6Ur. Dt\rMSjZ9 U%E364;F For j = 0 To nx - 1 YVS~|4hu?i ftwn<B xpos = xpos + pixelx wj#A#[e LP-_i}Kq 'shift source k86j&
.m_ LockOperationUpdates srcnode, True tunjV1 ,] GetOperation srcnode, 1, op 1/%g
VB8 op.val1 = xpos El:& op.val2 = ypos g|rbkK%SoE SetOperation srcnode, 1, op [$AOu0J LockOperationUpdates srcnode, False @eU5b63jM b?{ \t; raytrace N9=1<{Z DeleteRays eY#_!{*Wn CreateSource srcnode Z_}[hz$ TraceExisting 'draw 2UJjYrm y=spD^tM8 'radiometry )=@SA`J For k = 0 To GetEntityCount()-1 0s'H(qE,_ If IsSurface( k ) Then 1xzOD@=dI temp = AuxDataGetData( k, "temperature" ) TZYz`l+v emiss = AuxDataGetData( k, "emissivity" ) rwSmdJ~ If ( temp <> 0 And emiss <> 0 ) Then aokV'6 ProjSolidAngleByPi = GetSurfIncidentPower( k ) $K}Y frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) a1yGgT a?D irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi b!3Y<D* End If 8-cCWoc + Ssu^>D End If IMtfi(Y%F 4J${gcju Next k \4 5%K|
X[r\ Qa Next j 7t~12m8x QkU6eE<M* Next i E[2>je EnableTextPrinting( True ) %kSpMj| &h_do8R 'write out file 6< O|,7=_ fullfilepath = CurDir() & "\" & fname fA{t\ Open fullfilepath For Output As #1 1K&l}/zUl Print #1, "GRID " & nx & " " & ny T\b-<Xle Print #1, "1e+308" nOj0"c Print #1, pixelx & " " & pixely YR/%0^M'0 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 W_%@nm\y K! I]0!: maxRow = nx - 1 mX&!/U maxCol = ny - 1 NUp,In_ For rowNum = 0 To maxRow ' begin loop over rows (constant X) ,wPvv(b]a row = "" (>a8h~Na For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) |];f?1 row = row & irrad(colNum,rowNum) & " " ' append column data to row string fNnX{Wq Next colNum ' end loop over columns I5mtr h}SP` Print #1, row DL]\dD lz>>{ Next rowNum ' end loop over rows "s.]amC Close #1 %.[jz,;) 2SV}mK U Print "File written: " & fullfilepath b^q8s4( Print "All done!!" {sb2r%U!+ End Sub ngI3.v/R +\/1V` 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: yHNx,ra v|
Yh]y SL ) ope 找到Tools工具,点击Open plot files in 3D chart并找到该文件 Z0#&D&2sV <7R+p;y :Cdqj0O3u 打开后,选择二维平面图: PqVz^(Wz }Md5a%s<
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