| 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。 }%AfZ2g;h ? JTTl;
成像示意图 `7'^y 首先我们建立十字元件命名为Target 1k^$:' q[+h ~) 创建方法: 5%4yUd#b BsL+9lNue 面1 : "shX~zd5 面型:plane d`C$vj 材料:Air ]Yf^O @<<> 孔径:X=1.5, Y=6,Z=0.075,形状选择Box !@wUARQ sCP|d`'
54B`T/>R:E 辅助数据: 4q:8<*W= 首先在第一行输入temperature :300K, Jt#HbAY emissivity:0.1; gs7_Q >56fa6=3@ CBNt
_y 面2 : G Y.iCub 面型:plane uMpuS1 材料:Air %Ofw"W 孔径:X=1.5, Y=6,Z=0.075,形状选择Box zY7M]Az edCVIY'1 Ju&FwY+ 位置坐标:绕Z轴旋转90度, Z{:;LC GU9G5S.
$CJf 0[| 辅助数据: ZHUW1:qs HG< z,gE
2 首先在第一行输入temperature :300K,emissivity: 0.1; ?B$L'i[l hOkn@F. k Jw
Pd;% Target 元件距离坐标原点-161mm; M X?UmQ' A.@wGy4
$Ff6nc= 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 -QR]BD%J*[ _~{J."q ){z#Y#]dP 探测器参数设定: ,3c25.,* Oo-4WqRJ 在菜单栏中选择Create/Element Primitive /plane ),y`Iw 6Vncr}
EVBOubV UZmUYSu; c0HPS9N\ Ayv:Pv@ 元件半径为20mm*20,mm,距离坐标原点200mm。 Nn-k hl|11 5O]ZX3z> 光源创建: ]Hq,Pr_+ :?LNP3} 光源类型选择为任意平面,光源半角设定为15度。 98| v.d l:bbc!3 .Y^3G7On 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 6d6Dk>(V ZXkrFA | 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 0UW_ Pbh6 PFx.uqp B2*>7 kc_s 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 r..f$FF)\ f2pA+j5[ 创建分析面: *JZ9'|v_H w|6?A- SK&1l`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。 -5]lHw} 4p+Veo6B
"PWGtM:L8Y 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。 E(_k#X ;I80<SZ FRED在探测器上穿过多个像素点迭代来创建热图 w-$iKtb. >?)_, KL 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。 ^!i4d)) 将如下的代码放置在树形文件夹 Embedded Scripts, ;@Z1y @Q{:m)\
%Ie,J5g5 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。 RJd*(!y R.l!KIq 绿色字体为说明文字, AZ^>osr WA1yA*S '#Language "WWB-COM" PX0N7L 'script for calculating thermal image map ( xzruI5P 'edited rnp 4 november 2005 R/fE@d2~In _A&
[rBm| 'declarations $bF+J8%D Dim op As T_OPERATION jk_yrbLc Dim trm As T_TRIMVOLUME .I]v
D#o Dim irrad(32,32) As Double 'make consistent with sampling ^&y*=6C Dim temp As Double hVT>HER Dim emiss As Double zFipuG02 Dim fname As String, fullfilepath As String 'rFLG+W
v0(}"0 'Option Explicit UY,u-E" xaB#GdD Sub Main #lSGH 5Fp? 'USER INPUTS b "}ya/ nx = 31 )+hJi/g ny = 31 $sb@*K}:4 numRays = 1000 }weE^9GiJ minWave = 7 'microns
._;It198f maxWave = 11 'microns n ~ &ssFC sigma = 5.67e-14 'watts/mm^2/deg k^4 BILZ XMf fname = "teapotimage.dat" 6Fk[wH7 vl}}h%BC Print "" `WxGU Print "THERMAL IMAGE CALCULATION" mr_NArF WLh!L='{BK detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 e.(d?/!F_
]SL+ZT Print "found detector array at node " & detnode s(s_v ?k !Q%r4Nr
srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 0pB'^Q{ jJ@@W~/)B Print "found differential detector area at node " & srcnode C R't MIZ!+[At GetTrimVolume detnode, trm W$l4@A detx = trm.xSemiApe "]'W^Fg dety = trm.ySemiApe qT4`3nH: area = 4 * detx * dety 0|0IIgy Print "detector array semiaperture dimensions are " & detx & " by " & dety p&`I#6{ Print "sampling is " & nx & " by " & ny H.l
WHM+H4 [!} uj`e 'reset differential detector area dimensions to be consistent with sampling "
;8kKR pixelx = 2 * detx / nx FcOrA3tt pixely = 2 * dety / ny h]|2b0 SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False UN^M.lqZX Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 +:c}LCI9< @Y(7n/*
'reset the source power ]^a{?2ei SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 6OQ\f,h@ Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" @}+B%R 1OqVNp%K 'zero out irradiance array (V/!0Lj For i = 0 To ny - 1 #0#6eT{- For j = 0 To nx - 1 jlUT9Zp irrad(i,j) = 0.0 Ur""&@ Next j F:0 E-
z' Next i )D]LPCd[ Q2@yUDd! 'main loop 3A\Hiy!{F EnableTextPrinting( False ) Nk F2'Z{$+ 1ahb:Mjv ypos = dety + pixely / 2 Dl}va For i = 0 To ny - 1 j{/wG:: xpos = -detx - pixelx / 2 lx82:_ ypos = ypos - pixely IUh)g1u41O +J}h EnableTextPrinting( True ) f-}_ Print i g%4=T~ EnableTextPrinting( False ) gvP.\,U 3);Wgh6 'w\Gd7E For j = 0 To nx - 1 b&pL}o?/k q }9n. xpos = xpos + pixelx ]}_Ohe]X 5*$z4O:Aa 'shift source |X~vsM0 LockOperationUpdates srcnode, True MPsm)jqX GetOperation srcnode, 1, op P$`k*
v op.val1 = xpos %B Rll op.val2 = ypos (*!4O>] SetOperation srcnode, 1, op L7.LFWq$S LockOperationUpdates srcnode, False <L3ig%#B `
B+Pl6l)F 'raytrace \&Oc}] DeleteRays E0Kt4%b CreateSource srcnode Jqt|'G3 TraceExisting 'draw +n<;);h S'AS,'EnY 'radiometry FzFP 0 For k = 0 To GetEntityCount()-1 hB]<li)"C If IsSurface( k ) Then .[o?qCsw temp = AuxDataGetData( k, "temperature" ) t~]tw emiss = AuxDataGetData( k, "emissivity" ) 2fdC @V If ( temp <> 0 And emiss <> 0 ) Then sH)40QmO{ ProjSolidAngleByPi = GetSurfIncidentPower( k ) QPsvc6ds frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) xa%2w] irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi M 0RVEhX End If rJcZ a# ,#80`&\% End If DGx<Nys@B ZL- ` 3x Next k s#)tiCSVW L>2gx$f Next j d7L|yeb" 'ewVn1ME[ Next i o}lA\ A EnableTextPrinting( True ) d0 yZ9-t Cv1CRmqq% 'write out file KHt#mQy)9 fullfilepath = CurDir() & "\" & fname NE!] Open fullfilepath For Output As #1 &0@AM_b Print #1, "GRID " & nx & " " & ny .?-]+-J?` Print #1, "1e+308" je~gk6}Y Print #1, pixelx & " " & pixely #N|A@B5x Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 Gv}~ \>|:URnD maxRow = nx - 1 r1Cq8vD*m maxCol = ny - 1 U^xtS g For rowNum = 0 To maxRow ' begin loop over rows (constant X) .&c!k1kH row = "" )u_[cEJHO For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) ]Saw}agE[% row = row & irrad(colNum,rowNum) & " " ' append column data to row string e!O:z Next colNum ' end loop over columns -VRKQNT WEB enGQ Print #1, row hvU\l`m cP (is! Next rowNum ' end loop over rows l(
0:CM Close #1 PsoW:t |th"ET Print "File written: " & fullfilepath Sc3 B*. Print "All done!!" &dI;o$t End Sub 1c03<(FCd +h?z7ZY^ 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: "+KAYsVtU fIg~[VN" g|V0[Hnq6 找到Tools工具,点击Open plot files in 3D chart并找到该文件 RkXW(T` +%RB&:K7, !V;glx[ 打开后,选择二维平面图: [+Y;w`;Fq y5lhmbl: e
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