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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。 b5UIX Kim ~" U^N:I" 成像示意图 .:TSdusr~ 首先我们建立十字元件命名为Target \.MPjD esHcE{GNOS 创建方法: m)xz_Plc WeS$$:ro 面1 : 4]ETF+ 面型:plane zWq&HBs 材料:Air *> 7Zc 孔径:X=1.5, Y=6,Z=0.075,形状选择Box /cZ-+cu h1Q rFPQnu bqm%@*fZo 辅助数据: G\H |\i 首先在第一行输入temperature :300K, Jnq}SUev emissivity:0.1; 1(m[L=H5> 2[Bw+<YA` h
Ap(1h#m 面2 : j{H,{x 面型:plane b:6e2|xf? 材料:Air ~&Y%yN^ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 9rM6kLD "I&,':O+ xw~&OF& 位置坐标:绕Z轴旋转90度, {s~t>R p+ A&qZ:&(OM :pg]0X; 辅助数据: -jL10~/ 8H2A<&3i 首先在第一行输入temperature :300K,emissivity: 0.1; `:;fc U
jB5Xks tLe"i> Target 元件距离坐标原点-161mm; #P-T4R H!uq5`j0K rn%q*_3-o 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 DzG$\%G2R} )W$@phY(I ./E<v 探测器参数设定: 5jK9cF$> 5SwQ9# 在菜单栏中选择Create/Element Primitive /plane qZ DP- M07==R7 $Rv(v% n*vhCeL j\@osjUu jL9to6 Hmr 元件半径为20mm*20,mm,距离坐标原点200mm。 3q:>NB< *WZ?C|6+ 光源创建: ub=Bz1._ QAKA3{-( 光源类型选择为任意平面,光源半角设定为15度。 Sv|jR r' n~G-X
p+O,C{^f 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 k5]`:k6 _16IP 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 |;(0] @DA.$zn& s!F`
0=J^ 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。 \} +b_J6- ok<!/"RX$ 创建分析面: !O*uQB /;a b"b )0p7d:%mV 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。 LKe~ kC4}@{4i n6s[q-td 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。 !w=6>B^ 6F4OISy%3 FRED在探测器上穿过多个像素点迭代来创建热图 kxVR#: <c$K3 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。 \?rBtD( 将如下的代码放置在树形文件夹 Embedded Scripts, ]J>{ZL ,T\)%q 15tT%TC 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。 K"U[OZC` BP`'1Ns 绿色字体为说明文字, 8^|lsB}x? m03]SF(#3 '#Language "WWB-COM" }E]&,[4&M 'script for calculating thermal image map QpC,komLJ 'edited rnp 4 november 2005 <m!(eLm+B >lIQM3 'declarations L>Soj|WUy( Dim op As T_OPERATION l&4+v.zr Dim trm As T_TRIMVOLUME !$5.\D Dim irrad(32,32) As Double 'make consistent with sampling WyDL ah^/ Dim temp As Double UpIt"+d2& Dim emiss As Double `U[s d*C" Dim fname As String, fullfilepath As String $wx)/t< pz]#/Ry? 'Option Explicit 8O0E;6b B>"O~ gZ{# Sub Main ri?>@i-9= 'USER INPUTS
re;^, nx = 31 I? o)X! ny = 31 3A>Bnb numRays = 1000 2N$yn minWave = 7 'microns Yl!~w:O!o maxWave = 11 'microns GN%|'eU sigma = 5.67e-14 'watts/mm^2/deg k^4 leSR2os fname = "teapotimage.dat" vPbmQh ex pk,]yi,ZF Print "" Hp!c\z; Print "THERMAL IMAGE CALCULATION" mcB8xE ]-b`uYb detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 8kwe ._&) A:-r2;xB Print "found detector array at node " & detnode [ijK~ d5O_~xf& srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点
{j{H@rHuy =Pu;wx9 Print "found differential detector area at node " & srcnode bm:"&U*tu' @ZUrr_| GetTrimVolume detnode, trm FhkS"y detx = trm.xSemiApe .3QX*]{ dety = trm.ySemiApe F}Kkhs
{ area = 4 * detx * dety sKK*{+,kh; Print "detector array semiaperture dimensions are " & detx & " by " & dety _R 6+bB$ Print "sampling is " & nx & " by " & ny fI([vI wxx3']: 'reset differential detector area dimensions to be consistent with sampling 2a3RRP pixelx = 2 * detx / nx VX<jg #( pixely = 2 * dety / ny l9"T"9C{ SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False Bl"BmUn Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 &rmXz6F |{a`,%mw 'reset the source power iE;D_m.>`O SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) g} /efE Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" ?Dr K2;q RMfKM!
vE 'zero out irradiance array ?mCino For i = 0 To ny - 1 wcI?. For j = 0 To nx - 1 Z&VH7gi irrad(i,j) = 0.0 (v'#~ )R_` Next j c6@7>PM Next i 7i$)iNW xR`W9Z5 'main loop [$<\*d/ EnableTextPrinting( False ) ~5Cid)Q}@o % >\v6ea ypos = dety + pixely / 2 c :{#H9 For i = 0 To ny - 1 UbnX%2TW xpos = -detx - pixelx / 2 Mt93YD-2+ ypos = ypos - pixely G'M;]R9EP TJY
[s- EnableTextPrinting( True ) ,R~{$QUl Print i 8NJxtT~0c~ EnableTextPrinting( False ) %]m/fo4b XJ3p< abW[hp For j = 0 To nx - 1 m/T3Um Q,f~7IVX xpos = xpos + pixelx m'b9 f6 1#D &cx6 'shift source iW
#|N^ LockOperationUpdates srcnode, True 7^2 GetOperation srcnode, 1, op l[AQyR1+/ op.val1 = xpos Mkj` op.val2 = ypos .EF(<JC? SetOperation srcnode, 1, op =G9 9U/ LockOperationUpdates srcnode, False `;7eu= `u't raytrace +'ZJ] DeleteRays dx&!RK+ CreateSource srcnode {#_CzI.0f TraceExisting 'draw %lbDcEsf9 @F-InfB8. 'radiometry 'BiR ,M$mY For k = 0 To GetEntityCount()-1 %wDE+&M If IsSurface( k ) Then U{JD\G8m temp = AuxDataGetData( k, "temperature" ) b:M1P&R emiss = AuxDataGetData( k, "emissivity" ) b5@sG^ If ( temp <> 0 And emiss <> 0 ) Then c&mLK1A6 ProjSolidAngleByPi = GetSurfIncidentPower( k ) 1z6$>{FUR frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) I0qSx{K irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi QH d^?H* End If !<8-juY i0TbsoKh: End If "?X,);5S @|2L>N Next k XYh)59oM% aob+_9o Next j (^@rr[.o7 I""zg^Rq Next i ~Oc:b>~ EnableTextPrinting( True ) VL?sfG0 Z0'&@P$ 'write out file x@)G@'vV| fullfilepath = CurDir() & "\" & fname -P.51q Open fullfilepath For Output As #1 lM|}K-2 Print #1, "GRID " & nx & " " & ny \2c3Nsra Print #1, "1e+308" ]<xzCPB Print #1, pixelx & " " & pixely CQANex4&\ Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 Hh1]\4D,4 x<'<E@jpU; maxRow = nx - 1 m}$7d5 maxCol = ny - 1 j%`%
DQ For rowNum = 0 To maxRow ' begin loop over rows (constant X) kdP*{ row = "" cp)BPg For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) z%Eok row = row & irrad(colNum,rowNum) & " " ' append column data to row string ~z kzuh Next colNum ' end loop over columns @"G+kLv0 !\}X?Gf Print #1, row 1VR|z Pxvf"SXX Next rowNum ' end loop over rows >lV'}0u) Close #1 )4e8LO &E+mXEve Print "File written: " & fullfilepath &|K9qa~)Y Print "All done!!" 5<>"d :9 End Sub YctWSfh XkhGU?={ 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: 0 L$[w `PUGg[Zx^ X=KC+1e 找到Tools工具,点击Open plot files in 3D chart并找到该文件 {ew;
/; kRb %:* k.ttrKy<q/ 打开后,选择二维平面图: jcbq# aJ"m`5]=%
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