| 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。 K:AP 0Te 2_M+o]Z^
成像示意图 ;g2UIb?{6 首先我们建立十字元件命名为Target 61gyx6v _]D
6m2R 创建方法: >mEfd=p MI:%Eq 面1 : i-@V 面型:plane <1*\ ~CX 材料:Air Q^05n$ tI 孔径:X=1.5, Y=6,Z=0.075,形状选择Box vMJ(Ll7/ 4Xt`L"f
alNn(0MG 辅助数据: 3qH1\ 首先在第一行输入temperature :300K, vfm Y>nr emissivity:0.1; asmu< vo&h6'i>7 >w.%KVBJ 面2 : ,Sy&?t}` 面型:plane e0Gs|c+6 材料:Air }ALli0n`V) 孔径:X=1.5, Y=6,Z=0.075,形状选择Box FDGG$z?>m tuuwoiQ*` 1Qz@ 位置坐标:绕Z轴旋转90度, '<1Cta` q0vZR"y
Y(?SE< 4R 辅助数据: xpwy%uo e:.?T\ 首先在第一行输入temperature :300K,emissivity: 0.1; .ns=jp v?Cakwu q6>} Target 元件距离坐标原点-161mm; :7dc;WdM ,]]IJ;:w
R1<$VR 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 WQD:~*C: EdSUBoWF} C>,> _ 探测器参数设定: >dD$GD{ RQ^
\|+_ 在菜单栏中选择Create/Element Primitive /plane 5dD8s-;^T b7T;6\[m
h/8p2Mrqi 2cRru]VZ5 v'^}zO @M'qi=s* 元件半径为20mm*20,mm,距离坐标原点200mm。 CQrP%}`r }4h0{H 光源创建: Y3(I;~$! Ze#DFe$ 光源类型选择为任意平面,光源半角设定为15度。 }Ya! [tX 9$C?)XKXB :)tsz; 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 Hr!$mf)h u7Ix7`V 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。 `Lavjmfr2V T0)bnjm 8pftc) k 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。 u%I%4 gM n4}e!
创建分析面: 8ZM#.yBB 7n+,!oJ U[8F{LX 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。 _G'A]O/BZD <o*b6m%
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I3fk 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。 *,*O.#<6 )& Oxp&x FRED在探测器上穿过多个像素点迭代来创建热图 |JHNFs V|}9bNF 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。 4gNN " 将如下的代码放置在树形文件夹 Embedded Scripts, U,61 3G dga4|7-MY
p4UEhT 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。 M* Ej*# m.! M#x2! 绿色字体为说明文字, V3r)u\ o' op9vz[o#4 '#Language "WWB-COM" 'gg<)Bd 'script for calculating thermal image map rXE0jTf:a 'edited rnp 4 november 2005 !cM<&3/ dC-~=}HR^ 'declarations 4 dLnX3 v Dim op As T_OPERATION BT_XqO Dim trm As T_TRIMVOLUME {2D|,yH= Dim irrad(32,32) As Double 'make consistent with sampling d!Gy#<H Dim temp As Double 0chpC)#Q3; Dim emiss As Double Tcc83_Iq Dim fname As String, fullfilepath As String k`|E&+og xa<KF 'Option Explicit c_M[>#` V@b7$z Sub Main U=69q] 'USER INPUTS (FaYagD nx = 31 ?CC.xE ny = 31 r Dlu& numRays = 1000 g}gGm[1SUo minWave = 7 'microns y"'p#j maxWave = 11 'microns >wt.)c?5 sigma = 5.67e-14 'watts/mm^2/deg k^4 L%Rw]=v}v fname = "teapotimage.dat" ?~t5>PEonv d,(q3 Print "" cRD;a?0/6s Print "THERMAL IMAGE CALCULATION" ?*+U[*M n8_X<jIp3 detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 T#E$sZ |)Dm.)/0) Print "found detector array at node " & detnode k}&wy <2&qIvHL srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 rr1'|
k" UXdc'i g Print "found differential detector area at node " & srcnode S Z/yijf V;"2=)X GetTrimVolume detnode, trm Cb? !+U detx = trm.xSemiApe ex1!7A!}g dety = trm.ySemiApe Mog [,{w area = 4 * detx * dety ]BbV\# Print "detector array semiaperture dimensions are " & detx & " by " & dety I]+
zG Print "sampling is " & nx & " by " & ny 1Td`S1'#yg vo\'ycPv 'reset differential detector area dimensions to be consistent with sampling 3'` &D/n pixelx = 2 * detx / nx zF[Xem pixely = 2 * dety / ny Q[K$f %> SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False Xy 4k;+ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 )e`9U.C r0lI&25w 'reset the source power JQ0Z%;" SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) g |?}a]G Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" MZ-;'w&Z eZ]r"_? 'zero out irradiance array 2#lpIj For i = 0 To ny - 1 50-7L, For j = 0 To nx - 1 -bOtF% irrad(i,j) = 0.0 vnQFq Next j OEjX(F3= Next i t`|Rn9- 3?"gfw W 'main loop [qRww]g;P| EnableTextPrinting( False ) V'W*'wo nKr'cb ypos = dety + pixely / 2 !h7:rv/ For i = 0 To ny - 1 ciml:"nQ xpos = -detx - pixelx / 2 R$
+RTG:E ypos = ypos - pixely zc;kNkV#1Y i*mU<:t EnableTextPrinting( True ) :6t73\O Print i D3dh,&KO\ EnableTextPrinting( False ) R--s
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rCA!b"C2 [u K,.G For j = 0 To nx - 1 8WP"~Js! H@wjZ;R xpos = xpos + pixelx U9b[t k`N*_/(|n 'shift source 4C_1wk(' LockOperationUpdates srcnode, True YB4
ZI GetOperation srcnode, 1, op %u&Vt"6m= op.val1 = xpos NR_3nt^h op.val2 = ypos x+6z9{O SetOperation srcnode, 1, op C}xfo}i LockOperationUpdates srcnode, False 45.g ; ^i_v\E[QU 'raytrace "A~dt5GJ DeleteRays ~Uv#) CreateSource srcnode rqN+0CT TraceExisting 'draw kDmuj>D M=;csazN 'radiometry J0R{|]W8 For k = 0 To GetEntityCount()-1 .Er+*j;&w If IsSurface( k ) Then D60quEe3% temp = AuxDataGetData( k, "temperature" ) @"fv[=Xb emiss = AuxDataGetData( k, "emissivity" ) s-WZ3g If ( temp <> 0 And emiss <> 0 ) Then ",gVo\^ ProjSolidAngleByPi = GetSurfIncidentPower( k ) -th.(eAx frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 0.R3(O irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi zsQkI@)sO End If DPW^OgL; 2Q@na@s End If [O_5`X9| e#mf{1& Next k ivl %%nY' &4WA/'>R Next j Pz2Q]}(w |/l] ]+ Next i C7m/< EnableTextPrinting( True ) <eSg%6z %4x0^<k~ 'write out file GR*sk#{ fullfilepath = CurDir() & "\" & fname [|*7"Q( Open fullfilepath For Output As #1 W%^!<bFk}m Print #1, "GRID " & nx & " " & ny dT 7fyn Print #1, "1e+308" MNe/H\ Print #1, pixelx & " " & pixely + XBF,<P Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 L6nsVL& p{GO-gE@ maxRow = nx - 1 -WyB2$!( maxCol = ny - 1 r>bgCQ#-n For rowNum = 0 To maxRow ' begin loop over rows (constant X) _,K[kVn row = "" X}3?k<m For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) LHZsmUM(dg row = row & irrad(colNum,rowNum) & " " ' append column data to row string kkHK~(>G Next colNum ' end loop over columns W!XBuk- qrw*?6mSQ Print #1, row TeZu*c
R7z @y o Next rowNum ' end loop over rows 1qn/*9W}= Close #1 Lhg b g0ix" Print "File written: " & fullfilepath ;DZj.|Sj+ Print "All done!!" Pr%KcR ; End Sub M+ <SSi" => 'j_| 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: 4`oKvL9 0)K~pV0aT NqKeQezX 找到Tools工具,点击Open plot files in 3D chart并找到该文件 9&^5!R8 V :5aq.o! |p*cI @ 打开后,选择二维平面图: XHgW9 ;M! A-myY30
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