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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。 sfEy UE%~SVi.# 成像示意图 >l0D,-O]m 首先我们建立十字元件命名为Target fGDjX!3-S :g"UG0]; 创建方法: soB5sFt&] !>QD42 面1 : ~HyqHxy 面型:plane #p|7\Y 材料:Air WB>M7MI% 孔径:X=1.5, Y=6,Z=0.075,形状选择Box >=3ay^(Y2D rtgu{m02 m<e-XT 辅助数据: uSn<]OrZo` 首先在第一行输入temperature :300K, orr6._xw emissivity:0.1; SXm Hn.? gye'_AR?k |H@1g=q 面2 : %DF-;M"8 面型:plane a2`|6M; 材料:Air %:7fAB,PA 孔径:X=1.5, Y=6,Z=0.075,形状选择Box q.g0Oz@z D= LLm$y
-c'~0g]< 位置坐标:绕Z轴旋转90度, e8ZMB$byP *[O)VkL\%i zXx)xIO 辅助数据: 9)]asY 6.
6g9 首先在第一行输入temperature :300K,emissivity: 0.1; h(wu5G0C#u ojQjx|Q} h`%}5})= Target 元件距离坐标原点-161mm; lDm0O)Dh! 8 ,<F102( ()I';o 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 C@Fk Y)]x1I Iw-3Z'hOX 探测器参数设定: ZpTT9{PT=: WT9k85hqj 在菜单栏中选择Create/Element Primitive /plane MZInS:Vj tHV81F1J 5t&;>-A'?' zw,=mpf3_ Y$ To)qo UL
元件半径为20mm*20,mm,距离坐标原点200mm。 ,Rh6(I \9GJa"xA` 光源创建: QCvz| ) F7~T=X)1 光源类型选择为任意平面,光源半角设定为15度。 ?$&iVN^UA r.T!R6v} [ym
ynr3M 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 .W)%*~ O!; P,/=c(5\} 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 .Q^8_'ZG r#CQCq P5^<c\Mr,Y 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 CVyE5w OcWzo#q4[ 创建分析面: 7P$>T Ckc4U. t| ui\yY3? 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。 {BA1C
( ev_4!+ko )LP=IT 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。 z|:3,$~sN Z* Fxr;)d FRED在探测器上穿过多个像素点迭代来创建热图 A/zZ%h / .ddx< FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 e
MT5bn 将如下的代码放置在树形文件夹 Embedded Scripts, Nhnw'9 wgb
e7-{ *$eMM*4 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。 O-D${== !b0ANIp 绿色字体为说明文字, @{|vW dO{a!Ca '#Language "WWB-COM" np#RBy 'script for calculating thermal image map ~T_4M 'edited rnp 4 november 2005 =I}8-AS~V d/fg 'declarations cn~M:LW23 Dim op As T_OPERATION M'
d ,TV[ Dim trm As T_TRIMVOLUME XDWR] Dim irrad(32,32) As Double 'make consistent with sampling 0+]ol:i Dim temp As Double V#Hg+\{d Dim emiss As Double ?Thh7#7LM Dim fname As String, fullfilepath As String ]N\J~Gm )S;pYVVAl 'Option Explicit &r)i6{w81 dP0%<Q| Sub Main ,a&&y0, 'USER INPUTS :Rq>a@Rp nx = 31 {|;5P.,l ny = 31 j6NK7Li numRays = 1000 8 )W{C> minWave = 7 'microns {O4y Y=G maxWave = 11 'microns rk$$gXg9/ sigma = 5.67e-14 'watts/mm^2/deg k^4 .D~ZE94@ fname = "teapotimage.dat"
9z9EK'g dZ1/w0<M2 Print "" [-*1M4D9 Print "THERMAL IMAGE CALCULATION" HX(Z(rcI QR+{Yp detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 }5 2] M+mO4q6 Print "found detector array at node " & detnode L1'#wH Vh WF(* srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 nbVlP ]%RX\~Q.4 Print "found differential detector area at node " & srcnode 0gs0[@ vUX(h.}8 GetTrimVolume detnode, trm /n9yv detx = trm.xSemiApe &K1\" dety = trm.ySemiApe .fQ/a`AsU area = 4 * detx * dety &g{b5x{iD Print "detector array semiaperture dimensions are " & detx & " by " & dety u;[*Z Print "sampling is " & nx & " by " & ny E7_)P>aS5 Dd(# 'reset differential detector area dimensions to be consistent with sampling fc~6/ pixelx = 2 * detx / nx ww_gG5Fc$ pixely = 2 * dety / ny ]7*Z'E SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False \5]${vs&s Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 NaR/IsN8% _x.<Zc\x 'reset the source power j"8 f,er SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) {Q&@vbw' Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" J^Dkx"1GD ,}("es\b 'zero out irradiance array N^G:m~> For i = 0 To ny - 1 \Kx@?, For j = 0 To nx - 1 9WJS.\G^ irrad(i,j) = 0.0 *@XJ7G[ Next j AjTkQ)
Next i %[x oA)0! lHV&8fny 'main loop h\jV@g$ EnableTextPrinting( False ) $yZ(c#L w4: ypos = dety + pixely / 2 [>B`"nyNQ For i = 0 To ny - 1 jkPye{j xpos = -detx - pixelx / 2 #s'UA!) ypos = ypos - pixely BD)5br]. 6vx0F?>_ EnableTextPrinting( True ) 986y\9Zu Print i {Z529Ns EnableTextPrinting( False ) @_gCGI>Q our$Ka31 SMMV$;O{9 For j = 0 To nx - 1 m.F \Mn PRs[!EB6 xpos = xpos + pixelx [7K-L6X q'07 'shift source &8l"Dl LockOperationUpdates srcnode, True z!z+E%H^ GetOperation srcnode, 1, op #E[{ op.val1 = xpos _TB,2 R op.val2 = ypos 1;; is SetOperation srcnode, 1, op xKilTh_.6 LockOperationUpdates srcnode, False =F(fum;zH >i`V-" x raytrace 52*9q! DeleteRays %R18 CreateSource srcnode e{ce
\ TraceExisting 'draw 9@nDXZPY& .RI{\ i` 'radiometry B74L/h For k = 0 To GetEntityCount()-1 Z!@<[Vo6 If IsSurface( k ) Then J>I.|@W4 temp = AuxDataGetData( k, "temperature" ) R]0p L emiss = AuxDataGetData( k, "emissivity" ) IZ<d~ [y If ( temp <> 0 And emiss <> 0 ) Then Ig9gGI, ProjSolidAngleByPi = GetSurfIncidentPower( k ) //SH=>w2 frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) eXHk6[%[ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi oKl^Ttr End If HFJna2B` Y9b|lP7! End If 3GH@|id "pb$[*_@$ Next k Q(P'4XCm `Qf$]Eoft Next j uXs.7+f s0}OsHAj Next i dQ4VpR9|; EnableTextPrinting( True )
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%OA J&64tQl* 'write out file ~16QdwK fullfilepath = CurDir() & "\" & fname .hYrE5\- Open fullfilepath For Output As #1 h$#QRH Print #1, "GRID " & nx & " " & ny
ohK_~ Print #1, "1e+308" 2v
^bd^]u: Print #1, pixelx & " " & pixely zJp}JO Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 CNC3">Dk~9 hXsd12 maxRow = nx - 1 %/l9$>{ maxCol = ny - 1 W/(D"[:l% For rowNum = 0 To maxRow ' begin loop over rows (constant X) xc%\%8C} row = "" K;%P_f/KJP For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) 4!'1o`8vs row = row & irrad(colNum,rowNum) & " " ' append column data to row string XcoV27 Next colNum ' end loop over columns zTDB]z!A 8|>$M Print #1, row R{s&6 9H@I<`qGC Next rowNum ' end loop over rows |}~2=r z Close #1 V SJGp` OH` |
c Print "File written: " & fullfilepath W|IMnK- Print "All done!!" 1Sk=;Bic End Sub 08J[9a0[ `Yk~2t"V 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: ].W)eMC*c( #;9I3,@/Y uSZCJ#'G 找到Tools工具,点击Open plot files in 3D chart并找到该文件 p2]@yE7w +.Pv:7gh +mM=`[Z`?? 打开后,选择二维平面图: #6< X 6jv_j[[
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