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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。 uaPx" Me3dpF 成像示意图 |NFZ(6vNh 首先我们建立十字元件命名为Target Fke//- R t0E 51Ic@ 创建方法: x!<yT?A zw@'vncc 面1 : EG<s_d? 面型:plane @x&P9M0g 材料:Air E8[T 孔径:X=1.5, Y=6,Z=0.075,形状选择Box L"+$Wc[| I:j3sy (R}ii}& 辅助数据: ef"?|sn 首先在第一行输入temperature :300K, S~OhtHwK emissivity:0.1; 3`.P'Fh(k ~l E _L1-c 1R%1h9I4' 面2 : Wd,a?31| 面型:plane 7Ke&0eAw 材料:Air Z}6^ve 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 5jcte<
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$({C 9WG{p[ 位置坐标:绕Z轴旋转90度, 4_?7&G0( 8MwK.H[U 1 jb/o5n; 辅助数据: G=9d&N gXFWxT8S 首先在第一行输入temperature :300K,emissivity: 0.1; }?@5W, ^eq</5q D \_6OC Vil Target 元件距离坐标原点-161mm; +>f<EPGn HfNDD|Zz vG41C k1 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 (=x"Y{% o2H1N~e#c 3(E
$I5 探测器参数设定: `|Z}2vo;j tfO#vw,@ 在菜单栏中选择Create/Element Primitive /plane uRV<?y% B^ 7eo W ~l[ra [I*!
lbt )(M7lq.e7 /u<nLj 1 元件半径为20mm*20,mm,距离坐标原点200mm。 \K2*Q&> gk0.zz([ 光源创建: $rB3m~c| 3Hi+Z}8 光源类型选择为任意平面,光源半角设定为15度。
-T@`hk` T.e.{yO yBpk$ 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。 \;5\9B"i s54nF\3V 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。 +|cI:|H> $m$;v<PSe XKOUQc4!R 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。 Z3KO90O!8 ,U,By~s 创建分析面: :fcM:w& .1 )RW5|c %V!iQzL1 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。 x+5k
<Xi} gO?44^hMe NR%Y+8^M 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。 }Rvm &?~O H;ZHqcUX FRED在探测器上穿过多个像素点迭代来创建热图 /hW d/H] <E|s\u 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。 |iYg > 将如下的代码放置在树形文件夹 Embedded Scripts, +]xFoH
0Wvq>R.(]7 Ue:z1p;g 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。 >B -q@D JNI>VP[c 绿色字体为说明文字, rM}0%J' +YY8h>hj '#Language "WWB-COM" cc=gCE 'script for calculating thermal image map UM%o\BiO 'edited rnp 4 november 2005 FwAKP>6 * \kIMDg3} 'declarations Et2JxbD Dim op As T_OPERATION CBT>"sYE1 Dim trm As T_TRIMVOLUME ^ZeJ[t&!# Dim irrad(32,32) As Double 'make consistent with sampling 9v)%dO. Dim temp As Double 0BPMmk Dim emiss As Double 7v}x?I Dim fname As String, fullfilepath As String Wl"0m1G D87|q4 'Option Explicit yTM3^R( F!!N9VIC Sub Main NW9n 'USER INPUTS 7k%T<;V nx = 31 sd re#@n} ny = 31 'XOX@UH d numRays = 1000 M(q'%XL^ minWave = 7 'microns ^n.WZUk maxWave = 11 'microns b4 #R! sigma = 5.67e-14 'watts/mm^2/deg k^4 8y'; \(; fname = "teapotimage.dat" `b5 @}', A1Y7;-D Print "" 34|a\b} Print "THERMAL IMAGE CALCULATION" ,8G{]X) hjx)D detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 Btt]R V}w;Y?]J Print "found detector array at node " & detnode !/{+WHxIr| x<i}_@Sn_+ srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 t%1 ^Li WP**a Bp Print "found differential detector area at node " & srcnode zzGYiF? 4pU>x$3$ GetTrimVolume detnode, trm R\Z:n* detx = trm.xSemiApe )u ?' ; dety = trm.ySemiApe Z(0@1l`Z-` area = 4 * detx * dety nxm$}!Df Print "detector array semiaperture dimensions are " & detx & " by " & dety '(&%O8Yi Print "sampling is " & nx & " by " & ny 6&U+6gb [&S}dQ" 'reset differential detector area dimensions to be consistent with sampling U!w1AY| pixelx = 2 * detx / nx "O>n@Q| pixely = 2 * dety / ny H&}ipaDO SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False p4u5mM Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 ,38Eq`5&W n_D8JF 'reset the source power N6oq90G SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) G28O%jD? Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" DrW#v-d Q-TV*FD. 'zero out irradiance array h( QYxI,| For i = 0 To ny - 1 }1 vT) For j = 0 To nx - 1 ewsKH\#
irrad(i,j) = 0.0 bEuaOBc Next j >"3>s% Next i *DI)? \g)Xt?w0Wo 'main loop !7B\Xl'S EnableTextPrinting( False ) ?|;yVew "v*8_El ypos = dety + pixely / 2 _+f+`]iM For i = 0 To ny - 1 =;~I_)Pg1 xpos = -detx - pixelx / 2 J<n+\F-s ypos = ypos - pixely "R
#k~R JMBK{J K> EnableTextPrinting( True ) pj|pcv^ Print i s0UFym8 EnableTextPrinting( False ) rPzQ8< ~89P[$6 .]4W!])9 For j = 0 To nx - 1 {2'm^0Kl XdEPbD- xpos = xpos + pixelx 3M*Bwt;F_ Si}HX!s 'shift source <g8K})P LockOperationUpdates srcnode, True !v#xb3"/ GetOperation srcnode, 1, op [(LV op.val1 = xpos .~lKBkS`! op.val2 = ypos I XA>`D SetOperation srcnode, 1, op `RQ#. LockOperationUpdates srcnode, False Nw J:! DdV'c@rq+ raytrace ,0$)yZ3*3, DeleteRays l":c CreateSource srcnode 8Q`WB0E<| TraceExisting 'draw ]J1S#Q5' 2R-A@UE2 'radiometry \~rlgxd For k = 0 To GetEntityCount()-1 dmrps+L If IsSurface( k ) Then rWtZj}A temp = AuxDataGetData( k, "temperature" ) $*[{J+t_ emiss = AuxDataGetData( k, "emissivity" ) CCijf]+ If ( temp <> 0 And emiss <> 0 ) Then Sywu=b ProjSolidAngleByPi = GetSurfIncidentPower( k ) K2_Qu't0$ frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) .o{0+fC# irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi hi=XYC, End If 4tA_YIv
^[:9fs End If EER`?Sa( ?q2j3e[> Next k p(SRjQt c2l_$p Next j H2gj=krK +y+"Fyl Next i I 1d0iU EnableTextPrinting( True ) Upl6:xYrG k?nQ?B
W 'write out file JF9yVE - fullfilepath = CurDir() & "\" & fname j'%4{n Open fullfilepath For Output As #1 C=Fzu&N} Print #1, "GRID " & nx & " " & ny >>d m}X Print #1, "1e+308" #PvB/3 Print #1, pixelx & " " & pixely Huw\&E Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 2U
kK0ls :S@1 maxRow = nx - 1 vQV K$n` maxCol = ny - 1 `i~ Y Fr For rowNum = 0 To maxRow ' begin loop over rows (constant X) l|`9:H row = "" XK(`mEi
For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) f67NWFX row = row & irrad(colNum,rowNum) & " " ' append column data to row string 1B>V t*= Next colNum ' end loop over columns <<A`aU^fX ^(}585b Print #1, row <3PL@orO EUYCcL'G Next rowNum ' end loop over rows %b.UPS@I Close #1 Gnm4gF!BI WnFG{S{s Print "File written: " & fullfilepath ChryJRuwv5 Print "All done!!" 31+;]W=
End Sub }G46g#_6d> v<\A% 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: ?eV(1Fr@ ^62|d +Z2MIC|Ud 找到Tools工具,点击Open plot files in 3D chart并找到该文件 <|O^>s; DH DZ_t: ;32#t[ib 打开后,选择二维平面图: #BK 9 k>i 4Q=ftY<
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