| infotek |
2020-11-18 10:58 |
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。 _ p?q/-[4 _]<]:b
成像示意图 SkK=VeD>8 首先我们建立十字元件命名为Target 6!bf,T] =B;)h 创建方法: 9J>DLvl; QJv,@@mu 面1 : lRO4-
y 面型:plane x.d9mjLN8m 材料:Air ncWASw` 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ?"L>jr( [rQ#skf
Jcy`:C\Ay 辅助数据: D$j`+` 首先在第一行输入temperature :300K, "Uyw7 emissivity:0.1; FMR0?\jnT oVLz7Y[JE MY0Wr%@#0 面2 : (Q\w4?ci 面型:plane <1hwXo 材料:Air cW MZw|t 孔径:X=1.5, Y=6,Z=0.075,形状选择Box )of_"gZ$3A SBYRN##n_ u'=#~'6 位置坐标:绕Z轴旋转90度, g:O.$ z`TI<B
xvgIYc{ 辅助数据: IQH;`+ ma-|L3 # 首先在第一行输入temperature :300K,emissivity: 0.1; f(9w FT FL` . (, zmuq4-. Target 元件距离坐标原点-161mm; dso\+s FCI38?`%
\ 0:ITz 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 #'"h+[XY .}Xkr+
+] V,2O`D% 探测器参数设定: #ReW#?P%b/ #?aR,@n 在菜单栏中选择Create/Element Primitive /plane \Ud2]^D= TN l$P~X>
J,IOp- vnIxI a DrW]`%Ql <KJ18/ 元件半径为20mm*20,mm,距离坐标原点200mm。 ]ImS@!Ajjx 71wyZJ 光源创建: 4,)=r3;&! N\H(AzMw 光源类型选择为任意平面,光源半角设定为15度。 dLjT^ 9 !WDdq_n*v !3Pl]S~6! 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。 }P^n / fV[xv4D. 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。 z?V > ST M?]ObIM:5 `7'(U)x,F 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。 O 89BN6p e_,_:|t 创建分析面: j^LnHVHk1 6W3}6p aHb,4 wY 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。 7O"T`> _Hkc<j/e~
lJq
%me;4m 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。 -[+FVvS W/J3sAYv FRED在探测器上穿过多个像素点迭代来创建热图 CVu'uyy tMupX-V 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。 ,/Xxj\i 将如下的代码放置在树形文件夹 Embedded Scripts, $KtMv +m" 7_A(1Lx/l7
w/ZV9"BhE 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 .o
fYFK A(<-
U| 绿色字体为说明文字, [;};qQ-C2 \7W {/v4^ '#Language "WWB-COM" Z73 ysn} 'script for calculating thermal image map n)
`4*d$` 'edited rnp 4 november 2005 @ /c{gD egKYlfe" 'declarations _*&<hAZj Dim op As T_OPERATION YMz[je Dim trm As T_TRIMVOLUME KA.@q AEB Dim irrad(32,32) As Double 'make consistent with sampling 0z\=uQ0 Dim temp As Double b/E1v,/< Dim emiss As Double k%uRG_ Dim fname As String, fullfilepath As String tjYe82 ox)/*c< 'Option Explicit '?Hy"5gUA hydn" 9; Sub Main ?ILNp`k 'USER INPUTS R:OoQ^c nx = 31 8CMI\yk ny = 31 g"<kj" numRays = 1000 Hs2L$TX minWave = 7 'microns 'L= g( maxWave = 11 'microns v82@']IN sigma = 5.67e-14 'watts/mm^2/deg k^4 $8X?|fV) fname = "teapotimage.dat" Z;lE-`Z*(F ISOPKZ#F Print ""
%lEPFp Print "THERMAL IMAGE CALCULATION" 5E~][. d OB5{EILej detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 'gQm%:qU3r %_}#IS1 Print "found detector array at node " & detnode Fa@#nY|UV3 gl00$}C srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 $D8KEkW Pq;1EI Print "found differential detector area at node " & srcnode )W uuU [( R%}OZJ_ GetTrimVolume detnode, trm cLJ|VD7 detx = trm.xSemiApe ]ujH7T dety = trm.ySemiApe 7Nx@eoZ area = 4 * detx * dety 4W$53LP8 Print "detector array semiaperture dimensions are " & detx & " by " & dety us$~6 Print "sampling is " & nx & " by " & ny -%"MAIJnX 8={(Vf6 'reset differential detector area dimensions to be consistent with sampling
k|a{|2p pixelx = 2 * detx / nx Cl i k pixely = 2 * dety / ny (r:WG!I, SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False oM QH-\(} Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 "RZ)pav? 0jE,=<W0> 'reset the source power tz._*n83 SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) =yfr{5}R Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" :P;#Y7}Y$ h jWRU# 'zero out irradiance array V?5QpBKI For i = 0 To ny - 1 &<k)W For j = 0 To nx - 1 5+giT5K*h irrad(i,j) = 0.0 T%-F,i Next j Q
>)?_O( Next i Vs\)w>JF 2.?:[1g! 'main loop I0GL/a4s EnableTextPrinting( False ) o]PSyVg Y~gpi L3u ypos = dety + pixely / 2 rDm>Rm= For i = 0 To ny - 1 o%Pi;8 xpos = -detx - pixelx / 2 "fS9Nx3 ypos = ypos - pixely CM8WI~ +oe
~j\= EnableTextPrinting( True ) KiH#*u S Print i [ZDJs`h!` EnableTextPrinting( False ) %|r@q tE<L4;t Lp1wA* For j = 0 To nx - 1 Ff%m.A8d,4 {Yv
|C)O xpos = xpos + pixelx ~"+[VE5 irgjq/&d 'shift source |LiFX5!\ LockOperationUpdates srcnode, True 3l<)|!f]g GetOperation srcnode, 1, op &A=d7ASN= op.val1 = xpos $aG]V-M> op.val2 = ypos \MK)dj5uUJ SetOperation srcnode, 1, op D[:7B:i LockOperationUpdates srcnode, False ||9f@9 Ba!`x<wa 'raytrace 8t0i
j DeleteRays JnV$)EYi CreateSource srcnode mS!/>.1[ TraceExisting 'draw r 3pfG {%b>/r 'radiometry ,&z_ 2m For k = 0 To GetEntityCount()-1 -D38>#Y If IsSurface( k ) Then vTU"c>] temp = AuxDataGetData( k, "temperature" ) -V_e=Y<J/ emiss = AuxDataGetData( k, "emissivity" ) r(%#@?& If ( temp <> 0 And emiss <> 0 ) Then klv^310 ProjSolidAngleByPi = GetSurfIncidentPower( k ) WNlWigwYl frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) T-f+<Cxf irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi |;9OvR> A End If
2Xe2%{ LTBqXh End If in(n[K [ivJ&'vB Next k h`&mW w ;(VJZ_ Next j ++Az~{W7 6;[iX`LL Next i @*A(#U8p3 EnableTextPrinting( True )
E2!;W8M >SSF:hI"J 'write out file SYa!IL-B fullfilepath = CurDir() & "\" & fname /ExnW >wT Open fullfilepath For Output As #1 dKZffDTZ Print #1, "GRID " & nx & " " & ny ikyvst>O Print #1, "1e+308" Z+I[ Print #1, pixelx & " " & pixely [rE,fR Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 k.
px PyzWpf maxRow = nx - 1 sL+/Eeb` c maxCol = ny - 1 U%w?muJW For rowNum = 0 To maxRow ' begin loop over rows (constant X) yd`.Rb&V row = "" +#'exgGU^[ For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) <Pg.N row = row & irrad(colNum,rowNum) & " " ' append column data to row string 1fEV^5I Next colNum ' end loop over columns GS<,adD lZ/Yp~2S Print #1, row Q9FY.KUM vTP'\^; Next rowNum ' end loop over rows RHVMlMX Close #1 ]5uCs[ \T<?=A Print "File written: " & fullfilepath .VTHZvyn Print "All done!!" 19;\:tN End Sub :N%]<Mq V&)-u(s_S/ 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: IjJ3CJ< AR/`]"' J}%&;uv
找到Tools工具,点击Open plot files in 3D chart并找到该文件 UO>p-M L!-T`R8'c "m/0>UU0 打开后,选择二维平面图: 'OkF.bs g%[lUxL
QQ:2987619807 eUx|_*`
|
|