-
UID:317649
-
- 注册时间2020-06-19
- 最后登录2025-11-25
- 在线时间1891小时
-
-
访问TA的空间加好友用道具
|
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。 /}Y>_87 !c\d(u 成像示意图 k|,pj^ 首先我们建立十字元件命名为Target OedL?4 K^k1]!W= 创建方法: 02} &h oQ 5g0(J~ 面1 : J56+eC( 面型:plane IEdC
_6G 材料:Air !=#E/il, 孔径:X=1.5, Y=6,Z=0.075,形状选择Box u7&r'rZ1_! !Ljs9 =UF y5.Z <Y 辅助数据: mk1;22o{TX 首先在第一行输入temperature :300K, Ay!=Yk^~ emissivity:0.1; vt[4"eU _`L,}=um' f8)D| 面2 : sf]y\_zU 面型:plane k'wF+> 材料:Air E) >~0jv 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 0yXUVKq3 > >wbyj8 ]6</{b 位置坐标:绕Z轴旋转90度, @<\f[Znto %FQMB >/EmC3?b! 辅助数据: /g712\?M4 'bkecC 首先在第一行输入temperature :300K,emissivity: 0.1; ,-t3gc1~X Y*O7lZuF% er^z:1' Target 元件距离坐标原点-161mm; B} gi / X4&{/;$ b/ 'fC%o, 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 q~r)B} ^DVr>u 5SK{^hw 探测器参数设定: r~u/M0h ` ?{$Q'c_I 在菜单栏中选择Create/Element Primitive /plane U
n2xZ[4 }.4`zK&SB |v}"UW(y O$Wt\Y<q jwTb09 \rcbt6H
元件半径为20mm*20,mm,距离坐标原点200mm。 [Ym?"YwVX UMo=bs 光源创建: 09 eS&J<R @h
X 光源类型选择为任意平面,光源半角设定为15度。 |h*H;@$ J:'cj5@ ,|"tLN*m 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。 ME1lQ7E4B ]OM|Oo 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。 9<WMM) t'_Hp}, P`5@$1CJ 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 .jZmQtc <dD}4c+/t 创建分析面: /lm;.7_J+ 4t|g G`QW7 LS Na 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 R"Hhc(H a
=*(>= p<'#f,o 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 "QA# ~LuZpV FRED在探测器上穿过多个像素点迭代来创建热图 z;GnQfYG '[~NRKQJ FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 ,4jkTQ*@2 将如下的代码放置在树形文件夹 Embedded Scripts, CwTx7
^qa Q{UR3U'Q fr;>`u[; 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 za1MSR 4VSlgoz 绿色字体为说明文字, ?7@B$OlU _,=A\C_b@ '#Language "WWB-COM" >,y291p2 'script for calculating thermal image map )~T)$TS 'edited rnp 4 november 2005 XN5EZ# a:Y6yg%1> 'declarations `ndesP Dim op As T_OPERATION
VD;Ot<% Dim trm As T_TRIMVOLUME nY'0*:'u Dim irrad(32,32) As Double 'make consistent with sampling b>hNkVI Dim temp As Double -f#0$Z/0 Dim emiss As Double x:88E78 Dim fname As String, fullfilepath As String ~_QZiuq& M3o dyO( 'Option Explicit 'LpJ:Th ~jH@3\
?- Sub Main '~VKH}b 'USER INPUTS "2i{ L ' nx = 31 2^bq4c4J ny = 31 ,fpu@@2 numRays = 1000 xM8}Xo minWave = 7 'microns ';hU&D;s maxWave = 11 'microns JC(rSs* sigma = 5.67e-14 'watts/mm^2/deg k^4 X,IjM&o"Y fname = "teapotimage.dat" Yewn -/ ;y*mP Print "" @vss:'l Print "THERMAL IMAGE CALCULATION" -X'HZ\) M")J buI detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 AMG}'P: =dHM)OXD" Print "found detector array at node " & detnode WM.JoQ S 3Tp__ srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 UQ:H3 Gi~p-OS, Print "found differential detector area at node " & srcnode >N@tInE +(x^5~QX GetTrimVolume detnode, trm .X\p;~H
5 detx = trm.xSemiApe %%`Nq&' dety = trm.ySemiApe n1 =B area = 4 * detx * dety U s86.@| Print "detector array semiaperture dimensions are " & detx & " by " & dety 8*!<,k="9 Print "sampling is " & nx & " by " & ny 8>x!n/z) <gF=$u|}3[ 'reset differential detector area dimensions to be consistent with sampling uz-,) pixelx = 2 * detx / nx VLC<ju! pixely = 2 * dety / ny S_/9eI~X SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False ym9Z:2g
Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 QG*=N {%5 -=iGl5P? 'reset the source power MP(R2y SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) XE*
@* Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" z6ISJb veAg?N<c
p 'zero out irradiance array k{;"Aj:iL For i = 0 To ny - 1 0?KXQD For j = 0 To nx - 1 +~?ze,Di irrad(i,j) = 0.0 U`N|pPe:w Next j (+68s9XS7 Next i ."&,_F GL[#XB>n 'main loop <nlZ?~%} EnableTextPrinting( False ) rl4B(NZi} ig<Eyr ypos = dety + pixely / 2 Tm(XM< For i = 0 To ny - 1 :i_818h!?[ xpos = -detx - pixelx / 2 _x&;Fa% ypos = ypos - pixely qYR
$5 wwrP7T+d EnableTextPrinting( True ) dU1w)Y Print i W^npzgDCo EnableTextPrinting( False ) :,gnOfV= ("Z;)s4q 7 4Xk^8 For j = 0 To nx - 1 v,y nz'>) uPKq<hBI xpos = xpos + pixelx 4)0 %^\p mR@|] T 'shift source \95qH,w)T LockOperationUpdates srcnode, True vQ/}E@?u GetOperation srcnode, 1, op ph{p[QI:{X op.val1 = xpos 9pUvw_9MY op.val2 = ypos B!-hcn]y SetOperation srcnode, 1, op HeABU(o4 LockOperationUpdates srcnode, False .Uq?SmK rCfr&>nn raytrace ~,+n_KST; DeleteRays W,"|([t4.\ CreateSource srcnode x2x)y08 TraceExisting 'draw w}No ^.I*4 cpvN
}G 'radiometry Wt5x*p-!C For k = 0 To GetEntityCount()-1 Py7!_TX If IsSurface( k ) Then 6hDK;J J& temp = AuxDataGetData( k, "temperature" ) ]T|9>o! emiss = AuxDataGetData( k, "emissivity" ) QR4rQu If ( temp <> 0 And emiss <> 0 ) Then uw! ProjSolidAngleByPi = GetSurfIncidentPower( k ) h07Z.q ; frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) e9e%8hL irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi W%LTcm End If 2{;&c 9rXbv4{ End If Z0&^U#] 88}+.-3t$ Next k }/~%Ysl rt">xVl Next j RrrW0<Ed t`NZ_w / Next i _svEPHU EnableTextPrinting( True ) f!6oW( r-L +Go(yS 'write out file 5v"r>q[
X fullfilepath = CurDir() & "\" & fname 3sG7G:4 Open fullfilepath For Output As #1 Oop5bg Print #1, "GRID " & nx & " " & ny V.zKjoky@ Print #1, "1e+308" q-s! hiK Print #1, pixelx & " " & pixely q/y4HT,x Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 272j$T L9tjHC] maxRow = nx - 1 ,M2u (9 maxCol = ny - 1 XMhDx For rowNum = 0 To maxRow ' begin loop over rows (constant X) @X`~r8& row = "" AA][}lU:5 For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) [MSLVTR row = row & irrad(colNum,rowNum) & " " ' append column data to row string 9~+A<X]Hd Next colNum ' end loop over columns n]M1'yU |GuIp8~ Print #1, row Jf\lnJTyU8 s_]p6M Next rowNum ' end loop over rows sYV7t*l Close #1
.G}E rZRcy9$y> Print "File written: " & fullfilepath JQ{g'cT Print "All done!!" GwiG..Y]& End Sub 3:Bwf)* -H1mKZDPP 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: 89@\AjI ~3}Gu^@ #Mo`l/Cwp 找到Tools工具,点击Open plot files in 3D chart并找到该文件 IV{,'+hT 36>pa IOA"O9; 打开后,选择二维平面图: (;u tiupW Y"
9 o
|