-
UID:317649
-
- 注册时间2020-06-19
- 最后登录2026-02-27
- 在线时间1928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。 b09xf"D M6^
\LtFt 成像示意图 2/uZ2N|S 首先我们建立十字元件命名为Target g7*Uuh# -38"S;M8 创建方法: ;Oqf{em]; P3Lsfi. 面1 : xa<KF 面型:plane c_M[>#` 材料:Air Hs:zfvD 孔径:X=1.5, Y=6,Z=0.075,形状选择Box d
ePk}Sn "e8EA!Ipte o9]32l 辅助数据: dJJq]^| 首先在第一行输入temperature :300K, _;Xlw{FN^ emissivity:0.1; 0R[fH y"'p#j a7F_{Mm 面2 : L%Rw]=v}v 面型:plane #\QW <I#/ 材料:Air W;UPA~nT~ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box Y&U-d{" 5dN>Xjpu l5&5VC) 位置坐标:绕Z轴旋转90度, =N{?ll6x7g @fp@1n lX"m|W 辅助数据: RLF6Bc ]Sa#g&}T> 首先在第一行输入temperature :300K,emissivity: 0.1; S#B%[3@ +_cigxpTc YI"!&a'yj Target 元件距离坐标原点-161mm; a3\~AO H% Us'JMZ~ "5
~{ 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 &y=OZ
!M I]+
zG e7{6<[k3+$ 探测器参数设定: vo\'ycPv t,8?Tf+i 在菜单栏中选择Create/Element Primitive /plane RH _b R+(f~ j' F1- "yX1B 6'/Zq ;nW;M 4{ Tgtym"=xd 元件半径为20mm*20,mm,距离坐标原点200mm。 _BerHoQd [7gz?9VyLF 光源创建: 2)|=+DN; |UWIV 光源类型选择为任意平面,光源半角设定为15度。 Oy=0Hsh@x \y=28KKc:c A>upT' 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。 8w:mL^6x (:`4*xK
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。 @S}j=k Ua
6O~,\ H%U 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。 #I0FWZ>W X;6;v] 创建分析面: =0Y0o_ qg`ae OF']- 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。 &`n:AR` Qu=b-9 sGtxqnX:J 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。 JluA?B7E 1)
2-UT FRED在探测器上穿过多个像素点迭代来创建热图 \ 9V_[xD+ p qpsa' 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。 D3dh,&KO\ 将如下的代码放置在树形文件夹 Embedded Scripts, \M@IKE u;rmqo1 .U|'KCM9m 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。 _zM?"16I} YQd($ 绿色字体为说明文字, yy8BkG( @^ YXE, '#Language "WWB-COM" H.{Fw j4 'script for calculating thermal image map y< dBF[ 'edited rnp 4 november 2005 ((`{-y\K Wc+(xk 'declarations 6 *S/frE Dim op As T_OPERATION X{Vs Dim trm As T_TRIMVOLUME H#hpaP; Dim irrad(32,32) As Double 'make consistent with sampling E`^D9:3:) Dim temp As Double gTTKjlI[ Dim emiss As Double r5hkxk' Dim fname As String, fullfilepath As String uuFQTx)) 3T]cDVQ_ 'Option Explicit rqN+0CT kDmuj>D Sub Main M=;csazN 'USER INPUTS 4+d(d nx = 31 #BBDI ny = 31 XZ@+aG_%q numRays = 1000 L{>rN`{ minWave = 7 'microns ,.*Df)+ maxWave = 11 'microns e> 9X sigma = 5.67e-14 'watts/mm^2/deg k^4 ,{q#U3 fname = "teapotimage.dat" V*te8HIe 'G % ]/'_U Print "" k&t.(r\ Print "THERMAL IMAGE CALCULATION" 2oahQ:
}B UQh.o detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 e#mf{1& ivl %%nY' Print "found detector array at node " & detnode &4WA/'>R $X)|`$#pL# srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 |#cqxr " |?0MRX0'g Print "found differential detector area at node " & srcnode v ,h"u l
7dm@S GetTrimVolume detnode, trm i.On{nB"k detx = trm.xSemiApe !F}GSDDV* dety = trm.ySemiApe Q!IqvmO area = 4 * detx * dety ;rL1[qwk Print "detector array semiaperture dimensions are " & detx & " by " & dety X!z-J> Print "sampling is " & nx & " by " & ny xu-bn BRu}"29 'reset differential detector area dimensions to be consistent with sampling r]\[G6mE% pixelx = 2 * detx / nx "u~` ZV( pixely = 2 * dety / ny _UkBOJ:G$H SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False N@<-R<s^ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 #| gh Ofoh4BL'1@ 'reset the source power Kzq^f=p SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) !WlL RkwO Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" R{A$|Ipaq Sb2_&5 'zero out irradiance array OzC%6;6h For i = 0 To ny - 1 4|\M`T For j = 0 To nx - 1 >+i+_^] irrad(i,j) = 0.0 K9&Q@3V Next j f&5S`}C Next i Xqm?@JN E x_dqko 'main loop 'M? ptu?f EnableTextPrinting( False ) 'NjeF6 5GJkvZtFY ypos = dety + pixely / 2 Iy*Q{H3[ For i = 0 To ny - 1 j&S.k xpos = -detx - pixelx / 2 *HV_$^)= ypos = ypos - pixely &*O'qOO<2 M9Sj@ ww EnableTextPrinting( True ) G2!<C-T{2 Print i RJDk7{( EnableTextPrinting( False ) qu$FpOJ
zD8$DG8 o\Fv~^ For j = 0 To nx - 1 _M7|:* 0;`FS/[(f xpos = xpos + pixelx M{)eA<6 ircL/: 'shift source IR2Qc6+{ LockOperationUpdates srcnode, True d?YSVmG GetOperation srcnode, 1, op ^e]O
>CJ op.val1 = xpos MoiRAO op.val2 = ypos Bmt8yR2 SetOperation srcnode, 1, op ?@MY +r_G LockOperationUpdates srcnode, False QjpJIw _N|AI"sj. raytrace J]S6%omp> DeleteRays 4J=6U&b CreateSource srcnode _M;{}!Gc&A TraceExisting 'draw @*6_Rp"@ }NV<k 'radiometry Ax@7RJ|| For k = 0 To GetEntityCount()-1 (C`nBiL< If IsSurface( k ) Then Ik5-ooZ&{ temp = AuxDataGetData( k, "temperature" ) ~tW<]l7 emiss = AuxDataGetData( k, "emissivity" ) ^l
;Bo3^_ If ( temp <> 0 And emiss <> 0 ) Then 1v3 ProjSolidAngleByPi = GetSurfIncidentPower( k ) &DtI+)[| frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) _E-{*,7bZS irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi gLo&~|=L- End If
}7fzEo`g r}|)oG,= End If W S9:*YH u0[O /G Next k /K+;HAUTn Ft :_6T% Next j ]5ibg"{S ~<Wa$~oY Next i @\-*aS_8> EnableTextPrinting( True ) Rdd9JJsVd }+[!h=Bx 'write out file X^m@*,[s fullfilepath = CurDir() & "\" & fname
#^-'q`) Open fullfilepath For Output As #1 0}kvuuR Print #1, "GRID " & nx & " " & ny .OW5R* Print #1, "1e+308" \j
we Print #1, pixelx & " " & pixely kY4h-oZ Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 GV9pet89yu RdpOj >fT maxRow = nx - 1 2Qp]r+! maxCol = ny - 1 @k:@mzB7R For rowNum = 0 To maxRow ' begin loop over rows (constant X) j6 _w2 row = "" rg%m For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) r|3u]rt row = row & irrad(colNum,rowNum) & " " ' append column data to row string iN@|08 Next colNum ' end loop over columns q7rX4-G$ wlP%
U Print #1, row >Mm.MNU 98{n6$\ Next rowNum ' end loop over rows $K|2k7 Close #1 n2F*a M&/e*Ta5 Print "File written: " & fullfilepath :}v:=c k Print "All done!!" QX(t@VP End Sub d;r,?/C 8h|~>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: Au )%w 6H|T ) ZU9Rvtb KB 找到Tools工具,点击Open plot files in 3D chart并找到该文件 Mw;^`ZxT " M&zW& W;,RU8\f 打开后,选择二维平面图: B=%YD"FAv b0/[+OY
|