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。 )U`
c9*. <V{BRRx
成像示意图 7w|s8B 首先我们建立十字元件命名为Target joq
;N]S tp"\ 创建方法: R.@GLx_zpQ RA}PM?D/ 面1 : jBM>Pe^`3 面型:plane )I@iW\`7 材料:Air :([,vO: 孔径:X=1.5, Y=6,Z=0.075,形状选择Box iVRz \c)XN<HH
%?seX+ne 辅助数据: |Cm}%sgR\0 首先在第一行输入temperature :300K, iBCM?RiG emissivity:0.1; ^H'#*b0u X'Oo ogu @gd-lcMYW 面2 : %zGPF 面型:plane [0$Y@ek[ 材料:Air w[XW>4xK 孔径:X=1.5, Y=6,Z=0.075,形状选择Box KE_Ze\P N{'k
]& -{?Rq'H 位置坐标:绕Z轴旋转90度, |kn}iA@72p ;8!D8o(+
.s+e
hZ 辅助数据: ?~$y3<[ <]<50 首先在第一行输入temperature :300K,emissivity: 0.1; U[ed#9l> *\>& uQDu<@5^[ Target 元件距离坐标原点-161mm; wFe</U-'; |laqy`D
2b<0g@~X 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 *oF{ R^ Gfvz%%>l eu~;G H 探测器参数设定: T@L^RaPX Sdn]
f4 在菜单栏中选择Create/Element Primitive /plane
@`T6\ 1 ;,<s'5icyg
|1neCP@ng (wTg aV1 Ruf*aF( 3cnsJV] 元件半径为20mm*20,mm,距离坐标原点200mm。 + 7Z%N9 hAY_dM 光源创建: ow&R~_ (Lc%G~{ 光源类型选择为任意平面,光源半角设定为15度。 cD 1p5U u+]zi"k^s 4:K9FqU 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。 g3y44GCV % $J^dF_0 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 Dx8^V%b Dd*C?6 J9o]$.e 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。 'RPe5 vB ]`lTkh 创建分析面: 2nf{2edC v"^G9u s}5;)>3~@ 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。 +UB. M 7,:QFV
m49)c K? 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。 VH8,!# Q; |d{4_o90 FRED在探测器上穿过多个像素点迭代来创建热图
Eg
;r]?|6 Cjw|.c` 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。 qLcs)&}/A 将如下的代码放置在树形文件夹 Embedded Scripts, [z/OY&kF &Y\`FY\
0(]C$*~mk 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 ?(E$|A fi1tF/` 绿色字体为说明文字, {`{U\w5Af %/4ChKf!VR '#Language "WWB-COM" |A"zxNeS" 'script for calculating thermal image map @xmL?wz 'edited rnp 4 november 2005 }e1f kjWk "zv?qS 'declarations -2f_e3jF Dim op As T_OPERATION KZ&{Ya Dim trm As T_TRIMVOLUME Fvg>>HVu Dim irrad(32,32) As Double 'make consistent with sampling oB+drDp8U Dim temp As Double PKmr5FB Dim emiss As Double p?ICZg: Dim fname As String, fullfilepath As String ^`ny]3JA g%Eb{~v 'Option Explicit rxt)l t}+P|$[ Sub Main d7A vx 'USER INPUTS 86oa>#opU nx = 31 ZPRkk?M}. ny = 31 %R." numRays = 1000
~8Z)e7j minWave = 7 'microns "H#2 maxWave = 11 'microns \s<L2uRj sigma = 5.67e-14 'watts/mm^2/deg k^4 xO{yr[x"L fname = "teapotimage.dat" ]%pr1Ey ibha` Print "" ><^
, Print "THERMAL IMAGE CALCULATION" uS;N&6;: |<gYzbq detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 qi!+Ceo} #L
ffmS Print "found detector array at node " & detnode _ ZMoPEW 0F/o srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 O!#r2Y"?K1 ;Lr]w8d Print "found differential detector area at node " & srcnode l]C#bL>i 0w)Gb}o$ GetTrimVolume detnode, trm s,Azcqem detx = trm.xSemiApe -Q9} gaH_ dety = trm.ySemiApe /6 QwV-> area = 4 * detx * dety jnho*,X Print "detector array semiaperture dimensions are " & detx & " by " & dety q8#zv_>K Print "sampling is " & nx & " by " & ny 4d-f6iiFV `|(S]xPHM 'reset differential detector area dimensions to be consistent with sampling /fv;`?~d* pixelx = 2 * detx / nx mQUI9 pixely = 2 * dety / ny C%H{" SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False ZOw%Fw4B Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 a]\l:r m) QV2n 'reset the source power -?nr q <3 SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) ZD ~ra7 Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" :J6 xYy$ lu vrv m 'zero out irradiance array 0i[v,eS For i = 0 To ny - 1 #83`T&Xw* For j = 0 To nx - 1 zo83>bt irrad(i,j) = 0.0 H< 51dJn~ Next j %[B^b)2 Next i Gu@n1/m@o Sq:,6bcG 'main loop 5Q7Z$A1a
9 EnableTextPrinting( False ) [3 D*DyQt M47t(9krV ypos = dety + pixely / 2 4]G J+a For i = 0 To ny - 1 .7BJq?K. xpos = -detx - pixelx / 2 AdD,94/ ypos = ypos - pixely *\gYs{, )[wB:kG EnableTextPrinting( True ) nEHmiG Print i WIKSz
{"=/ EnableTextPrinting( False ) \?tE,\Ln ~)CGwST[ 7D&O5Z=%+ For j = 0 To nx - 1 Ua%;hI)j$ pF/s5z xpos = xpos + pixelx QZ&
4W cS#yfN, 'shift source X{Ij30Bmv LockOperationUpdates srcnode, True V!\'7-[R GetOperation srcnode, 1, op ;"B@QPX op.val1 = xpos jZr"d*Y op.val2 = ypos *47HN7 SetOperation srcnode, 1, op HjCe/J ; LockOperationUpdates srcnode, False ?k`UQi]Q l=UXikx 'raytrace <P~pn!F} DeleteRays Tm\a%Z`U> CreateSource srcnode [[#zB-| TraceExisting 'draw S ^]mF>xX8 7bk`u'0% 'radiometry E5q t~:C| For k = 0 To GetEntityCount()-1 xL [3R
If IsSurface( k ) Then K2{6{X= temp = AuxDataGetData( k, "temperature" ) ~^bf1W[ emiss = AuxDataGetData( k, "emissivity" ) p~WX\; If ( temp <> 0 And emiss <> 0 ) Then _9yW; i- ProjSolidAngleByPi = GetSurfIncidentPower( k ) >N~orSw% frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) K;7ea47m N irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi )=nB32~J" End If ZZ>F ^t ,Cd4Q7T End If ?{L5=X@$$ {4 {X`$ Next k \
[bJ@f*." k%R(Qga Next j `
ZBOaN^if !i_~<6Wa7 Next i C<#_1@^:8e EnableTextPrinting( True ) 4k!>JQor <UY9<o 'write out file b,x$wP+ fullfilepath = CurDir() & "\" & fname / hg)=p Open fullfilepath For Output As #1 Z.`0 Print #1, "GRID " & nx & " " & ny RdB,;Um9f Print #1, "1e+308" P~84#5R1 Print #1, pixelx & " " & pixely d*x&Uh[K Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 c*r@QmB: r 6&+pSA> maxRow = nx - 1 Tol V3 maxCol = ny - 1 9"?;H%. For rowNum = 0 To maxRow ' begin loop over rows (constant X) a4XK.[O row = "" Ej $.x6: For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) \0K&2' row = row & irrad(colNum,rowNum) & " " ' append column data to row string <qVOd.9c Next colNum ' end loop over columns f\FqZ?w F$ckW'V Print #1, row >,.\`.0 3:<[;yo Next rowNum ' end loop over rows *x_e] /} Close #1 #r,!-;^'p XP[~ :+ Print "File written: " & fullfilepath 2UopGxrPKw Print "All done!!" <kJ`qbOU End Sub ;Fd1:"1pP %XQJ!sC` 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: ^A=2#j~H\ ve\@u@K^ (G~M E> 找到Tools工具,点击Open plot files in 3D chart并找到该文件 qT01@Bku nbW.x7 --k!KrL 打开后,选择二维平面图: %!DTq`F ZENblh8fs
QQ:2987619807 WpOH1[8v
|
|