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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。 C2v_],] ([<HFc` 成像示意图 S}%z0g< 首先我们建立十字元件命名为Target @g5y_G{SP d:K\W[$Bz 创建方法: QE[<Y3M `<se&IZE 面1 : =cjO] 面型:plane pl&nr7\ 材料:Air QWfSm^
t 孔径:X=1.5, Y=6,Z=0.075,形状选择Box fuUtM_11 S5 q1Mn ySO\9#Ho 辅助数据: 7mMGH( 首先在第一行输入temperature :300K, .UL2(0 emissivity:0.1; qovsM M MYy58N Bgc]t 面2 : mXyP;k 面型:plane oHx:["F 材料:Air H"AL@= 孔径:X=1.5, Y=6,Z=0.075,形状选择Box B1nm?E 0i ~ `qWEu g[pU5%|"[ 位置坐标:绕Z轴旋转90度, \vT~2Y(K e~lFjr] @y;VV* 辅助数据: t7F0[E'=5\ !X-\;3kC0 首先在第一行输入temperature :300K,emissivity: 0.1; pPRX#3 Q+
V<& )f:i4.M Target 元件距离坐标原点-161mm; tpcB}HUv .i4aM;Qy lgU!D |v 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 X<;. f't.?M *FC8=U2\X 探测器参数设定: ,R`CAf%* Pqya%j 在菜单栏中选择Create/Element Primitive /plane bOr11? Nz`8)Le (?1$ :Pdh##k K.}jOm (rBsh6@) 元件半径为20mm*20,mm,距离坐标原点200mm。 `Uz.9_6 *Sj)9mp 光源创建: 06.%9R{ [y`Gp# 光源类型选择为任意平面,光源半角设定为15度。 6P
_+:Mf X.4WVI W$hCI)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。 jD S\ :
Z<\R0 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。 x/<]/D nb/q!8 9abUh3 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。 ZSQiQ2\) yg}O9!M J 创建分析面: s|<n7 =J cwzkA,e@ ?`?Tg&W 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。 ]gPx%c Hu<]*(lK% j13-?fQ& 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。 n zaDO-2! *x2!N$b FRED在探测器上穿过多个像素点迭代来创建热图 BGibBF^ 9y6u&!PZ\ FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 |=IJ^y(x| 将如下的代码放置在树形文件夹 Embedded Scripts, @3c'4O
/Kli C\ d {U%q
d 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 yP$esDP _oc6=Z 绿色字体为说明文字, 8X`DFeJ 6Z#Nh@!+C '#Language "WWB-COM" 4utwcXL 'script for calculating thermal image map }V]b4t 'edited rnp 4 november 2005 n+=qT$w) ?+hEs =Xs 'declarations Jp"29
)w Dim op As T_OPERATION eWv:wNouk Dim trm As T_TRIMVOLUME O/#3QK Dim irrad(32,32) As Double 'make consistent with sampling BT[|f[1 Dim temp As Double ASy?^Jrs5 Dim emiss As Double apm%\dN Dim fname As String, fullfilepath As String *Ze0V9$' bQ3<>e\%B 'Option Explicit }b54O\, *.nSv@F Sub Main HQ"T>xb 'USER INPUTS cL#-vW<s3 nx = 31 ^?Xs!kJP ny = 31 [G8EX3 numRays = 1000 $Be hU minWave = 7 'microns +&u/R')?6r maxWave = 11 'microns "W+>?u ) sigma = 5.67e-14 'watts/mm^2/deg k^4 y_L8i[ fname = "teapotimage.dat" Ich^*z(F$ Zm*d)</> Print "" 4$VDJ Print "THERMAL IMAGE CALCULATION" 5?H8?~&dz >+7{PF+sB detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 "v?F4&\ 8 _s@PL59, Print "found detector array at node " & detnode e4=FO;% ':_9o5I srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 +:^l|6%} EoJ\Jk Print "found differential detector area at node " & srcnode 9+9g (6 '/qy_7O GetTrimVolume detnode, trm H'#06zP>5 detx = trm.xSemiApe 8:c=h/fa
dety = trm.ySemiApe $Z)u04;&@ area = 4 * detx * dety 4#>Z.sf Print "detector array semiaperture dimensions are " & detx & " by " & dety KS(H_&j Print "sampling is " & nx & " by " & ny ^=^\=9"
b lv/im/]v 'reset differential detector area dimensions to be consistent with sampling k F^4kCJ@ pixelx = 2 * detx / nx B0|W pixely = 2 * dety / ny =cV|o] SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False /v9qrZ$$ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 0^S$_L ;8PO}{rD 'reset the source power GFLat SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 0'6ai=W Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" 4F.,Y3 `l'T/F\ 'zero out irradiance array 55s5(]`d For i = 0 To ny - 1 :AlvWf$d For j = 0 To nx - 1 :qxWANUa irrad(i,j) = 0.0 ORrZu$n`p Next j 'i$._Tx Next i V/H+9+B7Im (<>??(VM 'main loop z4_B/Q EnableTextPrinting( False ) Ojz'p5d`> @.E9ml ypos = dety + pixely / 2 '6vo#D9M For i = 0 To ny - 1 o@gceZuk xpos = -detx - pixelx / 2 D+:s{IcL< ypos = ypos - pixely AP%R*0] QWa@?BO2p EnableTextPrinting( True ) y}oA!<#3 Print i /7"V~c6 EnableTextPrinting( False ) b?OA |JqX az![u) ^G`6Zg;
For j = 0 To nx - 1 }*rS g . A^M]vk%dg xpos = xpos + pixelx |dEPy-Xe 67&IaDts 'shift source zZPWE"u} LockOperationUpdates srcnode, True 8y6dT GetOperation srcnode, 1, op _+9i op.val1 = xpos EpG9t9S9 op.val2 = ypos eE'>kP} SetOperation srcnode, 1, op ]QR]#[Tn' LockOperationUpdates srcnode, False 'kj
q C uQH] 'raytrace
*~
I HVU DeleteRays VD&wO'U CreateSource srcnode )/DN>rU TraceExisting 'draw jj2=|)w$3 &iw,||# 'radiometry Wjq9f; For k = 0 To GetEntityCount()-1 J \|~k2~ If IsSurface( k ) Then p5E
okh temp = AuxDataGetData( k, "temperature" )
Hy:x.'i emiss = AuxDataGetData( k, "emissivity" ) _Jg#T~ If ( temp <> 0 And emiss <> 0 ) Then lz>00B<Z ProjSolidAngleByPi = GetSurfIncidentPower( k ) vkJyD/;= frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) M887 Q'HSi irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi |sr\SCx End If K_Y{50# *JX$5bZsI End If `^{G`es VtzZ1/JE Next k ]t!v`TH >WZ%Pv* Next j 'fK=;mM IWi0? V Next i i_m&qy<v EnableTextPrinting( True ) r6\g#} R5QW4i9 'write out file 2m*ugBO; fullfilepath = CurDir() & "\" & fname uq9mq" Open fullfilepath For Output As #1 mY"Dw^) Print #1, "GRID " & nx & " " & ny Tx&H1 Print #1, "1e+308" MHWc~@R Print #1, pixelx & " " & pixely 8*&-u +@% Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 ;DX{+Z[ X~m57bj maxRow = nx - 1 -SD:G]un
maxCol = ny - 1 Ay6T*Nu` For rowNum = 0 To maxRow ' begin loop over rows (constant X) 5YPIv- row = "" Mz$qe For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) gYbvCs8O! row = row & irrad(colNum,rowNum) & " " ' append column data to row string ;Co"bP's Next colNum ' end loop over columns m`zd0IRTP }`
`oojz Print #1, row h{-en50tN BeRs;^r+ Next rowNum ' end loop over rows D_<B^3w) Close #1
Rq| 5%;1 bZWR.</ Print "File written: " & fullfilepath sCy.i/y Print "All done!!" anz7ae&P'K End Sub pHVDug3 ;;UsHhbhI 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: JYjc^m !^L}LtqHI QP<P,Bi~ 找到Tools工具,点击Open plot files in 3D chart并找到该文件 .Sw4{m[g k(>J?\iNW q{*[uJ}Xc" 打开后,选择二维平面图: EX<1hAw _`QME r?
QQ:2987619807 ,agkV)H
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