| 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。 \=?a/ '8RsN-w
成像示意图 UqFO|r"M 首先我们建立十字元件命名为Target 2\A$6N;_ JgKO|VO 创建方法: -LoZs
ru U3ADsdn 面1 : f}#~-.NGs 面型:plane |C;=-| 材料:Air 0U(@=7V 孔径:X=1.5, Y=6,Z=0.075,形状选择Box G\/zkrxmv o]J{{M'E
<Dl*l{zba 辅助数据: \%JgH=@
:= 首先在第一行输入temperature :300K, DbBcQ% emissivity:0.1; j\[dx^\= [64:4/<} '%s.^kn 面2 : sQUM~HD\a 面型:plane 4x=v?g& 材料:Air a+[KI 孔径:X=1.5, Y=6,Z=0.075,形状选择Box :KSV4>X[%a <$A p,5i)nEFj 位置坐标:绕Z轴旋转90度, v+W&9> vjbASFF0=
,8S/t+H 辅助数据: ''A_[J `> |k )=0mCz 首先在第一行输入temperature :300K,emissivity: 0.1; YFLZ %( SB;&GHq"n YiXk5B0Uh Target 元件距离坐标原点-161mm; Fd%#78UEo} j"t(0m
|{z:IQLv 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 4qb/daE:Z gDQ^)1k MD}w Y><C 探测器参数设定: wjU9ZGM 7cuE7" 在菜单栏中选择Create/Element Primitive /plane m<<+ QGMV}y
NlA,'`, e[{0)y>= S*,17+6dV gldAP: 元件半径为20mm*20,mm,距离坐标原点200mm。 poc`q5i+ Z\(q@3 C 光源创建: f$o_e90mu SpIv#? 光源类型选择为任意平面,光源半角设定为15度。 |QF7
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}a`0Y&{ 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 pE3?"YO 3p$?,0ELH 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。 :p1u(hflS =1@u 0gu_yg! R 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。 vRYQ{: T )&A2q 创建分析面: ^7`BP%6 (=FRmdeYl1 dUD[e,? 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。 4V"E8rUL( lwR<(u31e
Q8$}@iA[ 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。 "-Mp_O] ;_XFo&@ FRED在探测器上穿过多个像素点迭代来创建热图 !K#qe Y} %6t:(z 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。 }t!Gey 将如下的代码放置在树形文件夹 Embedded Scripts, ;'gWu \Zb;'eDv
2/U.|*mH 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。 qfX6TV5J}! ~EW(Gs!=C 绿色字体为说明文字, \wmN g%aYDl '#Language "WWB-COM" ~\r* 'script for calculating thermal image map C;v.S5x 'edited rnp 4 november 2005 xnjf hy9\57_# 'declarations #j;^\rSv- Dim op As T_OPERATION UklUw Dim trm As T_TRIMVOLUME )J=! L\ Dim irrad(32,32) As Double 'make consistent with sampling \-E^lIVF Dim temp As Double v6|RJt? Dim emiss As Double S*pGMuui Dim fname As String, fullfilepath As String pt?bWyKG 3s*mbk[J 'Option Explicit UB@Rs|) $Ph|e)p Sub Main [\]50=& 'USER INPUTS K&u_R
nx = 31 C-xr"]#] ny = 31 *9
{PEx numRays = 1000 O}gV`q; minWave = 7 'microns 5; C| maxWave = 11 'microns 4>YR{ sigma = 5.67e-14 'watts/mm^2/deg k^4 Fk7?xc fname = "teapotimage.dat" 39c2pV[ t[HE6ea Print "" P-[-pi@ Print "THERMAL IMAGE CALCULATION" UhF-K#Z9 v@sIHb detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 OHN _ SZ7:u895E Print "found detector array at node " & detnode A.F%Ycq ?JbilK}a srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 l03B=$ 85= )lu
Print "found differential detector area at node " & srcnode alJ)^OSIe
y`iBFC;_ GetTrimVolume detnode, trm $V;i
'(&7 detx = trm.xSemiApe MBK^FR-K dety = trm.ySemiApe %X]jaX7 area = 4 * detx * dety (le9q5Qr. Print "detector array semiaperture dimensions are " & detx & " by " & dety BkAm/R Print "sampling is " & nx & " by " & ny {L971W_L :]K4KFM 'reset differential detector area dimensions to be consistent with sampling eSn+ B;
pixelx = 2 * detx / nx g@Z))M+ pixely = 2 * dety / ny _~m5^Q& SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False t|?ez4/{z Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 d7^}tM y8y5*e~A-) 'reset the source power 'ycJMYP8 SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) [|wZ77\ Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" ho{*Cjv YpHg&|Fr 'zero out irradiance array wVXS%4|v For i = 0 To ny - 1 &A/]pi-\ For j = 0 To nx - 1 uh_RGM& irrad(i,j) = 0.0 O^PKn_OJ Next j "V7K SO Next i k8yEdi` OF>mF~ 'main loop hF?1y `20 EnableTextPrinting( False ) 'c&Ed hW')Sp ypos = dety + pixely / 2 mM~qBrwL For i = 0 To ny - 1 iozt&~o xpos = -detx - pixelx / 2 :k]1Lm|| ypos = ypos - pixely A|[?#S((] <{p4V|: EnableTextPrinting( True ) iU918!!N Print i ]EbM9Fo-U EnableTextPrinting( False ) w(Ovr`o?9t ?,Xw[pR o|^3J{3G For j = 0 To nx - 1 + J{IRyBc HWAdhDZ xpos = xpos + pixelx s+Pq&<nV- F;EwQjTF 'shift source ,,.QfUj/& LockOperationUpdates srcnode, True ;+_:,_ GetOperation srcnode, 1, op !TH)
+zi op.val1 = xpos (Rh,, op.val2 = ypos h&iC;yj= SetOperation srcnode, 1, op 6v!`1}
~ LockOperationUpdates srcnode, False 8nqG<!,q c]<5zyl"j1 'raytrace wu6;.xTLl DeleteRays DK~xrU' CreateSource srcnode -IudgO] TraceExisting 'draw MY)O^I X$ octL"t8w 'radiometry
**0~K" ;\ For k = 0 To GetEntityCount()-1 Wi<m{.%\E If IsSurface( k ) Then iMh#TUlQEQ temp = AuxDataGetData( k, "temperature" ) FUzzB94a emiss = AuxDataGetData( k, "emissivity" ) ~/U1xk% If ( temp <> 0 And emiss <> 0 ) Then -ad{tJV| ProjSolidAngleByPi = GetSurfIncidentPower( k ) ;1=1:S8 frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 2.y-48Nz irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi {WS;dX4 End If ^CH=O|8j cZ*@$%_ End If 3`?7<YJ S+6.ZZ9c Next k Q\vpqE!9 :,7hWs Next j Zl!kJ:0 (L:>\m&NO Next i DfD&)tsMQ EnableTextPrinting( True ) !|uWH G4;Oi= 'write out file ;;t yoh~t fullfilepath = CurDir() & "\" & fname 7EEl+;wK Open fullfilepath For Output As #1 I
34>X`[o Print #1, "GRID " & nx & " " & ny gVuFHHeUz Print #1, "1e+308" +=h:Vb8 Print #1, pixelx & " " & pixely t}4,]ms Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 ?j.,Nw4FC cVpp-Z|s8 maxRow = nx - 1 y.k~Y0 maxCol = ny - 1 >'$Mp < For rowNum = 0 To maxRow ' begin loop over rows (constant X) XT*sGM row = "" t?gic9
q For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) .{^5X)
row = row & irrad(colNum,rowNum) & " " ' append column data to row string f~[7t:WD* Next colNum ' end loop over columns gJ{)-\ 6MW{,N Print #1, row ~~P5k: [|L<_.8 Next rowNum ' end loop over rows Y=KT eYW` Close #1 }<r)~{UV q2j{tP# Print "File written: " & fullfilepath X?',n
1 Print "All done!!" ?V=ZIGj End Sub +sA2WK] q`-N7 ,$T 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: U)gH}0n& b%`1cV q;CiV 找到Tools工具,点击Open plot files in 3D chart并找到该文件 B9 uoVcW J@'wf8Ub ITBE|b 打开后,选择二维平面图: 6gE7e|+ zw[m9N5\h
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