| infotek |
2022-01-24 09:30 |
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。
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成像示意图 }7+`[g 首先我们建立十字元件命名为Target m2j]wUh" 6-t:eo9 创建方法: *a2-Vte y8Oz4| 面1 : ai$s 面型:plane i$jzn
ga 材料:Air 9 .3?$( 孔径:X=1.5, Y=6,Z=0.075,形状选择Box Lyy:G9OV 9lR-
T/nG\WZbZn 辅助数据: 3T)_(SM" 首先在第一行输入temperature :300K, mFx\[S emissivity:0.1; H9Dw#.em ,1e\}^ T%TfkQ__d 面2 : -Crm#Ib~ 面型:plane ~(P\'H&(h 材料:Air pp1kcrE\M 孔径:X=1.5, Y=6,Z=0.075,形状选择Box GbfA-\ ]wHXrB8vx m_C#fR /I 位置坐标:绕Z轴旋转90度, Prqr, )>r sX)
)tp;2rJ/ 辅助数据: mXJ`t5v^l 6|B;C 首先在第一行输入temperature :300K,emissivity: 0.1; /kc@ELl
_BPp=(| #``Alh8 Target 元件距离坐标原点-161mm; V[^+lR K0^Tg+U($p
5XF&yYWq 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 ?O.'_YS [ n2)6B\/ ^2-+MWW. 探测器参数设定: byN4?3F 6SP!J*F 在菜单栏中选择Create/Element Primitive /plane C%q]o >goG\y
@ev8"JZ1 B]wfDUG L',7@W a(IZ2Zmr 元件半径为20mm*20,mm,距离坐标原点200mm。 VX,@Gp_' m :BVYS|% 光源创建: 4cZlQ3OE. aSH =|Jnc 光源类型选择为任意平面,光源半角设定为15度。 (5efNugc -}KW"#9c ]>oI3&6s 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 U!i @XA%P !HSX:qAP$ 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。 t6! B qLk7C0 wt1Y&D 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。 5@yBUwMSj
)vy_m_f& 创建分析面: KD73Aw \$Aw[
5&t 9YVr9BM'K 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。 @X]JMicJ {9|S,<9
vg-'MG 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。 2O
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_|"+Ze FRED在探测器上穿过多个像素点迭代来创建热图 )(W%Hmi 1pZ[rM'} 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。 R0bWI`$Z 将如下的代码放置在树形文件夹 Embedded Scripts, f (ug3(j Pw/$
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g]m}@b6(h 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。 Py~N.@(:1u Vh8RVFi;c 绿色字体为说明文字, 9B2`FJ ldNWdz '#Language "WWB-COM" G ; 'script for calculating thermal image map ;-d2~1$ 'edited rnp 4 november 2005 ydf;g5OZ AN4(]_] 'declarations #r;uM+ Dim op As T_OPERATION KK41I8Mw Dim trm As T_TRIMVOLUME cPg$*,] Dim irrad(32,32) As Double 'make consistent with sampling M<cm] Dim temp As Double QR*{}`+l Dim emiss As Double _0!<iN L Dim fname As String, fullfilepath As String -< }#ImTN 4<y|SI! 'Option Explicit 6d%)MEM QI{<q< Sub Main oxJ#NGD 'USER INPUTS :AM_C^j~
D nx = 31 Fu"@)xw/-q ny = 31 h f9yK6 numRays = 1000 (qg~l@rf minWave = 7 'microns nCPIpw,]M maxWave = 11 'microns Vho^a:Z9}W sigma = 5.67e-14 'watts/mm^2/deg k^4 -r@/8" fname = "teapotimage.dat" ^ Mw=!n[ .tt= \R Print "" , \R,O Print "THERMAL IMAGE CALCULATION" CQ^I;[=d ~PiCA detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 '^~38=FA &E$:^a4d Print "found detector array at node " & detnode .8/W_iC92 <PTi>C8;r srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 H <ugc VDC"tSQ Print "found differential detector area at node " & srcnode m`H9^w%W b@yFqgJ_ GetTrimVolume detnode, trm ">rt *?^ detx = trm.xSemiApe rKr2 K' dety = trm.ySemiApe >TddKR@C area = 4 * detx * dety hv8j$2m Print "detector array semiaperture dimensions are " & detx & " by " & dety [nG[@)G~0M Print "sampling is " & nx & " by " & ny 62{[)jt{ MD=VR(P?eq 'reset differential detector area dimensions to be consistent with sampling dxF/]>t pixelx = 2 * detx / nx atWB*kqI pixely = 2 * dety / ny ;+4X<)y*> SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False wVY;)1? Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 ts~$'^K[- 9S$?2z".2 'reset the source power )0xEI SetSourcePower( srcnode, Sin(DegToRad(15))^2 )
=[G) Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" uq_h8JH$ R22P
ol 'zero out irradiance array 1PdxoRa4= For i = 0 To ny - 1 nO7#m~ For j = 0 To nx - 1 XqK\'8]\Mw irrad(i,j) = 0.0 TLiA>`r= Next j `-[+(+[" Next i ]z_C7Y"4BR >m&r,z 'main loop +jpC%o}C EnableTextPrinting( False ) C*fSPdg? qvhol ypos = dety + pixely / 2 6
&)fZt For i = 0 To ny - 1 PM!7ci xpos = -detx - pixelx / 2 'hw_ew ypos = ypos - pixely uSi/| /]*#+;;% EnableTextPrinting( True ) 1F_ 1bAh$ Print i Z`lCS
o; EnableTextPrinting( False ) ewb/Z[4 hSyA;*)U VIjsz42C For j = 0 To nx - 1 o4g<[X) 8{Id+Q>Vo, xpos = xpos + pixelx xr\wOQ*` W!G2$e6 'shift source
C6`<SW LockOperationUpdates srcnode, True WxFrqUz GetOperation srcnode, 1, op @43o4, op.val1 = xpos T c{]w?V op.val2 = ypos KU}HVM{ SetOperation srcnode, 1, op ]Ak@!&hyak LockOperationUpdates srcnode, False wh<s#q` v|v^(P,o raytrace C^x+'. ^N DeleteRays 6hs2B5)+ CreateSource srcnode +=bGrn>h TraceExisting 'draw \Ow-o0 Nl^{w'X0h 'radiometry (gl/NH! For k = 0 To GetEntityCount()-1 VIxt;yE If IsSurface( k ) Then $N#f)8v temp = AuxDataGetData( k, "temperature" ) hp E? emiss = AuxDataGetData( k, "emissivity" ) buhn~ c If ( temp <> 0 And emiss <> 0 ) Then >cPB:kD' ProjSolidAngleByPi = GetSurfIncidentPower( k ) )A4WK+yD$z frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) 6*,8 H& irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi M7(vI4V End If %q@eCN 43;@m}|7$ End If Pb|'f( !m#cneV Next k AE)<ee%\\ U$`)|/8 Next j y^ gazr" !(hP{k ^g Next i !t["pr\
? EnableTextPrinting( True ) OT9\K_ ^#R-_I 'write out file =Po!\[SBU fullfilepath = CurDir() & "\" & fname
]8q5k5~ Open fullfilepath For Output As #1 cf|<~7 Print #1, "GRID " & nx & " " & ny kQ$Q}3f Print #1, "1e+308" FV/X&u8~ Print #1, pixelx & " " & pixely pQxaT$ Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 byv(:xk|'e &DFe+y~PR maxRow = nx - 1 ?'K}bmdt}. maxCol = ny - 1 6$>m s6g% For rowNum = 0 To maxRow ' begin loop over rows (constant X) <4y1[/S row = "" Jr18faEZw For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) $.}fL;BzVz row = row & irrad(colNum,rowNum) & " " ' append column data to row string <v"C`cga Next colNum ' end loop over columns '?5=j1 X9nt;A2TU+ Print #1, row A>$VkGo QJo) Next rowNum ' end loop over rows n]x4twZ Close #1 Mz<4P3"H {W}.z Print "File written: " & fullfilepath YF@'t~_Z Print "All done!!" 0K,*FdA End Sub WZRrqrjq O@3EJkv 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: Q/iaxY# TeQWrms FpfOxF6A3 找到Tools工具,点击Open plot files in 3D chart并找到该文件 ?N#mD SPL72+S`, _"J-P={= 打开后,选择二维平面图: 'oHtg
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