| 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。 c=t*I0-OVS s}b*5@8|tA
成像示意图 `p"U 首先我们建立十字元件命名为Target )b9I@)C Hz4uZ*7\| 创建方法: "=`~iXT{e ^X;JT=r 面1 : M-91
JOt~ 面型:plane EC dfLn *c 材料:Air u@"o[e': 孔径:X=1.5, Y=6,Z=0.075,形状选择Box U5wTGv4S| 0O['w<_
pFH?/D/q 辅助数据: V9$-twhu 首先在第一行输入temperature :300K, )9pBu
B emissivity:0.1; 5fxbA2\ .%hQJ{vf-^ )O-sWh4 面2 : & ^!v*=z 面型:plane KH)pJG|NY 材料:Air zuj;T,R; 孔径:X=1.5, Y=6,Z=0.075,形状选择Box }moz9a W,'3D~g8 @{de$ODu 位置坐标:绕Z轴旋转90度, e>(Wvb&4 pqd4iR Wv
iDvpXn 辅助数据: ^AH-+#5 )ldUayJ 首先在第一行输入temperature :300K,emissivity: 0.1; {G]`1Q1DR H.;yLL= R mgxf/ Target 元件距离坐标原点-161mm; H!^C 2 ;op'V6iG
-&~IOqlui 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 GfQ^@Tl K;kLQ2) $/y%[ . 探测器参数设定: *@=fq|6l 2 D)RdOldr 在菜单栏中选择Create/Element Primitive /plane r8H7TJI0
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Ti} (h%|;9tF 元件半径为20mm*20,mm,距离坐标原点200mm。 2@OBeR E{?L= ^cU 光源创建: S@;&U1@h .w=:+msL{( 光源类型选择为任意平面,光源半角设定为15度。 tgS+"ugl |'!7F9GP fa/P%9db 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 W=(MsuirO CrT2#h 1# 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 ``/y=k/au `mWQWx$V! k^~@9F5k 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。 wZ}n3R, X~`.} 创建分析面: 1'gKZB)TG7 T;xHIg4 jw2_!D 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。 2"B}} 7v.#o4nPK
P<TpG0~( 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。 1NB2y[ )+VHt
FRED在探测器上穿过多个像素点迭代来创建热图 U`HXsq
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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。 wCTcGsw W 将如下的代码放置在树形文件夹 Embedded Scripts, JsHxQ0Tw d8VWi*
JuKk"tr~RB 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。 :9v*,*@x I 0x`H)DA 绿色字体为说明文字, ski1f |8&\N '#Language "WWB-COM" 1D3dYVE 'script for calculating thermal image map }D&"z8mP 'edited rnp 4 november 2005 YqK+F=0 ,'/HcF?yf 'declarations v3=&{}+j. Dim op As T_OPERATION Fv5x6a Dim trm As T_TRIMVOLUME EIy]qAE:f Dim irrad(32,32) As Double 'make consistent with sampling -k|g04Q? Dim temp As Double tIc0S!H# Dim emiss As Double 7TMDZ* Dim fname As String, fullfilepath As String {66Q" H"I 6:SK{RSURC 'Option Explicit Q>06dO~z8 >llwNT Sub Main S|O%h}AH; 'USER INPUTS J7 Oa})-+' nx = 31 Lqz}&A
ny = 31 c,{& numRays = 1000 fwar8
i1 minWave = 7 'microns \(3Qqbw maxWave = 11 'microns =DQd PA\K sigma = 5.67e-14 'watts/mm^2/deg k^4 QI
:/,w fname = "teapotimage.dat" YFC0KU 8k* Print "" TYmUPS$ Print "THERMAL IMAGE CALCULATION" Dn{19V.L f6dE\ detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 Q
T0IW(A tXb7~aO Print "found detector array at node " & detnode OoU '86) !z"a_ srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 ^bY^x+d ->RF`SQu Print "found differential detector area at node " & srcnode |P[D2R} /o}0oo5B GetTrimVolume detnode, trm /4f 5s#hR detx = trm.xSemiApe fjz2m dety = trm.ySemiApe zd*W5~xKg area = 4 * detx * dety qQ?,|4)y Print "detector array semiaperture dimensions are " & detx & " by " & dety H*:r>Lm= Print "sampling is " & nx & " by " & ny >uqS k8t Na@H 'reset differential detector area dimensions to be consistent with sampling B[U.CAUn pixelx = 2 * detx / nx cr=FMfhB pixely = 2 * dety / ny $
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< SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False n79DS(t Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 =^%Pwkz 1_dMe%53 'reset the source power $' I$n SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) d9Ow 2KrC Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" A=YEY n D/%b@Ls2ze 'zero out irradiance array }IalgQ(i For i = 0 To ny - 1 <EM LiiNY For j = 0 To nx - 1 =+sIX3 irrad(i,j) = 0.0
^F{)4 Next j 59%f|.Z) Next i xa%ktn v2uS6 'main loop -T>wi J EnableTextPrinting( False ) {1-CfQ0
8 .of:#~ ypos = dety + pixely / 2 5M.n'* For i = 0 To ny - 1 I!i#= xpos = -detx - pixelx / 2 JEkIbf?=r ypos = ypos - pixely J9KLO= l4B O@ EnableTextPrinting( True ) piM11W}|/ Print i pmpn^ZR EnableTextPrinting( False ) vM>`CZ pl^"1Z=* gm%bxr@X~ For j = 0 To nx - 1 k`J..f9 }rAN2D]"} xpos = xpos + pixelx B,na VA&OI;=ri 'shift source FOnA;5Aa LockOperationUpdates srcnode, True &.bR1wX GetOperation srcnode, 1, op C9;X6 op.val1 = xpos -L'`d op.val2 = ypos ) GT?Wd SetOperation srcnode, 1, op r1H['{$ LockOperationUpdates srcnode, False ;g)Fhdy! ug3lMN4UX raytrace ah$7
Oudj DeleteRays vgbjvyfN CreateSource srcnode x%?*]*W TraceExisting 'draw GbrPtu2{@V Ch&]<#E>` 'radiometry 3ijI2Zy For k = 0 To GetEntityCount()-1 b)`#^uxxJ If IsSurface( k ) Then ALieUf temp = AuxDataGetData( k, "temperature" ) gm\o>YclS emiss = AuxDataGetData( k, "emissivity" ) O0*L9C/Q If ( temp <> 0 And emiss <> 0 ) Then L-:L=
snO ProjSolidAngleByPi = GetSurfIncidentPower( k ) o0+BQ&A)s* frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) <XcMc<h~ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi W[Ew6)1T End If ^9f`3~!#bc )tQ6rd' End If 7Mg7B )KhVUFS1 Next k j I@$h_n NHVx!Kc Next j z ex.0OT; zZ0V6T} Next i Zgf||, EnableTextPrinting( True ) K[yJu 4 F,2#;t4 'write out file ?-& D' fullfilepath = CurDir() & "\" & fname tnbs]6 Open fullfilepath For Output As #1 |a:VpM Print #1, "GRID " & nx & " " & ny ^* v{t?u Print #1, "1e+308" '#
2J?f' Print #1, pixelx & " " & pixely v 5ddb) Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 2*DS_=6o =WRU<`\ maxRow = nx - 1 u,9U0ua@; maxCol = ny - 1 /;m!>{({) For rowNum = 0 To maxRow ' begin loop over rows (constant X) rd~W.b_b row = "" kAQ Zj3P] For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) [|O6n"' row = row & irrad(colNum,rowNum) & " " ' append column data to row string 1gK3=Ys Next colNum ' end loop over columns q x }fn/: bjX$idL Print #1, row n|2-bRK- 5!{g6=( Next rowNum ' end loop over rows aT1W]i Close #1 `mTxtuid{ eL4@%
]o Print "File written: " & fullfilepath g' U^fN Print "All done!!" !+ hgKZ] End Sub W G r\R ,qqV11P] 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: !h(0b*FUJ J%B?YO, Zpd>' ${4 找到Tools工具,点击Open plot files in 3D chart并找到该文件 y+x>{!pw >{=RQgGy rmoEc]kt] 打开后,选择二维平面图: )yAPYC <4bo7XH
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