| 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。 SEH[6W3 bo@,
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成像示意图 4`")aM 首先我们建立十字元件命名为Target <*oV-A 2)-4?uz~ 创建方法: NnaO!QW% wNmC1HOh 面1 : d;{k,rP6 面型:plane Bi>]s%zp 材料:Air [ B*r{ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box n98sY+$-z M;YJpi
F& 辅助数据: !-ZY_ 首先在第一行输入temperature :300K, 0;hn;(V]" emissivity:0.1; FOjX,@x& lR]FQnZ > }kZXeR| 面2 : 6Xbf3So 面型:plane ,T;D33XV 材料:Air dXsD%sG@ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box L$y~\1- RF~G{wz 2IGU{&s 位置坐标:绕Z轴旋转90度, YGRb|P- 08! _B\
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辅助数据: k$pND,Ws N7YCg 首先在第一行输入temperature :300K,emissivity: 0.1; '%o^#gJ p ln8es{q .K`n;lVs Target 元件距离坐标原点-161mm; / vu]ch n~tb z"&
ukRmjHbLf 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 "yj_v\@4 Y/T-q<ag8 )<qL8#["U 探测器参数设定: ^Y5I OX: Ex
skd} 在菜单栏中选择Create/Element Primitive /plane ?Mn~XN4F_ 9}Ge@a<j
u7j,Vc'~ F/3L^k] W=OryEV? NytodVZ'3 元件半径为20mm*20,mm,距离坐标原点200mm。 \,r*-jr sf:IA%.4t 光源创建: *xY3F8 Ge7B%p8 光源类型选择为任意平面,光源半角设定为15度。 Hi*|f!,H? eKZS_Q d n$9Xj@+ 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 lcgG5/82 eZ-fy,E 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 ?<Lm58p8 o[i*i<jv- 4jZB%tH 功率数值设定为:P=sin2(theta) theta为光源半角15度。我们为什么要这么设定,在第二部分会给出详细的公式推导。 N
Z,} v3 yK$aVK" 创建分析面: 4=;j.=>0X P"]l/ dnQ6Ras 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。 xq=!1> )VqPaKZl
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$' 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 ;jN1n
xF ~*<`PD O? FRED在探测器上穿过多个像素点迭代来创建热图 99CK [G FK`:eP{ FRED具有一个内置的可编译的Basic脚本语言。从Visual Basic脚本语言里,几乎所有用户图形界面(GUI)命令是可用这里的。FRED同样具有自动的客户端和服务器能力,它可以被调用和并调用其他可启动程序,如Excel。因此可以在探测器像素点上定义多个离轴光源,及在FRED Basic脚本语言里的For Next loops语句沿着探测器像素点向上和向下扫描来反向追迹光线,这样可以使用三维图表查看器(Tools/Open plot files in 3D chart)调用和查看数据。 +{C)^!zBK 将如下的代码放置在树形文件夹 Embedded Scripts, rK`^A dQ9W40g1
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Kv/ 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 LZ.Xcy u3E =r 绿色字体为说明文字, `%"x'B`mM ,v#n\LD` '#Language "WWB-COM" Ei\>gXTH1- 'script for calculating thermal image map g j]8/~lr 'edited rnp 4 november 2005 AO|1m$xf UUb0[oy 'declarations m^3j|'mG Dim op As T_OPERATION X.[bgvm~C Dim trm As T_TRIMVOLUME _\Z'Yl Dim irrad(32,32) As Double 'make consistent with sampling dU2; Dim temp As Double *+2_!=4V Dim emiss As Double Oh>hyY)} Dim fname As String, fullfilepath As String u86PTp+ aDxNAfP
'Option Explicit pV;0Hcy >goHQ30: Sub Main 8oXp8CC 'USER INPUTS \Q1&w2mw nx = 31 D
.LR-Z ny = 31 1s(]@gt numRays = 1000 "PO8 Q minWave = 7 'microns D6+3f#k6 maxWave = 11 'microns yNn=r;FZQ sigma = 5.67e-14 'watts/mm^2/deg k^4 !E_|Zp]up fname = "teapotimage.dat" R5(([C1 ,Z _@]D@ Print "" \%.oi@A Print "THERMAL IMAGE CALCULATION" 75R#gQ]EV Il(o[Q>jJ3 detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 3 H5 &=$f\O1Ty Print "found detector array at node " & detnode W[
W)q%[) " zD9R4\X. srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 O!XSU, N5ZOpRH{ Print "found differential detector area at node " & srcnode _>kc: 5|N`:h'9M GetTrimVolume detnode, trm ITTEUw~+o detx = trm.xSemiApe )oz2V9X{ dety = trm.ySemiApe $C fp1# area = 4 * detx * dety Kg"eS`- Print "detector array semiaperture dimensions are " & detx & " by " & dety un -h%-e| Print "sampling is " & nx & " by " & ny ID!S}D #\n*Qg4p 'reset differential detector area dimensions to be consistent with sampling D1 v0`od' pixelx = 2 * detx / nx J5HK1 pixely = 2 * dety / ny L?N-uocT SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False yt="kZ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 vt* K%mR=u#%& 'reset the source power JoiGuZd> SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) BG?>)]6 Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" nXoDI1<[ Zl3e=sg= 'zero out irradiance array CM++:Y vJ For i = 0 To ny - 1 X9]} UX For j = 0 To nx - 1 Q1x&Zm1v irrad(i,j) = 0.0 9X;*GC;d Next j 1E&S{. Next i PuGs%{$(h ?Z?(ky! 'main loop Og1vD5a EnableTextPrinting( False ) NFx%e hCr,6nc C ypos = dety + pixely / 2 =RRv&
"2r For i = 0 To ny - 1 2zh-ms xpos = -detx - pixelx / 2 ,zHL8SiTX ypos = ypos - pixely R2-F@_ y2s(]#8 EnableTextPrinting( True ) jaKW[@< Print i Xo~q}(ze^ EnableTextPrinting( False ) 6Q]c} }8aqSD<: zb!1o0, J For j = 0 To nx - 1 _0'X!1" };9s8VZE xpos = xpos + pixelx ln=fq: `NgQ>KV! 'shift source :}Yk0* LockOperationUpdates srcnode, True 5>0\= GetOperation srcnode, 1, op z+6PVQ op.val1 = xpos Y)5O %@Rl op.val2 = ypos NiW9/(;xB SetOperation srcnode, 1, op o ^UOkxs. LockOperationUpdates srcnode, False Qr3!6 #!UJY%c~ raytrace ``VE<:2+ DeleteRays 6?<lS.s CreateSource srcnode ov,s]g83 TraceExisting 'draw 5!qf{4j K&NH? 'radiometry 0LL0\ly] For k = 0 To GetEntityCount()-1 63Gq5dF If IsSurface( k ) Then u_9c> temp = AuxDataGetData( k, "temperature" ) uZrp ^ emiss = AuxDataGetData( k, "emissivity" ) %~Rg`+ If ( temp <> 0 And emiss <> 0 ) Then Y8v[kuo7 ProjSolidAngleByPi = GetSurfIncidentPower( k ) _!DH/?aU frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) FVrB#Hw~ irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi f*Q9u >1p End If ^$lZ 7R:Ij[dV End If M3@qhEf?vk ]7W!f 2@ Next k {Oy|c sZ&|omN Next j $G"\@YC< o(Z~J}l({ Next i 7UW\|r EnableTextPrinting( True ) L f"!:] 1aRTvaGo 'write out file Q`AlK"G, fullfilepath = CurDir() & "\" & fname ;2`6eyr Open fullfilepath For Output As #1 bs~P Print #1, "GRID " & nx & " " & ny :AztHf?X Print #1, "1e+308" |LQ%sV Print #1, pixelx & " " & pixely {*GBUv5 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 eQ/w
Mr CA`V)XIsP maxRow = nx - 1 t}h(j| maxCol = ny - 1 JnK<:]LcK For rowNum = 0 To maxRow ' begin loop over rows (constant X) O5p$
A@ row = "" ~210O5^ For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) @hg[v`~ row = row & irrad(colNum,rowNum) & " " ' append column data to row string z[_Y,I Next colNum ' end loop over columns MjC<N[WO>N k
$^/$N Print #1, row Z!|r> t>}S@T{~T Next rowNum ' end loop over rows N)Q_z9b= Close #1 jH<Sf: Y( ,%IP27bPW Print "File written: " & fullfilepath `Ze$Bd\ Print "All done!!" h?n?3x!( End Sub E<3xv;v8r v%*don 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:
O[MFp Fn`Zw:vp6 e7xv~C>g 找到Tools工具,点击Open plot files in 3D chart并找到该文件 BI)C\D3[ /fT"WaTEK SQK82/ 打开后,选择二维平面图: #*CMf.OCh iU 6,B
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