| 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
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成像示意图 (k"oV>a| 首先我们建立十字元件命名为Target KJa?TwnC 5eC5oX> 创建方法: DA
oOs}D fB5Bh;K 面1 : D PnKr/ 面型:plane JF*JFOb 材料:Air `hM:U 孔径:X=1.5, Y=6,Z=0.075,形状选择Box k=[!{I "F+
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8w|j Z@ 辅助数据: I}Z[F,}*J 首先在第一行输入temperature :300K, Z*kGWL emissivity:0.1; l;L&ijTQD #VC^><)3 oKTIoTb 面2 : w\Q3h`.
面型:plane DR9M8E 材料:Air 3V`K^X3 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 9AJ!7J#v" GI$t8{M $*%Ml+H- 位置坐标:绕Z轴旋转90度, t4?g_$> ~}4o=O(
-!MDYj +U 辅助数据: o lNL|WJ`w .jr1<LE 首先在第一行输入temperature :300K,emissivity: 0.1; Ul[>LKFY 76)(G/ .c"UlOZ&w^ Target 元件距离坐标原点-161mm; N|Ua|^ | qHWM
5 v~Y> 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 7&klX N{/q
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Z 探测器参数设定: yQhrPw> m ;ijJ%/ 在菜单栏中选择Create/Element Primitive /plane P1
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`Dh %c%j) dqUhp_f2qK xbo-~{ [ZURs3q 元件半径为20mm*20,mm,距离坐标原点200mm。 dWD,iO_"@ $2>tfKhtA 光源创建: ACl:~7; 2k"a%#H8 光源类型选择为任意平面,光源半角设定为15度。 WGG|d)'@ uh#PZ
xnP Eg-b5Z); 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 #jr;.;8sQ ' QT(TF> 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 qvYYKu :v{$]wg Ffj:xZ9rk 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。 l,*Q?q 7@EYF 创建分析面: $'9r=#EH OM!ES%c, D{'Na5( 到这里元件参数设定完成,现在我们设定元件的光学属性,在前面我们分别对第一和第二面设定的温度和发射系数,散射属性我们设定为黑朗伯,4%的散射。并分别赋予到面一和面二。 dhK$XG !kASEjFz|f
`yYgL@Zt 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。 #yr19i ? {k?Y: FRED在探测器上穿过多个像素点迭代来创建热图 FbFUZ^Zj Rdt8jY6F/ 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。 Q(]-\L' 将如下的代码放置在树形文件夹 Embedded Scripts, ,C&h~uRi#f Q^MB%L;D
D<++6HN 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。 '12|:t&7 Vg
\-^$ 绿色字体为说明文字, 0BaL!^> bk6$+T=> '#Language "WWB-COM" M8cLh!! 'script for calculating thermal image map _hh|/4( 'edited rnp 4 november 2005 n+Ag |.,| |!!E5osXq 'declarations $d8A_CUU Dim op As T_OPERATION RTY$oUqlZ Dim trm As T_TRIMVOLUME cC}s5` Dim irrad(32,32) As Double 'make consistent with sampling uhc0,V;S Dim temp As Double r]HLO'<] Dim emiss As Double ]LSa(7>EU Dim fname As String, fullfilepath As String Cg{$$&_(Hj =JVRm
2#* 'Option Explicit Uw&+zJ Z,4=<;PF Sub Main GU[Cq=k 'USER INPUTS p\-.DRwT` nx = 31 #[KwR\b{:+ ny = 31 v Q_ B2#U: numRays = 1000 .9^;? Ts minWave = 7 'microns $s]@%6f maxWave = 11 'microns 4l$8lYi sigma = 5.67e-14 'watts/mm^2/deg k^4 w
x,; fname = "teapotimage.dat" O4E2)N 23OVy^b Print "" w`7l;7[ Print "THERMAL IMAGE CALCULATION" T=R94 @H_LPn detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 ;XtDz 2(c#m*Q!b Print "found detector array at node " & detnode Z^~6pH\ ^|K*lI/ srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 ffB]4 n9J>yud| Print "found differential detector area at node " & srcnode _:K}DU'6 (w^&NU'e GetTrimVolume detnode, trm
g8x8u| detx = trm.xSemiApe _$cBI_eA7 dety = trm.ySemiApe _x'StD area = 4 * detx * dety 8/F2V?iT Print "detector array semiaperture dimensions are " & detx & " by " & dety 5Y&@
:Y Print "sampling is " & nx & " by " & ny ^7''x,I MnS"M[y3 'reset differential detector area dimensions to be consistent with sampling uB^]5sqfk pixelx = 2 * detx / nx 3AL.UBj&} pixely = 2 * dety / ny .^NV e40O SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False jF5JpyOc Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 .Lp-'!i 'H9~rq7 'reset the source power <qy+@t SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) :_H88/?RR Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" .o8Gi*PEY MmK\|CtV 'zero out irradiance array s6]f#s5o For i = 0 To ny - 1 G`P+J For j = 0 To nx - 1 >mV""?r] irrad(i,j) = 0.0 Iymz2 Next j #Nd+X@j Next i Rq9gtx8,= :ox CF0Y 'main loop pqr"x2=. EnableTextPrinting( False ) #.='dSj i,HAXPi ypos = dety + pixely / 2 2uHp %fv; For i = 0 To ny - 1 pZjFpd| xpos = -detx - pixelx / 2 zN:752d^+r ypos = ypos - pixely X<{m;T ` G~]BC#nB_ EnableTextPrinting( True ) *k}d@j,*" Print i 4jW{IGW EnableTextPrinting( False ) IviWS84 LQjqwsuN{ )/JC.d# For j = 0 To nx - 1 ;1 fM L,8 )'g vaT xpos = xpos + pixelx %'HUC>ChN 3:(`#YY 'shift source qSd
$$L^ LockOperationUpdates srcnode, True ^PI49iB GetOperation srcnode, 1, op ]3C8 op.val1 = xpos GM/1ufZH op.val2 = ypos |3LMVN SetOperation srcnode, 1, op ]*|K8&jxl LockOperationUpdates srcnode, False c>Se Onf 4Rn i7qH 'raytrace k.ZfjX" DeleteRays Xwi&uyvU& CreateSource srcnode #L)rz u TraceExisting 'draw Z7^}G=* L7- nPH 'radiometry ?zEF?LJoK For k = 0 To GetEntityCount()-1 SXEiyy[7v If IsSurface( k ) Then 7E95"B&w temp = AuxDataGetData( k, "temperature" ) NP8TF*5V emiss = AuxDataGetData( k, "emissivity" ) PwW @I~@> If ( temp <> 0 And emiss <> 0 ) Then )R4<*
/C:w ProjSolidAngleByPi = GetSurfIncidentPower( k ) J (h> frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) vF&b|V+, irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi BR2y1Hfi End If K5SO($ pA'A<|)K0 End If g8Z14'Ke (=j!P* Next k w%;'uN_ >gl.(b25C Next j (4LLTf0 Pcs@`&}7r Next i eXK`%' EnableTextPrinting( True ) ?=kswf %j@FZ
)a[ 'write out file 7&4,',0VL fullfilepath = CurDir() & "\" & fname 3U)8P6Fz Open fullfilepath For Output As #1 (Y([^N q Print #1, "GRID " & nx & " " & ny I8?[@kg5b' Print #1, "1e+308" O 0#Jl8 Print #1, pixelx & " " & pixely pC-OZ0 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 zwtsw [. {%{GZ maxRow = nx - 1 3;NRW+ maxCol = ny - 1 Q8?D}h For rowNum = 0 To maxRow ' begin loop over rows (constant X) W#j,{&KVn row = "" +`8)U 3u0 For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) "zbE row = row & irrad(colNum,rowNum) & " " ' append column data to row string l #Q`f. Next colNum ' end loop over columns P~e$iBH' 9#ft;c Print #1, row s~
A8/YoU} |@.<}/ Next rowNum ' end loop over rows dn_OfK Close #1 :N*T2mP I&8m5F?$` Print "File written: " & fullfilepath
c^s> Print "All done!!" yipD5,TC End Sub @88i/ Z_ Y)}%SP>, 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: f)Q]{ cb6 CDnz
&? -P>=WZu 找到Tools工具,点击Open plot files in 3D chart并找到该文件 T+R I8.#o % VpBB ~qxXou,J 打开后,选择二维平面图: !"%sp6Wc v&2@<I>
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