| 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。 |>'.( tz^2?wO
成像示意图 x$SxGc~4gb 首先我们建立十字元件命名为Target n%R l$ 8h?):e 创建方法: Yl$R$u) xs}3=&c( 面1 : |_h$}~; 面型:plane LvPcH 材料:Air 7Rq|N$y.3 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 39yp1 Au\j6mB
v1j&oA}$. 辅助数据: lSG"c+iV 首先在第一行输入temperature :300K, S|K#lL emissivity:0.1; \@8.BCWK ahUc;S:v# #Fwf]{J 面2 : H6oU Ne 面型:plane AY(z9&;6 材料:Air $sxm MP 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 2?}5U)Hg 2uEvu x| =]Xxco 位置坐标:绕Z轴旋转90度, b%TLvV 9F `zP{E T_Y
>qL-a*w:a 辅助数据: q}+Fm?B V4CL%i 首先在第一行输入temperature :300K,emissivity: 0.1; MXP3ZN' EpCT !e L60Sc Target 元件距离坐标原点-161mm; |Bhj L, DX b=Ku
L5RBe 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 .l:x! (Do](C V"u .u 探测器参数设定: 7i##g, 3$n O@rOS 在菜单栏中选择Create/Element Primitive /plane c?t,,\o(} *%aWGAu:
K?]c ,&ld:v?~ 2PDU(R 2_C&p6VGj 元件半径为20mm*20,mm,距离坐标原点200mm。 ;56mkP M@a=|N~ 光源创建: OaF[t*]D3 ;8iK] ;^ 光源类型选择为任意平面,光源半角设定为15度。 :(TOtrK@ wqE+hKs, =%ry-n G 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。 \2OjIEQQ ,xOOR 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。 >mCS`D8 LEJn
1 nJr:U2d 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。 %<yH6h*u 4iC=+YUn 创建分析面: H6V!W\:s eZvG NA{?DSP 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。 $/|2d4O:{
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yr[HuwU 到此,所有的光学结构和属性设定完成,通过光线追迹我们可以查看光线是否可以穿过元件。 +<$b6^>!$ nS9 kwaO FRED在探测器上穿过多个像素点迭代来创建热图 ATkx_1]KM- qGhwbg 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。 Br}0dha3E 将如下的代码放置在树形文件夹 Embedded Scripts, $guaUe[x i7|sVz=
0`~#H1TK 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 S*Hv2sl MzpDvnI9 绿色字体为说明文字, ,cwjieM th]pqhl> '#Language "WWB-COM" F&)(G\ 'script for calculating thermal image map 8i Xt8XY3 'edited rnp 4 november 2005 2|:x_rcj 5169E* 'declarations b6ui&Y8z Dim op As T_OPERATION ]`T*}$| Dim trm As T_TRIMVOLUME 0s o27k
Dim irrad(32,32) As Double 'make consistent with sampling @z<IsAE Dim temp As Double p)YI8nW Dim emiss As Double ?7cT$/4 Dim fname As String, fullfilepath As String TBu[3X% P{[@t_ 'Option Explicit ?a{es! |L%d^m Sub Main *^s^{0Ad 'USER INPUTS *jrQ-'<T nx = 31 54>gr1B ny = 31 OiJz?G:m numRays = 1000 K/IG6s;Xj minWave = 7 'microns v i~NfD@s maxWave = 11 'microns 0;n}{26a sigma = 5.67e-14 'watts/mm^2/deg k^4 ]>H'CM4JR fname = "teapotimage.dat" )Nkf'& i=aK ?^+ Print "" ~X<Ie9m1x Print "THERMAL IMAGE CALCULATION" 65>}Q.p o@@,
} detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 [z> Ya-uz7 (^9dp[2 Print "found detector array at node " & detnode 1b`WzoJgH 6o=Q;Mezl srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 R,f"2
k dH_g:ocA Print "found differential detector area at node " & srcnode -YJ4-]Z ?CO..l GetTrimVolume detnode, trm ql2O%B.6? detx = trm.xSemiApe 5rUDRFO6 dety = trm.ySemiApe Ew>lk9La( area = 4 * detx * dety w3Z;&sFd Print "detector array semiaperture dimensions are " & detx & " by " & dety 1`v$R0`! Print "sampling is " & nx & " by " & ny vD3j(d ,l7',@6Y 'reset differential detector area dimensions to be consistent with sampling B0dv_'L}L pixelx = 2 * detx / nx Pt[ b;} pixely = 2 * dety / ny ~%d* #Yxq SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False mz?1J4rt Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 @8"cT- -I*NS6 'reset the source power Y2>0Y3yM SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 'RzzLk|$ Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" W'}^m*F _(0GAz%9 'zero out irradiance array !lk9U^wnd For i = 0 To ny - 1 1YJ@9 *l For j = 0 To nx - 1 q~G@S2=}0} irrad(i,j) = 0.0 z\r29IRh Next j k.Q4oyei Next i Bl*.N9* _ m<@ou7 'main loop <nbc
RO. EnableTextPrinting( False ) `~+[pY1r R~H +.Vh ypos = dety + pixely / 2 {bMOT*X=A For i = 0 To ny - 1 yR4++yk xpos = -detx - pixelx / 2 &LDA=B ypos = ypos - pixely &l
_NCo2 yYn7y1B EnableTextPrinting( True ) z%~rQa./$ Print i A_}6J,*u EnableTextPrinting( False ) E0aJ~A(Hv }e0>Uk`[ x}X
hL For j = 0 To nx - 1 ^Kfm(E DhzmC xpos = xpos + pixelx <g'0q*qE #Pe|}!)u 'shift source QrRnXlEM8 LockOperationUpdates srcnode, True -PLh| GetOperation srcnode, 1, op ve@E.` op.val1 = xpos `&5_~4T7 op.val2 = ypos C[Nh>V7= SetOperation srcnode, 1, op |rwx;+ LockOperationUpdates srcnode, False /\d@A B^5I MVOWJaT(Aq 'raytrace ^Q5advxuq DeleteRays $
nHf0.V1 CreateSource srcnode WI\jm&H r TraceExisting 'draw z\+Ug9Of 7O\ Qxc\ 'radiometry ">x"BP For k = 0 To GetEntityCount()-1 H rI(uZ] If IsSurface( k ) Then @nxpcHj temp = AuxDataGetData( k, "temperature" ) RR[1mM emiss = AuxDataGetData( k, "emissivity" ) ~R
C\ If ( temp <> 0 And emiss <> 0 ) Then `*w!S8} m; ProjSolidAngleByPi = GetSurfIncidentPower( k ) ;kR+jC( frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) cs7K^D;.V irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi 4v;KtD;M End If VX]Ud\( k4`(7Z End If E<r<ObeRv` E5
uk<e_ Next k z\c$$+t JlhI3`X;/ Next j uQO\vRh0 CC|=$(PgT Next i 8&c:73=?X EnableTextPrinting( True ) UIK4]cYC' 0i~?^sT' 'write out file ]oizBa@?G fullfilepath = CurDir() & "\" & fname RKD$'UWX Open fullfilepath For Output As #1 e1Bqd+ Print #1, "GRID " & nx & " " & ny JGQ)/( Print #1, "1e+308" %z"n}|%! Print #1, pixelx & " " & pixely 21 N!?DR Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 @
GXi{9 rHJtNN8$k maxRow = nx - 1 [BuAJ930#5 maxCol = ny - 1 6@-O#,]J For rowNum = 0 To maxRow ' begin loop over rows (constant X) b0uWUI(= row = "" WuMr";2*E For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) xaNM?]% row = row & irrad(colNum,rowNum) & " " ' append column data to row string W
![*0pL Next colNum ' end loop over columns 37 d-! )}i|)^J Print #1, row k`NXYf: b{a\j% Next rowNum ' end loop over rows 5~{s-Ms Close #1 b/obHB+: As>P( Print "File written: " & fullfilepath Lv7$@|"H9 Print "All done!!" h]DzX8r} End Sub gzEcdDD =&#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: |SuN3B4e <Y+>a#T m(CAXq-t 找到Tools工具,点击Open plot files in 3D chart并找到该文件 BjV;/<bt -> `R[k y;=/S?L.: 打开后,选择二维平面图: wG
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