| infotek |
2023-04-06 08:38 |
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。 qra5&Fvb tx01*2]pX
成像示意图 ~pj/_@S@x 首先我们建立十字元件命名为Target f3Cjj]RFv /?Fa<{ 创建方法: {Tym# =a3qpPkx 面1 : Xv1mjHZCC 面型:plane (>gAnebN
L 材料:Air 84$#!=v 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ,c\3b)ax ^qD@qJ
6Jf\}^4@k 辅助数据: X6lR?6u%| 首先在第一行输入temperature :300K, FtL{f=
emissivity:0.1; %T:7I[f ^@0-E@ {c
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AU 面2 : *K1GX 面型:plane yhi6RDS 材料:Air drZ1D s 孔径:X=1.5, Y=6,Z=0.075,形状选择Box PgY q=|]` 8!uqR!M<C (1my9k5C 位置坐标:绕Z轴旋转90度, nQW`X=Ku j*aYh^
!\%0O`b^4 辅助数据: CH/*MA &\0V*5tI 首先在第一行输入temperature :300K,emissivity: 0.1; C3
m#v[+ v<qiu>sbz} 5%E.UjC Target 元件距离坐标原点-161mm; #r4S% M~1 n#
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ZC80 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 :6Q`! in 5wws8w O]Mz1 ev| 探测器参数设定: 5c~OG6COx 8v)PDO~D}A 在菜单栏中选择Create/Element Primitive /plane cNd2XQB9= oqOXRUy
8I'Am"bc\ 75pz' Cb S2jO .RNr^*AQ 元件半径为20mm*20,mm,距离坐标原点200mm。 +I+7@Xi Z {,|J?>{ 光源创建: +AT!IZrB2i 8'(|1 光源类型选择为任意平面,光源半角设定为15度。 '5mzlR LK^t](F 2_4m}T3 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。 ]eJjffx jR^>xp; 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。 UJ'}p&E `euk&]/^.) $^2 j#]uX 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。 MpV6Vbp F+`DfI]/m 创建分析面: 0-^wY8n-= ?'_Q^O> @42!\1YT 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。 QcQ:hHF 7b2N'^z}
J@{yWgLg 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。 "KY9MBzPD GA{Q6]B FRED在探测器上穿过多个像素点迭代来创建热图 A|BvRZd 6'M"-9?G 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。 U~SOHfZ%( 将如下的代码放置在树形文件夹 Embedded Scripts, nJTV@mXVq $?OuY*ZeY9
HHbkR2H1 打开后清空里面的内容,此脚本为通用脚本适用于一切可热成像的应用。 VxOrrs7Z VK+#!!Ha 绿色字体为说明文字, <mc[-To MR90 }wXE '#Language "WWB-COM" 1u\fLAXn 'script for calculating thermal image map a$c7d~p$I 'edited rnp 4 november 2005 i6[,m*q~2x :B=p%C 'declarations T
x_n$ & Dim op As T_OPERATION Fc;)p88[ Dim trm As T_TRIMVOLUME t/,k{5lX Dim irrad(32,32) As Double 'make consistent with sampling )T6+} Dim temp As Double 'iN8JO> Dim emiss As Double wovWEtVBU Dim fname As String, fullfilepath As String 0;Y_@UVj OC'cP[$ _ 'Option Explicit 9-+6Ed^2 46'EZ@#s Sub Main }6P]32d 'USER INPUTS a$I;
L nx = 31 %S22[;v{N ny = 31 ?K7m:Dx numRays = 1000 c@{,&,vsj minWave = 7 'microns 35yhe:$nf maxWave = 11 'microns XcA4EBRj
sigma = 5.67e-14 'watts/mm^2/deg k^4 ^/HE_keY fname = "teapotimage.dat" O'deQq[ voaRh@DZ%/ Print "" S<Q6b_D Print "THERMAL IMAGE CALCULATION" l\5}\9yS d]h[]Su/? detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 FXFQ@q*}v \z8TYx@ Print "found detector array at node " & detnode p/WEQ2 &adKKYN srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 ~K^Z4 tkWWR%c" Print "found differential detector area at node " & srcnode 9VIsLk54^ +D1;_DU GetTrimVolume detnode, trm VLtb16| detx = trm.xSemiApe Tk/K7h^ dety = trm.ySemiApe A20_a;V area = 4 * detx * dety C,-V>bx g Print "detector array semiaperture dimensions are " & detx & " by " & dety lp?geav Print "sampling is " & nx & " by " & ny NF0} eom *D]/V U 'reset differential detector area dimensions to be consistent with sampling =#1iio&
pixelx = 2 * detx / nx G
<m{ o pixely = 2 * dety / ny Y&k'4Y% SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False }(J6zo9(x Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2
~J"*ahl yq[C?N &N 'reset the source power : 4Sj2
SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) -BACdX Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" >'Nrvy%&0 a&ZH 'zero out irradiance array ,[+gE\z{{u For i = 0 To ny - 1 ~&k1P:#R For j = 0 To nx - 1 Old5E& irrad(i,j) = 0.0 L<QqQ"` Next j " I`<s < Next i W32mAz; ^`=Z=C$fj 'main loop o?^j1\^ EnableTextPrinting( False ) " S#0QH%5 ~mK9S^[ ypos = dety + pixely / 2 i/oaKpPN For i = 0 To ny - 1 LUKdu&M xpos = -detx - pixelx / 2 |)pT"` ypos = ypos - pixely w{K_+}fAC }RG EnableTextPrinting( True ) v"_hWJ) Print i Y.F:1<FAtf EnableTextPrinting( False ) #)=P/N1 7Y@&& v.\1-Q? For j = 0 To nx - 1 T
-C2V$1 wvJm)Mj+ xpos = xpos + pixelx %S.R@C[3 z{``v|K 'shift source A#2Fd7& LockOperationUpdates srcnode, True B4[onYU GetOperation srcnode, 1, op A(Ugam~} op.val1 = xpos 8K6yqc H op.val2 = ypos 0l^-[jK) SetOperation srcnode, 1, op &cayhL/% LockOperationUpdates srcnode, False WZ@nuK.39T }#'O b 'raytrace e}kEh+4 DeleteRays IR(JBB|xNQ CreateSource srcnode `IkWS7| TraceExisting 'draw 5cgDHs (tx6U.Oy 'radiometry N!/^s": For k = 0 To GetEntityCount()-1 rMfp%DMA If IsSurface( k ) Then 7DKbuUK temp = AuxDataGetData( k, "temperature" ) Skp&W*Ai emiss = AuxDataGetData( k, "emissivity" ) yYp!s If ( temp <> 0 And emiss <> 0 ) Then z~L(kf4 ProjSolidAngleByPi = GetSurfIncidentPower( k ) @aY 8VL7C0 frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) O|?>rK irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi gI'4g ZH End If =+'4u t_x\&+W End If ,>`wz^z `kVy1WiY Next k _CciU.1k&, _rY,=h{+ Next j M7fw/i M{3He)& Next i "S_t%m&R EnableTextPrinting( True ) ;6U=fBp7< +/-#yfn!TR 'write out file ,N?~je. fullfilepath = CurDir() & "\" & fname NK~j>>^;v Open fullfilepath For Output As #1 D7olu29 Print #1, "GRID " & nx & " " & ny iaLsIy#h Print #1, "1e+308" y5RcJM Print #1, pixelx & " " & pixely b Zn:q[7 Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 1ePZs$ b{b2L. maxRow = nx - 1 M`9qo8zCi maxCol = ny - 1 k/u6Cw0/ For rowNum = 0 To maxRow ' begin loop over rows (constant X) KArR.o } row = "" gieTkZ For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) [C,<Q row = row & irrad(colNum,rowNum) & " " ' append column data to row string C~yfuPr\B Next colNum ' end loop over columns XWf8ZZj YRfs8I^rg Print #1, row Gvb>M=9 ic%<39 Next rowNum ' end loop over rows *[wy-
fu Close #1 \=kH7 ! w9SPkPkYE Print "File written: " & fullfilepath .a8N 5{` Print "All done!!" <_dyUiT$J End Sub 4askQV &hj \A6MVMF8 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: 5IOOV Yl SsIy ;l J{
P<^<m_ 找到Tools工具,点击Open plot files in 3D chart并找到该文件 >8"oO[U5> w-C~
Ik j\B]>PP5 打开后,选择二维平面图: mSp- Kyt.[" p
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