| 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。 Wu,=jL3?$A C^?/9\
成像示意图 :EPe,v RT 首先我们建立十字元件命名为Target Z%sTj6Th XcbEh 创建方法: s&%r? >d;U>P5. 面1 : >xRUw5jN 面型:plane 9AWP`~l` 材料:Air ,*[N_[ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 4tkb7D
q }w=|"a|,
U8aNL
sw 辅助数据: iQ;lvOja 首先在第一行输入temperature :300K, s4Jy96< emissivity:0.1; H H3Z?g rZAP3)dA -f'&JwE0= 面2 : z3^gufOkQ 面型:plane sCf)#6mI 材料:Air RP^L.X(7^ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ?J| ^c}kVQ\g3 PE_JO(e;Xm 位置坐标:绕Z轴旋转90度, xxgdp. ( ocS}4.a@
\^cXmyQ <% 辅助数据: Vo%ikR # .5~3D97X& 首先在第一行输入temperature :300K,emissivity: 0.1; v/7^v}[< C
szZr>Z V2yX;u Target 元件距离坐标原点-161mm; OSJL,F, u3cl7~- yW
F${}n1D 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 ubKp
P%Z ;Rxc(tR!n z+c8G 探测器参数设定: iII%!f?{[ Ln4Dq[M 在菜单栏中选择Create/Element Primitive /plane fG@]G9Z ND3|wQ`M0
=Q# (2 ;e2D} @E> rqI;` ^C2SLLgeJ 元件半径为20mm*20,mm,距离坐标原点200mm。 y?iW^>|?L= Q}^qu6 光源创建: +}g6X6m {(d 6of`C_ 光源类型选择为任意平面,光源半角设定为15度。 ziQ&M\ *y~~~ 'J/ >+%0|6VSb 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。 8y4t9V "`KT7 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。 2%-/}'G* ]~pM;6Pu0 ?%T]V+40 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。 Gg^gK*D .;dI&0Z 创建分析面: TQpR'
S O`b+B MdnapxuS 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。 E,/nK +WCV"m
<.
V*]g/; 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。 =s:Z-*vy! `{ \)Wuw FRED在探测器上穿过多个像素点迭代来创建热图 t&o&gb b:x~Jz#%2 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。 1#XZVp;M 将如下的代码放置在树形文件夹 Embedded Scripts, Tog'3k9Uw H96|{q=
IRsyy\[kp8 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。 |-]'~@~ EiPOY' 绿色字体为说明文字, .aC/ g?U 4@jX{{^6% '#Language "WWB-COM" 8&y#LeM1TT 'script for calculating thermal image map Xz'o<S 'edited rnp 4 november 2005 7!
/+[G w*7wSP 'declarations dlDO?T Dim op As T_OPERATION v|rBOv Dim trm As T_TRIMVOLUME I7;|`jN5K Dim irrad(32,32) As Double 'make consistent with sampling xE6hE'rh.O Dim temp As Double ?V =#x.9 Dim emiss As Double N1JM[<PP Dim fname As String, fullfilepath As String xQxq33\ 'Z6x\p 'Option Explicit 1(WBvAPS g7v(g? Sub Main !)EYM&:Y 'USER INPUTS 4@9xq<<5 nx = 31 =<r1sqf
ny = 31 @h%Nn)QBq numRays = 1000 pE{Ecrc3| minWave = 7 'microns CE|rn8MB maxWave = 11 'microns CS;4 ysNf sigma = 5.67e-14 'watts/mm^2/deg k^4 =DXN`]uN fname = "teapotimage.dat" /Uni6O)oc ~6#O5plKc Print "" |u#7@&N1 Print "THERMAL IMAGE CALCULATION" ;IR.6k$; G^le91$ detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 HDj260a /PE L[Os Print "found detector array at node " & detnode CTQJ=R" ,Y7QmbX^ srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 WIw*//nw
^]?juL Print "found differential detector area at node " & srcnode 3 ]pHc)p!. D/Py?<n-B GetTrimVolume detnode, trm 5Rae?*XH detx = trm.xSemiApe sL#MYW5E dety = trm.ySemiApe 2u(G:cR area = 4 * detx * dety vywpX^KPv Print "detector array semiaperture dimensions are " & detx & " by " & dety cT
nC Print "sampling is " & nx & " by " & ny ,hE989x<iI "-Wb[*U; 'reset differential detector area dimensions to be consistent with sampling C40o_1g pixelx = 2 * detx / nx c-ql pixely = 2 * dety / ny x!n8Wx SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False HbJ^L:/ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 0@Z}.k30 L.: 8qY 'reset the source power !1/F71l DX SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 'i4L.& Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" -0P9|;h5 v4F+^0? 'zero out irradiance array VPb8dv(a3 For i = 0 To ny - 1 Yw_!40` For j = 0 To nx - 1 x7/";L> irrad(i,j) = 0.0 @I#uv|=N Next j ^ U~QQ Next i Yh;A)Np DTHWL 'main loop /|isRh| EnableTextPrinting( False ) M[(pLYq: w[AL'1s] ypos = dety + pixely / 2 ~JO.h$1C For i = 0 To ny - 1 y2=yh30L0E xpos = -detx - pixelx / 2 IRTD(7"oyp ypos = ypos - pixely Z{ 1B:aW -_XTy!I EnableTextPrinting( True ) hw=~%f; Print i /O~Np|~v EnableTextPrinting( False ) W:K '2j Zpz3?VM( K|I<kA~!H For j = 0 To nx - 1 >T-4!ZvS\j 2+ywl}9 xpos = xpos + pixelx Y(R.<LtY F6aC'<#/ 'shift source 8 [D" LockOperationUpdates srcnode, True
Z58{YC Y GetOperation srcnode, 1, op <T&v\DN op.val1 = xpos B<0Kl.V op.val2 = ypos h}kJ,n SetOperation srcnode, 1, op mhB2l/ LockOperationUpdates srcnode, False h J0U-m $m A2AI raytrace 2f620 DeleteRays YrV@k*O* CreateSource srcnode na"!"C
s3 TraceExisting 'draw 'gHg&E9E& pTXF^:8 'radiometry @0d"^ For k = 0 To GetEntityCount()-1 _W^;a If IsSurface( k ) Then N1B$z3E* temp = AuxDataGetData( k, "temperature" ) _
j`tR: emiss = AuxDataGetData( k, "emissivity" ) ]Y!x7 If ( temp <> 0 And emiss <> 0 ) Then (|NC xey ProjSolidAngleByPi = GetSurfIncidentPower( k ) W/AF frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) *ifz@8C } irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi Dp!91NgB p End If >H ?k0M`L %"eR0Lj+zq End If i1!1'T8 57-Hx; Next k }
!y5hv!_ C511hbF Next j s^K2,D]P -Jw4z#/- Next i T6QRr}8`/J EnableTextPrinting( True ) Ka_;~LS>( )BvMFwQG 'write out file *@H\J e` fullfilepath = CurDir() & "\" & fname ,Aai-AGG@ Open fullfilepath For Output As #1 aU^6FI Print #1, "GRID " & nx & " " & ny Qd{8.lB~LQ Print #1, "1e+308" =^i K^) Print #1, pixelx & " " & pixely 8QZI(Xe9r Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 WTJ{M$ gdA2u;q maxRow = nx - 1 8'%m! maxCol = ny - 1 8|)^m[c& For rowNum = 0 To maxRow ' begin loop over rows (constant X) D}LM(s3li7 row = "" X-(4/T+v For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) J=k=cFUX row = row & irrad(colNum,rowNum) & " " ' append column data to row string }ML2-k Next colNum ' end loop over columns oLh ,F"nB P_w4
DU Print #1, row YWvD+ }\Rmwm- Next rowNum ' end loop over rows YO$D- Close #1 [
'lu;1-, }Sbk qd5 Print "File written: " & fullfilepath d?T!)w Print "All done!!" xcU!bDV End Sub &i(Ip'r YrB-n 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: | @$I< C5 Q!_x( #Pp:H/b 找到Tools工具,点击Open plot files in 3D chart并找到该文件 b%%r`j,'JE h]s~w &UOxS W 打开后,选择二维平面图: o3/o2[s V<J1.8H
|
|