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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。 >a6{y b#h}g>l 成像示意图 5"5tY 首先我们建立十字元件命名为Target %Y0,ww2 k/U1
: 9 创建方法: 7FQ&LF46 .?<M$38fv 面1 : <FaF67[Q 面型:plane H8$l }pOz 材料:Air nTy8:k '] 孔径:X=1.5, Y=6,Z=0.075,形状选择Box Nft~UggK ?W6qwm,?L O
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辅助数据: 4Lg!54P8 首先在第一行输入temperature :300K, >#9f{ emissivity:0.1; FR bmeq3c CtEpS<*c XBvJc'(s 面2 : \B72 #NR 面型:plane m'j]T/WF 材料:Air ~2HlAU))<& 孔径:X=1.5, Y=6,Z=0.075,形状选择Box 8ztVv (pDu ,sa%u Fm 位置坐标:绕Z轴旋转90度, Wqy\yS [ PG51+# Lo<-;;vQ 辅助数据: eNQQ`ll@m ~!t# M2Sk 首先在第一行输入temperature :300K,emissivity: 0.1; l0
Eh? BXzn-S %ZKP d8 Target 元件距离坐标原点-161mm; 26e. Hu CXAW>VdK_ q=, 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 WLO4P yA+NRWWj >TKl`O 探测器参数设定: 5 R* k}0Y&cT!rU 在菜单栏中选择Create/Element Primitive /plane 006qj. =x &"aF1 6d# 7 c[E" C>MEgGP dcn/|"jr 元件半径为20mm*20,mm,距离坐标原点200mm。 f4mQDRlD 7o99@K, 光源创建: 8@)4)+e B$\,l.hE 光源类型选择为任意平面,光源半角设定为15度。 Q>%{Dn\? G`D~OI Ic<J]+Xq 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。 :`Z'vRj G/)]aGr 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。 !gyEw1Re7 C"gH>G R(1N]> 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。 r@30y/C Z=I+_p_G 创建分析面: .='hYe. C/JFb zVx xY=%+o.?* 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。 iVUkM3 #
o;\5MOE% <@](uWu 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。 v PJ=~*P= myvn@OsEw FRED在探测器上穿过多个像素点迭代来创建热图 ir?Y> S 9;:) 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。 `pJWZ:3 将如下的代码放置在树形文件夹 Embedded Scripts, `h(*D [
U`}) Y+ Qm. 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。 -qDM(zR !iHJ! 绿色字体为说明文字, ;,2;J3,pA !uxma~ZH- '#Language "WWB-COM" xULcS :Q 'script for calculating thermal image map .B? J@, 'edited rnp 4 november 2005 9^zA( c`M
,KXott 'declarations AnW72|=A( Dim op As T_OPERATION vK7J;U+cJ Dim trm As T_TRIMVOLUME (oG-h"^/ Dim irrad(32,32) As Double 'make consistent with sampling $j"TPkW{M Dim temp As Double 713)D4y} Dim emiss As Double `*ml/% \
Dim fname As String, fullfilepath As String >>I~v)a>w 8j^3_lD 'Option Explicit wc~k4B9" ';J><z{> Sub Main 0Vwl\,7z9 'USER INPUTS VUbg{Rb) nx = 31 [CAV"u)0 ny = 31 xU(yc}vw, numRays = 1000 ){M)0,: minWave = 7 'microns 5n#@,V.O/ maxWave = 11 'microns iqAME%m sigma = 5.67e-14 'watts/mm^2/deg k^4 yu98d1 fname = "teapotimage.dat" g-O}e4 J.g4I|{ Print "" i4g99Kvl Print "THERMAL IMAGE CALCULATION" ,Srj38p bi<?m^j detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点 f{j.jfl\x H]a@"gO Print "found detector array at node " & detnode q*pWx]Y =L F9im srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 :dM
eNM- a]%>7yr4 Print "found differential detector area at node " & srcnode \|< 5zL "<^]d~a_ GetTrimVolume detnode, trm 8^U+P% detx = trm.xSemiApe j{ :>"6 dety = trm.ySemiApe 5.o{A#/NTl area = 4 * detx * dety "i1r9TLc Print "detector array semiaperture dimensions are " & detx & " by " & dety @`S8d%6P Print "sampling is " & nx & " by " & ny SBog7An9SI |.;LI=CT 'reset differential detector area dimensions to be consistent with sampling 1XD|H_JG<j pixelx = 2 * detx / nx u^Ss8}d pixely = 2 * dety / ny Au[H!J SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False XL2iK) A Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 WY`hNT6M r_?i l]l 'reset the source power 5:6]ZFW SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) 15L0B5(3 Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" $=rLs) |-!
yKB 'zero out irradiance array $Eh8s( For i = 0 To ny - 1 tiHP?N U For j = 0 To nx - 1 ET:B" irrad(i,j) = 0.0 <RPy Next j "<LVA2v; Next i f6O5k8n _=d
X01 'main loop ,f2tG+P EnableTextPrinting( False ) HaiaDY) Btu=MUS ypos = dety + pixely / 2 fD:>cje For i = 0 To ny - 1 VfON{ 1g xpos = -detx - pixelx / 2 ;+W9EbY2 ypos = ypos - pixely @ApX43U( FaVeP%v EnableTextPrinting( True ) JAA{5@ST Print i Qk_`IlSd EnableTextPrinting( False ) DTi\ 4&41 Dw-i!dq YnLwBJ 2i For j = 0 To nx - 1 Wgr`)D mE+ xpos = xpos + pixelx !/|^
)d^U Y#[>j4<T 'shift source xO nW~Z LockOperationUpdates srcnode, True Z.v2!u GetOperation srcnode, 1, op <z+b88D op.val1 = xpos eo~>|0A*V op.val2 = ypos ;{e=Iz}/ SetOperation srcnode, 1, op |fTWf}Jx LockOperationUpdates srcnode, False #{]Yw}m w\PCBY= 'raytrace u>U4w68 DeleteRays |DZ3=eWZ CreateSource srcnode
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x`|! TraceExisting 'draw gY=Ry=w9 Er]lObfQo 'radiometry X8Ld\vZYn For k = 0 To GetEntityCount()-1 (K>=!&tlp= If IsSurface( k ) Then S7_^E temp = AuxDataGetData( k, "temperature" ) vxrRkOU1 emiss = AuxDataGetData( k, "emissivity" ) IC:wof " If ( temp <> 0 And emiss <> 0 ) Then yk<$XNc ProjSolidAngleByPi = GetSurfIncidentPower( k ) !"e~HZmr frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) Jfkdiyy" irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi 5HAIKc End If
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*AI QoVRZ $!p End If Zagj1OV| 5?()o}VjAO Next k NX5A{ }CyS_Tc Next j on=I*?+R >.]'N:5 Next i w`?Rd EnableTextPrinting( True ) D]UqM<0Rz ,& ^vc_} 'write out file kQY+D1 fullfilepath = CurDir() & "\" & fname KOQ9K Open fullfilepath For Output As #1 0/F/U=Z! Print #1, "GRID " & nx & " " & ny .;'3Roi Print #1, "1e+308" 3n=`SLj/a Print #1, pixelx & " " & pixely d*A(L5;@ Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 =b* Is,R/ ydyGPZt maxRow = nx - 1 uDZ$'a maxCol = ny - 1 +.RC{o, For rowNum = 0 To maxRow ' begin loop over rows (constant X) yQXHEB row = "" (^ Q:zU For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) {#c**' 4 row = row & irrad(colNum,rowNum) & " " ' append column data to row string Rt{`v< Next colNum ' end loop over columns MGmUgc ca!=D $ Print #1, row ~GWn > F$QAWs Next rowNum ' end loop over rows +C(v4@=nd Close #1 t#0/_tD $m:4'r Print "File written: " & fullfilepath WLTraB[? Print "All done!!" 1;4]
HNI End Sub (xJZeY)-b^ _IK@K6V1 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: MwlhL? A?q9(n|A" NNt,J; 找到Tools工具,点击Open plot files in 3D chart并找到该文件 J"x M[c2 =7Wr e[lRY>Pe5 打开后,选择二维平面图: ZN:~etd E!eBQ[@
QQ:2987619807 73C
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