| 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。 Hf#/o{=~} 07CGHAxJ`
成像示意图 *8Gx_$t& 首先我们建立十字元件命名为Target KVJiCdg- Z[|(}9v?~ 创建方法: B6,"S5@ `6UW?1_Z5 面1 : /+%1Kq.hP 面型:plane 8He^j5 材料:Air (ZDRjBth[ 孔径:X=1.5, Y=6,Z=0.075,形状选择Box &FGz53fd4 \ B<(9
kpEES{f 辅助数据: Aj-}G^># 首先在第一行输入temperature :300K, A2]N := emissivity:0.1; 7|\[ipVX:3 Q9{% 9;kWuP>k4u 面2 : iz>a0~(K 面型:plane HnrT;!C~ 材料:Air /8lGP!z 孔径:X=1.5, Y=6,Z=0.075,形状选择Box ]x! vPIyq jPhOk>m TR|G4l? 位置坐标:绕Z轴旋转90度, wC;N*0Th R|Y)ow51
qd"*Td 辅助数据: cvi+AZ= anHP5gD 首先在第一行输入temperature :300K,emissivity: 0.1; pz~AsF |>Kf_b Y# .F&\xa{ Target 元件距离坐标原点-161mm; zAS&L%^ tV [p|-G*=00
FX 0^I 0 单透镜参数设定:F=100, bend=0, 位置位于坐标原点 OP{ d(~+ sLPFeibof5 5YJLR; 探测器参数设定: ^!!@O91T $D1Pk 在菜单栏中选择Create/Element Primitive /plane 1P@&xcvS\ =D<46T=(RB
dyD=R Z'hW;^e%_z 3@_je)s pO4}6\1\ 元件半径为20mm*20,mm,距离坐标原点200mm。 mq do@ UeX3cD 光源创建: ^3 F[^#" Hi|' 光源类型选择为任意平面,光源半角设定为15度。 ;VNwx(1l` 79z(n[^ #Q"el3P+q 我们将光源设定在探测器位置上,具体的原理解释请见本章第二部分。 5,|^4
ZA P10`X& 我们在位置选项又设定一行的目的是通过脚本自动控制光源在探测器平面不同划分区域内不同位置处追迹光线。 Cir==7A0 8S&` s+$l.aIO! 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。 8!'#B^ x?VX,9;j 创建分析面: <{JHFU`^ )W(?wv!, : DCj2" 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。 m&EwX ^1- 0,{Dw9W:
xzbyar< 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。 4hr;k0sD (G*--+Gn FRED在探测器上穿过多个像素点迭代来创建热图 1BmevEa) O
sbY}*S 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。 ?TLMoqmXM{ 将如下的代码放置在树形文件夹 Embedded Scripts, =(3Qbb1i #db8ur3?
dc|"34;^" 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。 mpIRe@#Z 'RC(ss1G 绿色字体为说明文字, t:9}~%~ -:h5Ky" '#Language "WWB-COM" r=~yUT 'script for calculating thermal image map 1>[3(o3t 'edited rnp 4 november 2005 m1heU3BUWU j*Ta?'* 'declarations 6Y>MW 4q Dim op As T_OPERATION Hl8-1M$& Dim trm As T_TRIMVOLUME J$%mG*Y( Dim irrad(32,32) As Double 'make consistent with sampling |K YON Q Dim temp As Double U"v(9m@
Dim emiss As Double 4/&Us Dim fname As String, fullfilepath As String 2G=Bav\n+ k"uqso/ 'Option Explicit xa[<k>r3 Zz'(!h Uy Sub Main bN`oQ.Z 4 'USER INPUTS RFU(wek nx = 31 ),(ejRP'r ny = 31 I3uaEv7OZc numRays = 1000 %M2.h;9]*\ minWave = 7 'microns mnzamp maxWave = 11 'microns tV<}!~0,* sigma = 5.67e-14 'watts/mm^2/deg k^4 j7K9T fname = "teapotimage.dat" [=z1~dXKb KdHR.;* Print "" "WdGY*r Print "THERMAL IMAGE CALCULATION" Am'5| R
rs?I,NV detnode = FindFullName( "Geometry.Detector.Surface" ) '找到探测器平面节点
o3 P`y:& d kHcG&) Print "found detector array at node " & detnode >9'G>~P~I= };o6|e:2E srcnode = FindFullName( "Optical Sources.Source 1" ) '找到光源节点 bHH{bv~Z .h~M&d! Print "found differential detector area at node " & srcnode Qw!cd-zc ^>gRK*, GetTrimVolume detnode, trm 'S@% detx = trm.xSemiApe =;-/( C dety = trm.ySemiApe ^hv area = 4 * detx * dety DmEmv/N= Print "detector array semiaperture dimensions are " & detx & " by " & dety OD-CU8X9 Print "sampling is " & nx & " by " & ny 4(o: #9I VT96ph 'reset differential detector area dimensions to be consistent with sampling z'=*pIY5f pixelx = 2 * detx / nx :WIbjI= pixely = 2 * dety / ny S5*wUd*p# SetSourcePosGridRandom srcnode, pixelx / 2, pixely / 2, numRays, False B$1nq#@ Print "resetting source dimensions to " & pixelx / 2 & " by " & pixely / 2 <"{Lv)4 []/=!?5B 'reset the source power VI,z7
\ SetSourcePower( srcnode, Sin(DegToRad(15))^2 ) Z#BwJHh Print "resetting the source power to " & GetSourcePower( srcnode ) & " units" }jBr[S5 JryDbGc8 'zero out irradiance array ~
nNsq(4 For i = 0 To ny - 1 vmK<_xbwd For j = 0 To nx - 1 VQ5T$,& irrad(i,j) = 0.0 [wG?&l$.KB Next j t_6sDr'. Next i izsAn"v
!/znovoD 'main loop [7q~rcf,Z EnableTextPrinting( False ) ^crk8O@Fw XeX0\L')R ypos = dety + pixely / 2 ?`V%[~4_I For i = 0 To ny - 1 E#JDbV1AC xpos = -detx - pixelx / 2 !SEHDRp ypos = ypos - pixely FiMP_ y*S ks<gSCB EnableTextPrinting( True )
Z+`mla Print i YNA %/ EnableTextPrinting( False ) uNZJNrV% !;.i#c_u xfCq;?MupW For j = 0 To nx - 1 ^Crl~~Gk` ..V6U"/ xpos = xpos + pixelx EQ1wyKZS2g 28JWQ%- 'shift source A1e| Y LockOperationUpdates srcnode, True "P\k_-a' GetOperation srcnode, 1, op Pwf2dm$,+ op.val1 = xpos G`!#k!&r op.val2 = ypos 6f,#O8]#5 SetOperation srcnode, 1, op /f~V(DK LockOperationUpdates srcnode, False C9`#57 Pp #X'!wr|- 'raytrace 34_:.QK- DeleteRays \gaGTc2& CreateSource srcnode H8.U#% TraceExisting 'draw +Wh0Of O&!>C7 'radiometry Qc#<RbLL For k = 0 To GetEntityCount()-1 3$[!BPLFO If IsSurface( k ) Then Uq `B#JI temp = AuxDataGetData( k, "temperature" ) rU`#3}s emiss = AuxDataGetData( k, "emissivity" ) Q!(16 If ( temp <> 0 And emiss <> 0 ) Then )pLde_ k ProjSolidAngleByPi = GetSurfIncidentPower( k ) Ql&5fyW frac = BlackBodyFractionalEnergy ( minWave, maxWave, temp ) fw kX-ON irrad(i,j) = irrad(i,j) + frac * emiss * sigma * temp^4 * ProjSolidAngleByPi DcaVT]" End If Ic/D!J{Y `VY -3 End If Tm~a&p .P+om<~B Next k Cp=DdmR "- @{ ) Next j | YmQO#'' Jj4!O3\I Next i ' _Ij9{M EnableTextPrinting( True ) f{MXH&d 1\ d|CSWcU 'write out file N-EVHe'}6 fullfilepath = CurDir() & "\" & fname VSP6osX{ Open fullfilepath For Output As #1 "4"gHs Print #1, "GRID " & nx & " " & ny IoWh&(+KdH Print #1, "1e+308" &QFg= Print #1, pixelx & " " & pixely aal5d_Y Print #1, -detx+pixelx/2 & " " & -dety+pixely/2 <|9s {z oe`t ? (U maxRow = nx - 1 \9TCP;{ maxCol = ny - 1 D_ er( For rowNum = 0 To maxRow ' begin loop over rows (constant X) Lpd q^X row = "" hvCX,^LoJ For colNum = maxCol To 0 Step -1 ' begin loop over columns (constant Y) ,pL%,>R5 row = row & irrad(colNum,rowNum) & " " ' append column data to row string sc
dU Next colNum ' end loop over columns ?CIMez(h h}r64<Y2{ Print #1, row ovJwor a<-NB9o~v Next rowNum ' end loop over rows N
GP}Z4 Close #1 @)=\q`vV cnJ(Fv_F$ Print "File written: " & fullfilepath }tue`">h Print "All done!!" veX#K# End Sub +Qy0K5Ee L5$r<t< 在输出报告中,我们会看到脚本对光源的孔径和功率做了修改,并最终经过31次迭代,将所有的热成像数据以dat的格式放置于: T pXbJ]o9 .`qw8e}y#' aoj6/ 找到Tools工具,点击Open plot files in 3D chart并找到该文件 AX=$r]_ x[l_dmq WgX9k J 打开后,选择二维平面图: ;LEO+,6 nP`#z&C
|
|