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文檔簡介
CST–COMPUTERSIMULATIONTECHNOLOGY|w
ModellingThinMaterialsinCSTSTUDIOSUITE2012
LossyMetalOhmicSheets
TabulatedSurfaceImpedanceThinPanel
VariousMaterialTypes
Materialtypes Availableinwhichsolvers?
*
FIT TLM
*Apartfrom“LossyMetal”,only
availablefortetrahedralmesh.
SurfaceImpedanceMaterials
Inprincipleaclassicaldispersivematerialcouldbeusedtomodelthesematerials.
However,anexcessivelyfinemeshmightbeneeded:
iftheobjectmadeofthatmaterialistoothin
ifthepenetrationdepthofthefieldintotheobjectisvery
small
ifthematerialconsistsofseveralrelativelythinlayers.
Thesurfaceimpedancemodelisawaytoavoidaveryfinemeshinsidethematerial.Useoneofthesematerialtypeswhenevertheskindepthorthematerial’sthicknessistoosmalltomodelin3D.
PrincipleofSurfaceImpedanceMaterials
AsurfaceimpedanceformulationrelatesthetangentialEandHfieldsatthesurfaceofamaterial.
Thefieldinsidethevolumeenclosedbythesurfaceimpedanceisnotcomputed(itisactuallyzero).
k y
Hy
Ez
x
Zs=Ez/Hy
z
k
y
x
Hy1
Hy2
Ez1
z
Ez2
Zt=Ez2/Hy1
CST–COMPUTERSIMULATIONTECHNOLOGY|w
ExtensionoftheSurfaceImpedanceModel:Transferimpedance
Atransferimpedance(Zt)modelrelatestheE-fieldononesideofthematerialsheettotheH-fieldontheotherside;thinpanelmodelusesbothZsandZt
CST–COMPUTERSIMULATIONTECHNOLOGY|w
Transparency
Somematerialtypesallowwavesto“passthrough”themiftheobjectisinfiniythin.Forasurfaceimpedancematerialthismeansthattheelectricfieldonbothsidesofthematerialisthesame.
Lossymetal;corrugatedwall:alwaysopaque
Ohmicsheet:transparentifinfini ythin(i.e.thickness=0);opaqueiftheobjecthasavolume
Surfaceimpedance:user’schoiceifinfini ythin;
opaqueiftheobjecthasavolume
Thinpanel:transparent(hastobeinfini ythin)
CoatedMaterials
3D(thick)objectofcertainmaterialscanhaveacoating
Thesurfaceimpedanceoftheoriginalmaterialisyticallytransformedtotakeintoaccountthe
parametersofthecoatinglayers.
Coatinglayers:“Normal”typematerial,canbedispersive
Theresultisanopaquesurfaceimpedanceobject(transparentonlyforinfini ythinOhmicsheet).
OhmicSheet
Useitifaconstantsurfaceimpedanceoverthewholefrequencyrangeisneeded(inthetransientsolverafirst-ordermodelisused).
Typicalapplications:
ICsimulation(thematerialparametersareoftendirectlygiveninOhmspersquare)
Realizinganon-Cartesianboundaryinthefrequency
solver(filleverythingunwantedwithanOhmicsheetmaterialwhoseinteriorisnotmeshed)
TabulatedSurfaceImpedance
Usethisifthesurfaceimpedanceisstronglyfrequency-dependent(inthetransientsolverafittingofuptoorder10isused).
Typicalapplication:
Lossylayersusedtoabsorborattenuatean ingwavewhicharetoothintobemodelledin3D
CoatedMaterial
Usethismodelforthinabsorbinglayers(dielectrics)cedonmetallicobjects,ifthelayersaretoothintobemodelledin3D,e.g.fordielectric-coatedmetals.
Typicalapplication:
Coating(e.g.RAM)onthesurfaceofanairne
SurfaceModelsforMetalsAccurateatDC
Lossymetalisonlyaccurateathighfrequencies.
ForaccurateDCvalues,onecouldusea“TabulatedSurfaceImpedance”modelwithappropriaow-frequencyandhigh-frequencytabulatedvalues.
ThemacroMaterialsCreateTabulatedSurfaceImpedanceMaterialcanbeusedforthis.
Moreover,itallowsthedefinitionofametalliccoating
(the“CoatedMaterial”typeonlyallowsdielectriccoatings)
Macro:TabulatedSurfaceImpedance
Surfaceimpedanceformultilayeredstructures
Surfaceroughness
Causalityen ment
Example(SurfaceRoughnessRequired)
50mmlong
striplinemodel
FR4dielectricsubstrate–εr=3.5,tgδ=0.06
Summary
Metalwithlosses:“Lossymetal”
AccurateatDC:macro
Thinlossydielectrics(alsouser-definedmetals)
Frequencyindependent:Ohmicsheet
Dispersive:tabulatedsurfaceimpedance
Coatingonmetallicobject
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