Updating the Bob Smith Termination Technique.docx

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UpdatingtheBobSmithTerminationTechnique

UpdatingtheBobSmithTerminationTechnique

WhiletheBobSmithTerminationtechniquehaswonacclaimworldwide,ithasitsflaws.Fortunately,anewterminationtechniqueisproposedherethatcansolvemanyoftheproblemsdesignerswillencounterwhenusingtheBobSmithapproach.

ByJimSatterwhite,TeltestElectronicLaboratories

FordesignersofEthernetsystems,theBobSmithTerminationtechniqueisregardedasanimportantapproachformigratingpotentialRFemissionandsusceptibilityproblemsforEthernetinfrastructure.But,whatifthetechniquehasflaws?

Unfortunately,therearesomeflawswiththeterminationtechniquepatentedbyBobSmithINthe90s.ThisarticlepointsoutpotentialflawsandthenshowshowaproposedterminationtechniquecansolvesomeoftheproblemsencounteredusingaBobSmithterminationapproach.Thearticlealsoprovidesaphysicalverificationmethodthatdesignerscanusetoanalyzetheimpactoftheproposedterminationtechnique.

Theproblematicresultsofimproperterminationaredifficultdifficulttomeasureandverify.Theyshowupasproblemswithelectromagneticcompatibility(EMCcertificationandworseasintermittentanddifficulttoidentifyperformanceproblemsinservice.Thus,thisarticlewillalsoprovideasoundtheoreticalapproachforevaluatingtheproposedterminationscheme.

ProblemswithMr.Smith

InaU.S.patent,RobertW.(Bob)Smithdescribedamethodtoreducethelongitudinalorcommonmodecurrentonmulti-pairconductorsystemswherethepairsareinterrelatedinauniformmanner.HealludestothefactthatthepairtopairrelationshipsofaCAT5cableformtransmissionlinesinthemselves.

Smithassertsincorrectlythatsuchtransmissionlinesexhibitacharacteristicimpedanceofapproximately145ohms.Hisdescriptionisconfusingandmisleadingbecausehedoesnotdefinetheconfigurationinwhichthisissupposedlyexhibited.Hecorrectlygoesontosaythatthecablecansupportandradiatecommon-modesignals.Moreover,hestatesthatthereisamethodtoreducethecommonmoderadiationbymatchingthecommonmodeimpedanceofthecable,andthenpresentsamethodofterminatingthecommonmodetransmissionline,thatdoesnotinactualityaccomplishthatgoalwell.Histerminationtechniquedoesreducethecommonmoderadiation,butnotoptimallyandnotfromthecorrectunderstanding.

ForaCAT5cable,therearetwocommonmodesofinterest.Thefirstisthepair-wisecommonmodeandthesecondisthecable-wisecommonmode.Inthearticletofollow,we'llnoteswilladdressthepair-wisecommonmode.

Thepair-wisecommonmodehasacommonmodecharacteristicimpedancethatcanbereadilycharacterized,whilethecable-wisecharacteristicimpedanceisgrosslydependentonimplementation.Actually,thecharacteristicimpedanceofthecable-wisecommonmodeisnotameaningfulconceptexceptinsomewell-definedcircumstances.

Withthatbackgroundinmind,let'slookatthepair-wisecommonmodecharacteristicimpedancerelationshipswithinaCAT5cable.AsFigure1pointsout,thepair-wisemodecallsforfourpairswithanintrinsiccharacteristicimpedancebetweeneachpair.Duetotheapproximatesymmetryintheconstructionofthecable,eachpairhasthesamerelationwithanyotherpair.Itisprudenttodefinetherelationshipstobedescribed(Smithdoesn'tdothat).Sincetheinherentcharacteristicimpedancescannotbemeasureddirectly,toverifythetheoryitisnecessarytomeasurethemincombinationsandresolvetheindividualelements.

Figure1:

Pair-wisecharacteristicimpedancesonaCAT5cable.

Thefirstrelationshipisbetweenanytwopairs(Z1-1).Thisparameterissomewhatmeaninglessinapplicationbecauseallfourpairsareinterrelated,butitisusefulandcanbecharacterizednone-the-less.Thesecondandmoremeaningfulrelationshipisthecharacteristicimpedanceofonepairrelativetotheotherthreepairs(Z1-3).Thethirdistherelationshipoftwopairstotheothertwopairs(Z2-2).Forthecaseofonepairversusanyotherpairwiththetworemainingpairsfloating,themeasuredcharacteristicimpedanceisapproximately100ohms.

Forthecaseofonepairversustheotherthreepairstiedtogetherthemeasuredcharacteristicimpedanceisapproximately70ohms.Forthecaseoftwopairstiedtogetherversustheothertwoparstiedtogetherthemeasuredcharacteristicimpedanceisapproximately50ohms.NowheredoesthereexistarelationshipthatthecharacteristicimpedanceisanywherenearSmith'sstated145ohms.

Figure2showsthedefinitionsofsomeofthepossiblemeasurablecharacteristicimpedances.

Figure2:

Definitionsofpossiblemeasurablecharacteristicimpedances.

Table1showssomemeasureddatasamples.TheseweretakenusingtheAgilent4396BNetworkAnalyzer.

Table1:

MeasuredDataSamples.

Analysis

Analysisofthemeasuredvaluestodeterminetheinherentcharacteristicimpedancevaluesiscomplex.Sometechniquesinclude:

Z1-3(1,234)=Z14//Z12//Z13

Z2-2({12,34)=Z14//Z23//Z13//Z24

Z1-3(1,234)=Z12//(ComplicatedcombinationofZ14,Z34,Z23,Z13,Z24)

Thisdoesnotappeartobereadilymanageable.Therefore,asimulationwasdevelopedselectingvaluesforZnntogivevaluessomethingnearthemeasureddata.Fromthis,theintrinsiccharacteristicimpedanceZnnappearstobeinthevicinityof200ohms.Fromthissimulation,itcanbesuggestedthatthevalueofZnnvariesalongthelengthofthecableaswellasfrompairtopair.Thus,toproperlyterminatethecommonmodetransmissionlines,thetechniqueinFigure3mustbeused.

Figure3:

Diagramshowingtheproposedterminationtechniqueapplied.

OnewaytovisualizeaproposedterminationmethodistoterminatetheZ1-3characteristicimpedance.First,thattransmissionlinemustbeterminatedwithavalueequaltoitscharacteristicimpedance.Asingleresistorterminationwillaccomplishthis,howevertheotherthreepairsarenottiedtogetherinnormaluse.

Amoregeneralapproach,intheory,istoformaresistornetworkcomprisedoffourresistorsofequalvalue,oneinserieswiththeotherthreeinparallel.Oncethenetworkissetup,designerscanthencomputetheresistancevaluesuchthatthenetworkmatchestheZ1-3characteristicimpedanceofthecable(Figure4).

Figure4:

Matchingequations.

Smithclaimsthatallfourresistorsshouldbe75ohms(Figure5).Thismeansthata75-ohmresistorinallfourterminationswouldmatchacommonmodeimpedanceof100ohmsforZ1-3.

Figure5:

DiagramshowingtheSmithterminationtechnique.

ButSmithclaimsthecharacteristicimpedanceof"some"common-modeconfigurationthatheisattemptingtomatchis145ohms.Sinceit'sdifficulttounderstandinthepatenttheconfigurationSmithisdescribingandconfigurationstypicallyarenotanywherenear145ohms,itcanonlybeconcludedthatSmith'snumbersandapproachtoderivingthemarewrong.Additionally,hismatchingtechnique,givenacommonmodecharacteristicimpedance,doesnotproduceamatch.

Thus,Smithhasn'tpresentedareallyworkablesolutiontotheproblemhehasrecognized.Forexample,forCAT5andCAT5Ecableanimprovementinreturnlossachievedbyreplacingthe75ohmresistorsby52.3ohmresistors,wouldbefrom15dBtomorethan28dB,givenavariationincommonmodeimpedanceof+/-5ohms.Thevariationofcommonmodecharacteristicimpedanceistakenintoaccountinthecalculationofreturnloss(Table2).

PhysicalVerification

Fortheaboveconclusionstobeaccurate,it'simportanttohaveaphysicalverificationmethod.Fortunately,thereisarelativelysimplemethodfordoingverifyingtheaboveclaims.

Undertheproposedverificationmethod,designersconfigurealengthofcablewiththeterminationresistors,theninsertacommonmodepulsewhilemonitoringthatinsertionwithanoscilloscope(apoorman'sTDR).Apulsegeneratorwithanoutputimpedanceof50ohmsandarisetimeofapproximately1nswasused(Figure6).

Figure6:

Diagramshowingtheverificationsetup.

Intheverificationmethod,ifthecableisproperlymatched,noreflectionshouldbeseen.Ifnot,areflectionwillbeobserved.

Intheexampledescribedinthisarticle,terminationsofthreevalueswereappliedateachendofacablesevenfeetlong.Theresistorvaluesemployedweresetsof52.3,75and100ohms.Thecableemployedwas7feetlong.

TheseriesofscopepresentationsinFigure7showimplementationsofthevariousterminationsforcomparison.Thefactthataterminationinthevicinityof52.3ohmsisproperforthematchcanbeclearlyseen.

Figure7:

Diagramshowingreflectionmatchviews.

Forcalibrationpurposes,severalconditionsareshownareshowninFigure7.Thefirstscopepresentationshowstheoutputofthepulsegeneratorwithnoload.ThesecondshowsthecableconnectedtothepulsegeneratorasinFigure6andthefarendopencircuited.Thethirdisthesameconditionswiththefarendshort-circuited.Theremainingthreescopepresentationsshowtheresultsforthethreevaluesoftheterminationresistance.

Itisclearthatforthe100ohmand75ohmresistancesthereisareflection,whereas,with52.3ohmsthereisnot.Theconclusionisthatinthevicinityof52.3ohmsiscorrectandthatBobSmith's75-ohmvalueisnotcorrect.

Asanote,CAT6cablehasahighercommon-modeimpedance.Thisisexpectedduetothesignificantdifferenceinitsconstruction.Itisanticipatedthatalsoduetoitsmethodofconstructionthatthecharacteristicimpedanceswillbemuchmoreuniformbothversuseachotherandalongthelengthofthecable.

TheoreticalAnalysis

Figure8showsthemodelforcomputationofthetermination

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