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  • 7/28/2019 Formulae Sheet Final

    1/3

    HacettepeUniversity,MechanicalEngineeringDepartment

    AutomotiveEngineeringProgram

    OMU418:MECHANICALVIBRATION

    1

    FREEVIBRATIONSOFUNDAMPEDSDOFSYSTEMS

    EquationofMotion 0SubjecttoInitialConditions0 0 GeneralSolution

    where

    Period: Frequency: FREEVIBRATIONSOFDAMPEDSDOFSYSTEMS

    EquationofMotion 0 2 0SubjecttoInitialConditions0 0 CriticalDampingCoefficient

    2

    Nondimensionaldampingratio

    2For 1.Thegeneralsolutionis: e eCase1: 1UnderdampedFreeVibrationsGeneralSolution sin Where Dampednaturalfrequencyandperiod

    1

    Logarithmic

    Decrement

    for

    one

    cycle

    21Forsmalldampingratio,Logarithmicdecrementcanbeapproximatedas 2Dampingratiointermsof 4 LogarithmicDecrement forncycle 1

    TotalEnergyoftheSystem

    12 12TheRatiooftheenergydissipatedbetweensuccessive

    cycles

    TheRatiooftheenergydissipatedbetweenmsuccessive

    cycles

    intermsoflogarithmicdecrement

    Case2: 1CriticallyDampedFreeVibrations

    Case3: 1OverdampedFreeVibrations 2 1

    1

    1

    HARMONICEXCITATIONOFSDOFSYSTEMS

    Equationof

    Motion

    ForcedResponseofanUndampedSystemdueto

    SingleFrequencyExcitation

    EquationofMotion sin CASE

    A:

    If

    ParticularSolution sin TotalResponse Applyingtheinitialconditionstototalresponse sincos 1 cos sin

    sin

    CASEB:If

    2 cos TotalResponse Applyingtheinitialconditionstototalresponse cos 2sin 2 cos ForcedResponseofaDampedSystemduetoSingle

    FrequencyExcitation

    EquationofMotion

    2 ParticularSolution Where 2 2 Definefrequencyratio

    Definemagnificationfactor

  • 7/28/2019 Formulae Sheet Final

    2/3

    HacettepeUniversity,MechanicalEngineeringDepartment

    AutomotiveEngineeringProgram

    OMU418:MECHANICALVIBRATION

    2

    11 2The

    following

    are

    noted

    about

    maginification

    factor

    1. 1 when 0. In this case the excitation force isconstant and the forcedeveloped in the springofmassspringdashpotsystem isequaltothevalueoftheeciting

    force.

    2. 0as Theamplitudeoftheforcedresponse isverysmallforhighfrequencyexcitations

    3. Foragivenvalueof,decreaseswithincreasing4. Themagnification factor growswithout bound only for 0. For 0 , the magnification factor has a

    maximumvalueforsomevalueof5. For 0 , the maximum value of magnification

    factoroccursforfrequencyratioof 12 6. Thecorrespondingmaximumvalueof

    is

    1217. For ,maximum value of i.e. 0 occurs for 0.For ,monotonicallydecreasesThenondimensionalformofis Eqn(A)Thefollowingarenotedaboutphaseangle1. The forcedresponseand theecitation forceare inphase

    for 0.For 0,therepsonseand theexcitationareinphaseonlyfor

    0

    2. If 0 and 1, then . If 0, then theexcitation is a pure sine wave while the steadystateresponseisapurecosinewave.Theexcitationisinphase

    with thevelocity.Thedirectionofexcitation isalwaysas

    thedirectionofmotion

    3. If 0and 1, then .The response leadstheexcitation

    4. If 0and 1, then .The signof the steadystateresponseisoppositethatoftheexciatation

    ForcedResponseduetoExcitationWhoseAmplitudeis

    ProportionaltotheSquareoftheExcitationFrequency

    EquationofMotion

    2 FormofExcitationForce sin sin ParticularSolution Define Eqn(B)

    isstillthesame.UseEqn(A)anditsproperties

    Thefollowingarenotedaboutmaginificationfactor 1. 0,ifandonlyif 0,forallvaluesof2. 1forlargeandforallvaluesof3. growswithoutboundnear 1for 04. For0 , hasamaximumforafrequencyratio

    112

    5. For0 ,themaximumvalueofcorrespondstothefrequencyratioandisgivenby 1216. For ,doesnot reachamaximum.grows from

    zerofor 0andapproachesoneforlargeApplication:RotatingUnbalance

    EquationofMotion 2 FormofExcitationForce

    sin

    Define ThedefinitionisthesameasinEqn(B).ResponseduetoHarmonicExcitationofSupport

    EquationofMotion

    Relativemotionofstructurew.r.t.base Ifthebasedisplacementisdefinedas Then Where isdefinedinEqn(B)and isdefinedinEqn(A). And Eqn(C) Eqn(C)Thefollowingarenotedabout1. Theamplituderatioisnearunityforsmall2. For all , 0 1, the amplitude ratio grows until it

    reachesamaximumforfrequencyratioof

    12 18 1

  • 7/28/2019 Formulae Sheet Final

    3/3

    HacettepeUniversity,MechanicalEngineeringDepartment

    AutomotiveEngineeringProgram

    OMU418:MECHANICALVIBRATION

    3

    3. The maximum amplitude ratio corresponding to thefrequencyratio, 4

    4. The amplitude ratio has a value of one for 2,independentofthevalueof

    5. For 2

    ,the amplituderatioislargerforsmallervalue

    of.However,for 2,theamplituderatio issmallerforsmallervalueof.6. For all values of , the amplitude ratio is less than one

    whenandonlywhen 2.

    Fig.1.Thegraphofmagnificationfactorv.s.

    Fig.2.Thegraphofv.s.

    Fig.3.Thegraphof

    v.s.

    Fig.4.ThegraphofTv.s.r

    VIBRATIONISOLATION

    MotionIsolation

    Ifthebasedisplacementisdefinedas Theresponseofthesytstemis Forisolationwewant

    1

    1ifandonlyif 2SeeFig.4foragraphofTanduseEqn(C)tocomputeTandForceIsolation

    Iftheharmonicexcitationforceis

    sin

    Theforce

    transmitted

    to

    ground

    is

    where Forforceisolation 1when 2If is constantor is constant is constant in forcingdue tounbalance i.e. theexpression forTcanbeused

    SeeFig.4foragraphofTanduseEqn(C)tocomputeTand