a set is posted set duebe real no oscillation damping tone and restorative restorative force force...

12
Reminders a Problem Set 10 is posted problem Set 11 will be due on the last day of class Exam 2 will take place this Thursday in the following manner At 6pm on Thursday you will receive the exam via email you must submit the ocean by 6pm on Friday If you foresee this presents Scheduling problems email me immediately today Wronski au 3.2 3 6 Mechanical and electrical vibrations 3.7 Undetermined coefficients 3.25 and Vaiak of parameter 3 6 Wronsk ian Consider the equakin att c bet it CH U O 7 Suppose you have two solutm u Lt and

Upload: others

Post on 24-Jan-2021

1 views

Category:

Documents


0 download

TRANSCRIPT

  • Reminders a Problem Set 10 is postedproblem Set 11 will be due on

    the last day of class

    Exam 2 will take place thisThursday in

    the following mannerAt 6pm on

    Thursday you will

    receive the examvia email you

    must submit theocean by 6pm on

    FridayIf you foresee this

    presents

    Scheduling problems emailme

    immediately

    todayWronski au 3.2 3 6Mechanical and electrical vibrations

    3.7

    Undetermined coefficients 3.25and

    Vaiak of parameter3 6

    Wronsk ian

    Consider the equakinatt c bet it CH U O 7

    Suppose you havetwo solutm u Lt and

  • zit and you want to solve the

    initial value problemfor with

    Uco Uo ie co ie

    Uo Io Sone given number

    we look for aSouther of the fon

    Ult C UH Cz Udt

    Ci Cz thumhento be determined

    The numbers Ci Czare given by the

    system of algebraic equatuC U Cos Cz UzCo7 Uo

    e ie Ca c Cz UID lio

    There is one condition onthe coefficients

    Udo Uz lo ieK cider that

    guarantees this always has oneand

    exactly are soluhr 9,4

    CaioThe condition is

    der I o

  • The Wronskian of two solutions

    u and uz 13the functor of

    t given by

    triumitt dett Ya

    U A Walt il A Udt

    Exera.se SeeProklensetWe have seen Thor

    for a Z d

    system I AX

    and two fundamentalsolders 71,72

    that theirwronshian f der five 5k

    solves the equatorW tr A W

    when for A 94 91 the

    tr A au 1922

    bell

  • E For each equation bellae

    let's find a set of fundamentalHf

    solutions and compete their Wronskian

    1 is 144 0Characteristicpolynomial d 4Roots are 112 4

    0 X I 2 I

    Sit and eZit are solution their

    real and imaging pantsare trees also

    sobbing u wee getµ it cos

    Zt Uz Ct sink 1

    Their Wronski an i's

    D u Uz t Ulitz El Uzcos Zt 2Costa f zsin

    sink

    zcoscztf zsinczc72z.to

    Hi cuz it 2

    2 it Zvi Yu Ocharacteristic polynomial 12

    211 4

    Roots use quadraticformula D 2IF2

    l I I V127I I jI iT t arealpart imaginaryport

  • Then we haveU Lt e cos Dt

    Uch e thin Pt

    Wronski anEr Its etoes t B e

    tsin Dt

    insect Etsi Dt Bet us taftersomecancellations

    u iz U 42 e cos 32e si e

    Z

    Z tBe 2T

    True uz it Be

    3 it 5 it 4 u O TAK2 154 4 0

    moons51 25102

    Note boaEhueigseamaml.es

    5235 4utt

    Uz It eU It e utu H e

    t ie Ct Ye

    wit et fue at f Et e

    ut

    5TMtle51

    3 e

  • u ii 3 at 44 0

    d2 3 4 0

    moon 3 0296 31722

    Zz I IA

    Tal parTimagm past

    wilt e Ztcos htt

    Uz It e Etsi AtTutti exercise

    A autbn

    The charactersher equatorfor

    This equateis

    a Rtbdt C 0

    The roots are

    D EaVb2

    za

    Xz Fa Visz a

  • Note that the sign of5 Uac

    determines if the roots are real

    or not

    If b 0 anda c 30 Then

    the roots are purely imaginary

    Ii aand solutions are

    ascfat in fatIf b 0 and a c

    0 then if

    b is smell we willget tf Ya Ceo

    and the roots well de

    de Ia iVua

    29

    112 Ia ib2Za

    If we unite ft FaW

    Uac 52Ta

    the solutes beam

    u A enters cwt uz Henthicwt

    functors oh

  • so there are functus oscillating butalso deaagins exponentiallylastly if bSO and sufficiently lazethem b2 Uac

    O and the roots willbe real no oscillation

    Damping tone andrestorative

    restorativeforce forcemoi K x k

    o

    Hooke's Law

    m I e KK 25gdamp.rs frichn

    Iq9mneeThe results quite has thefirm Moitra Kx 0

    ahu Mgr KH

  • In summaryNo damping b o

    perfectly oscillatingsolutes

    Some damp'sb 0 small oscillatingexponential

    decay

    More daeemi b 0 laze wemore

    oscillate purelyexponentialbehave

    One moreterm

    m KK JI fitExternefForce

    This leads to consider

    inhomogeneous equationsacit bit cu fees

  • InhomogeneousequationTwo methods

    Dyariatu of parameter2 Undetermined coefficients

    Vor of parameters Two waysof thinking about

    it

    The books's Sechin 3.6

    Redneck to 2 d systemsUw of pants in Chapter 7

    I'll discuswhen dealing

    with

    a t bit cue fees

    one approach is toconsider

    the corresponding2 d system

    iI

  • ex Ea ba xt Isto the system we

    can applyaide of parameters get

    a solute xH7 of which

    the first componentwill be

    the solution tothe 2nd order

    We get the followingif

    UK weltsare a fondurutd

    ergshen ofsolutes to

    a iitbie tea D

    Then a particular solutesto

    aiitb.ci Ccn fris green by

  • Upa

    f sina.I.fisds um iI d was

    The guard solute isRen

    Singhacts C UCH 1 Cz

    Uit t 4pctI