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