Forest UCM Osc Resonance

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Oscillators driven by a source in resonance

¨x+2β˙x+ω20x=f(t)


Complete Solution for the Sinusoidally Driven Damped oscillator

x(t)=xh+xp=C1er1t+C2er2t+Acos(ωtδ)

where

r1=β+β2ω20
r2=β+β2+ω20
A=f0(ω20ω2)2+4β2ω2
δ=tan1(2βω(ω20ω2))


The first two terms in the solution are exponentially decaying and tend to damp the oscillation.

The last term in the solution is the response of the system to a sinusoidal driving force.

Thus you can apply a force to prevent the oscillations from dying out.

Resonance

Resonance is the condition that your applied sinusoidal force is set to a frequency that will maximize the damped oscillations.

This means that the amplitude A is maximized.

since

A=f0(ω20ω2)2+4β2ω2

then for a given forced amplitude (f0)

you can maximize the oscillation by minimizing the denominator term

(ω20ω2)2+4β2ω2

since β is the amount of friction being applied remove energy from the system and ω0 is the natural oscilaltion frequency (constants that characterize the system)

the only term you can change is the drive frequency ω of your applied sinusoidal force.

if your set your sinusoidal force to a frequncy

ω=ω0

then the denominator is minimazed thereby maximizing the amplitude of the forced oscillation.

Resonance occurs when your applied sinusoidal force matches the natural frequency of the oscillaor.

This amplude is

A=f02βω0

Quality factor (Q)

While the natural frequency (ω0) determine the frequency where the maximum oscillation can occur, the dampening force parameter (β) determines the width of the resonance.


Problem 5.41


The "sharpness" of the resonance is quantified in terms of a quality factor given by the ration of the natural frequency to the dampening as

Qω02β

Forest_UCM_Osc#Resonance