Question #73505

Giving the necessary mathematical expressions, discuss the transient and steady state
of a weakly damped forced oscillator. Show that the average power absorbed by a
forced oscillator is given by
<p > = (bF2/m) w2/w2-w2+4b2w2
1

Expert's answer

2018-02-19T09:44:07-0500

Answer on question #73505-physics-mechanics|relativity.

For a damped oscillator, amplitude will decrease with time because of resistive forces. This has the effect of energy decreasing with time too.

The equation for the displacement of a forced oscillator is given as


d2xdt2+ω2+dxdt2b=fcosωt\frac {d ^ {2} x}{d t ^ {2}} + \omega^ {2} + \frac {d x}{d t} 2 b = f c o s \omega t


The general solution to this differential equation is given as x(t)=x1(t)+x2(t)x(t) = x1(t) + x2(t) where x1(t)x1(t) is the complementary function and x2(t)x2(t) is the particular integral. In transient state, x1(t)x1(t) decays exponentially to zero as time increases hence the damped oscillation of the system dies off. The system now oscillates with the driving force frequency called the steady state. The solution of the equation at steady state is given as


x2(t)=Acos(ωtδ)=fcos(ωt)x 2 (t) = A c o s (\omega t - \delta) = f c o s (\omega t)


Velocity of the system, dx2(t)dt=aωsin(ωtδ)\frac{dx2(t)}{dt} = a\omega \sin (\omega t - \delta) .

Average power absorbed by the system

Power=force×velocity, f (t)=fcos(ωt) and v=aωsin(ωt-δ).

<p>=ωfacosωt(sinωtcosδcosωsinδ),=ωfAcosωtsinωtcosδωfAcos2ωtsinδ< p> = \omega f a c o s \omega t (s i n \omega t c o s \delta - c o s \omega s i n \delta), = \omega f A c o s \omega t s i n \omega t c o s \delta - \omega f A c o s ^ {2} \omega t s i n \delta

Taking one complete cycle of power over time average, <cosωtsinωt>=0< \cos \omega t \sin \omega t > = 0 and <cos2ωt>=1/2< \cos^2 \omega t > = 1/2

<p>=ωf1/2sinδ< p> = \omega f1 / 2\sin \delta , but sinδ=2bω/((w2ω2)+4b2ω2\sin \delta = 2b\omega /\sqrt{((w^2 - \omega^2) + 4b^\wedge 2\omega^\wedge 2}

<p>=ωf1/2×2bω/((w2ω2)+4b2ω2)< p> = \omega f1 / 2 \times 2b\omega / \sqrt{((w^{\wedge}2 - \omega^{\wedge}2) + 4b^{\wedge}2\omega^{\wedge}2)}

<p>=bF2/m×ω2/((w2ω2)+4b2ω2)< p> = b F^{\wedge}2 / m \times \omega^{\wedge}2 / ((w^{\wedge}2 - \omega^{\wedge}2) + 4b^{\wedge}2\omega^{\wedge}2)

Reference

1. Dr.M ghosh,Dr. D Bhattacharyya(2014) oscillations, waves and acoustics.


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