Show that for a particle in linear SHM the average kinetic energy over a period of oscillation equals the average potential energy over the same period.
Solution 1
The equation of displacement of a particle executing SHM at an instant t is given as:
`x =Asin omegat`
Where,
A = Amplitude of oscillation
ω = Angular frequency = `sqrt(k/M)`
The velocity of the particle is:
`v = (dx)/(dt) = Aomegacosomegat`
The kinetic energy of the particle is:
`E_k = 1/2 Mv^2 = 1/2 MA^2omega^2 cos^2 omegat`
The potential energy of the particle is:
`E_rho = 1/2 kx^2= 1/2 Momega^2 A^2 sin^2 omegat`
For time period T, the average kinetic energy over a single cycle is given as:
`(E_k)_"Avg" = 1/T int_0^T E_k dt`
= `1/T int_0^T 1/2 MA^2 omega^2 cos^2 omega t dt`
= `1/2T MA^2 omega^2 int_0^T (1+cos 2 omegat)/2 dt`
`= 1/(4T) MA^2omega^2[t + (sin 2 omegat)/(2omega)]_0^T`
`= 1/(4T) MA^2 omega^2 (T)`
`= 1/4 MA^2 omega^2` .... (i)
And, average potential energy over one cycle is given as:
`(E_p)_'Avg" = 1/T int_0^T E_p dt`
`= 1/T int_0^T 1/2 Momega^2 A^2 sin^2 omegat dt`
`= 1/2T Momega^2 A^2 int_0^T ((1-cos 2 omegat))/2 dt`
`= 1/4T Momega^2A^2[(t - sin 2omegat)/2omega]_0^T`
`= 1/"4T" M omega^2 A^2 (T)`
`= (Momega^2A^2)/4` .... (ii)
It can be inferred from equations (i) and (ii) that the average kinetic energy for a given time period is equal to the average potential energy for the same time period.
Solution 2
Let the particle executing SHM starts oscillating from its mean position. Then displacement equation is
`x= A sin omega t`
Particle velocity, `v = Aomega cos omegat`
Instantaneous K.E, `K = 1/2 mv^2 = 1/2 mA^2 omega^2 cos^2 omegat`
Average value of K.E over one complete cycle
`K_"av' = 1/T int_0^T mA^2omega^2 cos^2 omegat dt = (mA^2omega^2)/2T int_0^Tcos^2 omegat dt`
`= (mA^2omega^2)/(2T) int_0^T (1+cos 2omegat)/2 dt`
`= (mA^2omega^2)/(4T) [t +(sin 2 omegat)/(2omega)]_0^T`
`= (mA^2omega^2)/4T[(T-0)+ ((sin 2 omegat - sin 0)/(2omega))]`
`= 1/4 mA^2omega^2` ... (i)
Again instantaneous P.E, `U = 1/2 kx^2 = 1/2 momega^2 x^2 = 1/2 momega^2 A^2 sin^2 omegat`
:. Average value of P.E over one complete cycle
`uu_"av" = 1/2 int_0^T 1/2 momega^2 A^2 sin^2 omegat = (mv^2 A^2)/(2T) int_0^T sin ^2 omegat dt`
`= (momega^2A^2)/(2T) int_0^T ((1-cos 2omegat))/2 dt`
`= (momega^2A^2)/4T [t -(sin 2omegat)/(2omega)]_0^T`
`= (momega^2A^2)/(4T) = [(T-0)- (sin 2omegat -sin 0)/(2omega)]`
`= 1/4 momega^2A^2` .....(ii)
Simple comparision of (i) and (ii) shows that
`K_"av" = uu_"av" = 1/4 momega^2A^2`