Question #41179

A simple harmonic oscillator has amplitude a angular velocity ω and mass m. then average energy in one time period will be

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Answer on Question #41179, Physics, Mechanics | Kinematics | Dynamics

A simple harmonic oscillator has amplitude A angular velocity ω\omega and mass m. Then average energy in one time period will be

Solution:

Linear Harmonic oscillator.

Mechanical model: mass m on a spring characterized by a spring constant k.

Elastic restoring force F=kxF = -kx is balanced according to Newton's second law


F=maF = m amx¨=kxm \ddot{x} = - k x


The equation of motion


x¨+ω2x=0\ddot{x} + \omega^2 x = 0


where


ω=km\omega = \sqrt{\frac{k}{m}}


Such system oscillates with amplitude A and angular frequency ω\omega.

Consider solution


x=Asin(ωt+φ)x = A \sin(\omega t + \varphi)


The velocity v is equal to


v=x˙=Aωcos(ωt+φ)v = \dot{x} = A \omega \cos(\omega t + \varphi)


and thus the kinetic energy


K=12mv2=12mA2ω2cos2(ωt+φ)=K0cos2(ωt+φ)K = \frac{1}{2} m v^2 = \frac{1}{2} m A^2 \omega^2 \cos^2(\omega t + \varphi) = K_0 \cos^2(\omega t + \varphi)


where the maximum kinetic energy is equal to


K0=12mA2ω2=12kA2K_0 = \frac{1}{2} m A^2 \omega^2 = \frac{1}{2} k A^2


The potential energy – work done by applied force displacing the system from 0 to x


U(x)=0xkxdx=12kx2U(x) = \int_0^x k x \, dx = \frac{1}{2} k x^2


Substituting x


U(x)=12kA2sin2(ωt+φ)=U0sin2(ωt+φ)U(x) = \frac{1}{2} k A^2 \sin^2(\omega t + \varphi) = U_0 \sin^2(\omega t + \varphi)


where U0U_0 is the maximum potential energy (for x=Ax = A)


U0=12kA2U_0 = \frac{1}{2} k A^2


The average values over one oscillation period are calculated using the definition


f=1t2t1t1t2f(t)dt\langle f \rangle = \frac{1}{t_2 - t_1} \int_{t_1}^{t_2} f(t) \, dt


Thus:


U=0TUdt0Tdt=0TU0sin2(ωt+φ)dtT=12U0=12kA2\langle U \rangle = \frac {\int_ {0} ^ {T} U d t}{\int_ {0} ^ {T} d t} = \frac {\int_ {0} ^ {T} U _ {0} \sin^ {2} (\omega t + \varphi) d t}{T} = \frac {1}{2} U _ {0} = \frac {1}{2} k A ^ {2}


and


K=0TKdt0Tdt=12K0=12kA2\langle K \rangle = \frac {\int_ {0} ^ {T} K d t}{\int_ {0} ^ {T} d t} = \frac {1}{2} K _ {0} = \frac {1}{2} k A ^ {2}


The sum of the kinetic and potential energies in a simple harmonic oscillator is a constant, i.e., KE+PE=constant. The energy oscillates back and forth between kinetic and potential, going completely from one to the other as the system oscillates.

Thus,


E=K+U=12kA2+12kA2=kA2=mA2ω2\langle E \rangle = \langle K \rangle + \langle U \rangle = \frac {1}{2} k A ^ {2} + \frac {1}{2} k A ^ {2} = k A ^ {2} = m A ^ {2} \omega^ {2}


Answer. E=mA2ω2\langle E\rangle = mA^2\omega^2

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