Answer on Question #41179, Physics, Mechanics | Kinematics | Dynamics
A simple harmonic oscillator has amplitude A angular velocity ω \omega ω 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 = − k x F = -kx F = − k x is balanced according to Newton's second law
F = m a F = m a F = ma m x ¨ = − k x m \ddot{x} = - k x m x ¨ = − k x
The equation of motion
x ¨ + ω 2 x = 0 \ddot{x} + \omega^2 x = 0 x ¨ + ω 2 x = 0
where
ω = k m \omega = \sqrt{\frac{k}{m}} ω = m k
Such system oscillates with amplitude A and angular frequency ω \omega ω .
Consider solution
x = A sin ( ω t + φ ) x = A \sin(\omega t + \varphi) x = A sin ( ω t + φ )
The velocity v is equal to
v = x ˙ = A ω cos ( ω t + φ ) v = \dot{x} = A \omega \cos(\omega t + \varphi) v = x ˙ = A ω cos ( ω t + φ )
and thus the kinetic energy
K = 1 2 m v 2 = 1 2 m A 2 ω 2 cos 2 ( ω t + φ ) = K 0 cos 2 ( ω t + 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) K = 2 1 m v 2 = 2 1 m A 2 ω 2 cos 2 ( ω t + φ ) = K 0 cos 2 ( ω t + φ )
where the maximum kinetic energy is equal to
K 0 = 1 2 m A 2 ω 2 = 1 2 k A 2 K_0 = \frac{1}{2} m A^2 \omega^2 = \frac{1}{2} k A^2 K 0 = 2 1 m A 2 ω 2 = 2 1 k A 2
The potential energy – work done by applied force displacing the system from 0 to x
U ( x ) = ∫ 0 x k x d x = 1 2 k x 2 U(x) = \int_0^x k x \, dx = \frac{1}{2} k x^2 U ( x ) = ∫ 0 x k x d x = 2 1 k x 2
Substituting x
U ( x ) = 1 2 k A 2 sin 2 ( ω t + φ ) = U 0 sin 2 ( ω t + φ ) U(x) = \frac{1}{2} k A^2 \sin^2(\omega t + \varphi) = U_0 \sin^2(\omega t + \varphi) U ( x ) = 2 1 k A 2 sin 2 ( ω t + φ ) = U 0 sin 2 ( ω t + φ )
where U 0 U_0 U 0 is the maximum potential energy (for x = A x = A x = A )
U 0 = 1 2 k A 2 U_0 = \frac{1}{2} k A^2 U 0 = 2 1 k A 2
The average values over one oscillation period are calculated using the definition
⟨ f ⟩ = 1 t 2 − t 1 ∫ t 1 t 2 f ( t ) d t \langle f \rangle = \frac{1}{t_2 - t_1} \int_{t_1}^{t_2} f(t) \, dt ⟨ f ⟩ = t 2 − t 1 1 ∫ t 1 t 2 f ( t ) d t
Thus:
⟨ U ⟩ = ∫ 0 T U d t ∫ 0 T d t = ∫ 0 T U 0 sin 2 ( ω t + φ ) d t T = 1 2 U 0 = 1 2 k A 2 \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} ⟨ U ⟩ = ∫ 0 T d t ∫ 0 T U d t = T ∫ 0 T U 0 sin 2 ( ω t + φ ) d t = 2 1 U 0 = 2 1 k A 2
and
⟨ K ⟩ = ∫ 0 T K d t ∫ 0 T d t = 1 2 K 0 = 1 2 k A 2 \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} ⟨ K ⟩ = ∫ 0 T d t ∫ 0 T K d t = 2 1 K 0 = 2 1 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 ⟩ = 1 2 k A 2 + 1 2 k A 2 = k A 2 = m A 2 ω 2 \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} ⟨ E ⟩ = ⟨ K ⟩ + ⟨ U ⟩ = 2 1 k A 2 + 2 1 k A 2 = k A 2 = m A 2 ω 2
Answer. ⟨ E ⟩ = m A 2 ω 2 \langle E\rangle = mA^2\omega^2 ⟨ E ⟩ = m A 2 ω 2
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