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Physics (AS & A Level) 9702 · Chapter 17

Oscillations

Oscillation terms and angular frequency, the defining equation of simple harmonic motion, displacement, velocity and acceleration equations and graphs, energy interchange, damping, and resonance.

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17.1 Simple harmonic oscillations

Terms

TermMeaning
Displacement xxdistance from the equilibrium position, in a given direction
Amplitude x0x_0maximum displacement
Period TTtime for one complete oscillation
Frequency ffoscillations per unit time, f=1/Tf = 1/T
Angular frequency ω\omegaω=2πf=2π/T\omega = 2\pi f = 2\pi/T, in rad/s
Phase differencehow far one oscillation is ahead of another, in radians or degrees

The defining equation

Simple harmonic motion (SHM) occurs when the acceleration is proportional to the displacement from a fixed point, and is always in the opposite direction, so directed towards that point:

a=−ω2xa = -\omega^2 x

The minus sign is what makes it SHM: the acceleration always points back towards the equilibrium. A graph of aa against xx is a straight line through the origin with gradient −ω2-\omega^2.

Examples include a mass on a spring and a simple pendulum at small angles.

Solutions

If timing starts at the equilibrium position:

x=x0sin⁡ωtv=v0cos⁡ωtx = x_0\sin\omega t \qquad v = v_0\cos\omega t

where v0=ωx0v_0 = \omega x_0 is the maximum speed. If timing starts at the maximum displacement, swap to x=x0cos⁡ωtx = x_0\cos\omega t.

The speed at any displacement is:

v=±ωx02−x2v = \pm\omega\sqrt{x_0^2 - x^2}

PositionDisplacementSpeedAcceleration
Equilibrium0maximum, ωx0\omega x_00
Extreme±x0\pm x_00maximum, ω2x0\omega^2 x_0

Graphs

Displacement, velocity and acceleration against time for simple harmonic motion, with each curve shifted by a quarter of a cycle from the next

Displacement, velocity and acceleration against time for simple harmonic motion, with each curve shifted by a quarter of a cycle from the next
  • Velocity is the gradient of displacement against time, and it leads displacement by a quarter of a cycle (π/2\pi/2).
  • Acceleration is the gradient of velocity against time, and it is exactly opposite to the displacement (π\pi out of phase).

17.2 Energy in simple harmonic motion

During SHM, energy continually changes between kinetic and potential, while the total stays constant, if there is no damping.

  • At equilibrium: all kinetic.
  • At the extremes: all potential.

E=12mω2x02E = \tfrac{1}{2}m\omega^2 x_0^2

This comes from the maximum kinetic energy, 12mv02\tfrac{1}{2}mv_0^2, with v0=ωx0v_0 = \omega x_0. So the energy is proportional to the amplitude squared.

The kinetic energy at displacement xx is 12mω2(x02−x2)\tfrac{1}{2}m\omega^2(x_0^2 - x^2), and the potential energy is 12mω2x2\tfrac{1}{2}m\omega^2x^2.

17.3 Damped and forced oscillations, resonance

Damping

A resistive force acting on an oscillating system causes damping: it removes energy, so the amplitude falls over time.

DampingWhat happens
Lightmany oscillations, with the amplitude falling gradually (exponentially) and the period almost unchanged
Criticalreturns to equilibrium in the shortest possible time, with no oscillation
Heavyno oscillation, and a slow return to equilibrium, taking much longer than critical

Displacement-time graphs for light, critical and heavy damping

Displacement-time graphs for light, critical and heavy damping

Car suspensions are close to critically damped, so that the car settles quickly without bouncing.

Forced oscillations and resonance

A free oscillation happens at the system's natural frequency. In a forced oscillation, a periodic driving force makes the system oscillate at the driver's frequency.

Resonance is a maximum amplitude of oscillation, occurring when the driving frequency equals the system's natural frequency. Energy is then transferred from the driver most efficiently.

Amplitude against driving frequency: a resonance peak at the natural frequency, lower and broader with more damping

Amplitude against driving frequency: a resonance peak at the natural frequency, lower and broader with more damping

More damping makes the peak lower and broader, and it moves the peak slightly to a lower frequency.

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