An object oscillates or vibrates when it moves back and forth repeatedly on either side of some fixed position (equilibrium position)
Free oscillations occur without a driving mechanism and the oscillating object continues to move for some time after being set into oscillation
Examples of oscillating objects
Thermal vibrations of atoms in a solid, swaying motion of the top of a skyscraper, plucked guitar string, skin of a banged drum, beating of a hummingbird's wings, x-rays, microwaves, radio waves
When an object is set into free oscillation, it will vibrate at a particular frequency called the natural frequency of vibration
A forced oscillation occurs when an object is caused to vibrate by a periodic driving force, making the object vibrate at the forcing frequency
Examples of forced oscillations
Engine vibrations felt in the steering wheel and gear stick of a car
The natural frequency of vibration of an oscillator is the frequency with which it will vibrate freely after an initial disturbance
The wing beat of a mosquito, the pendulum movement in a Grandfather clock, and the vibrations of a cymbal after it has been struck are examples of free oscillations
The shaking of a building during an earthquake and the vibration of a bat are examples of forced oscillations
Types of oscillations
Free oscillations
Forced oscillations
Free oscillations
The pendulum movement in a Grandfather clock
The vibrations of a cymbal after it has been struck
The vibration of a bat after a cricket ball is struck
Forced oscillations
The shaking of a building during an earthquake
The vibrations of a washing machine during its spin cycle
Vibrating loudspeaker cone
Heavily-loaded trolley attached by identical springs
When pulled horizontally to one side and released, it oscillates freely back and forth along the bench
Speed of the trolley during oscillation
Greatest at the centre, zero at the extremities
Kinetic and potential energy during oscillation of the trolley
Maximum kinetic energy and minimum potential energy at the centre, maximum potential energy and zero kinetic energy at the extremities
Pendulum bob oscillation
Freely oscillates at its natural frequency
Speed of the pendulum bob during oscillation
Maximum at the centre, zero at the extremities
Kinetic and potential energy during pendulum oscillation
Maximum kinetic energy at the centre, zero at the extremities; minimum potential energy at the centre, maximum at the extremities
Examples of SHM
Swinging pendulum, oscillating mass-spring system, vibrating loudspeaker cone, vibrations of atoms or molecules in a solid
The equation for a SINUSOIDAL oscillation is: x = A sinωt = A sin(2πft) OR x = A cos(2πft)
MAXIMUM SPEED (vmax) of a simple harmonic oscillator
The maximum speed of a simple harmonic oscillator
Displacement (x)
Distance moved by an oscillating object in either direction from the equilibrium position at any given time
Amplitude (A)
Maximum displacement of an oscillating object from the equilibrium position
Period (T)
Time taken for each complete oscillation
Frequency (f)
Number of complete oscillations per second
Angular Frequency (ω)
Frequency of the oscillations expressed in radians per second
Oscillations and circular motion are closely related
For 1 complete revolution of P, which is 1 complete oscillation of the foot of its perpendicular across XY: ω = 2π/T and ω = 2πf (since T = 1/f)
PHASE is the term used to describe the point that an oscillating object has reached within the complete cycle of an oscillation
PHASE DIFFERENCE between two oscillations tells us the amount by which they are 'out of step' (out of phase) with each other
In Phase
Two points that have exactly the same pattern of oscillation
Antiphase
If the patterns of movement at two points are exactly opposite to each other
Simple Harmonic Motion (SHM)
The oscillatory motion of an object in which acceleration is directly proportional to its displacement from a fixed point and always in the opposite direction to the displacement
Maximum Displacement
xmax = ±A (where A = amplitude)
Time Period (T)
Independent of the amplitude of the oscillations
The variation of displacement (x) with time (t) depends on its initial displacement
If x = 0 when t = 0, the displacement at time (t) is given by x = A sin(2πft)
If x = +A when t = 0, the displacement at time (t) is given by x = A cos(2πft)
The v/t graph can be deduced from the x/t graph because v = dx/dt (velocity = gradient of the displacement/time graph)
v is +ve when dx/dt is +ve (object moving to the right) and v is -ve when dx/dt is -ve (object moving to the left)