Syllabus Edition

First teaching 2023

First exams 2025

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Phase Angles in Simple Harmonic Motion (SHM) (HL) (HL IB Physics)

Revision Note

Katie M

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Katie M

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Phase Angles in Simple Harmonic Motion

  • Two points on a sine wave, or on different waves, are in phase when they are at the same point in their wave cycle
    • The angle between their wave cycles is known as the phase angle

3-1-7-phase-angles-circle-sine-wave-comparison

The relationship between a sine wave and phase angle

  • If an oscillation does not start from the equilibrium position, then it will be out of phase by an angle of ϕ
    • This would be compared to an oscillation which does start from the equilibrium position
  • The phase angle ϕ of an oscillation (in SHM) is defined as

The difference in angular displacement compared to an oscillator which has a displacement of zero initially (i.e. x space equals space 0 when t space equals space 0)

  • The phase angle can vary anywhere from 0 to 2π radians, i.e. one complete cycle
  • With the inclusion of the phase angle ϕ, the displacement, velocity and acceleration SHM equations become:

x space equals space x subscript 0 sin space open parentheses omega t space plus space ϕ close parentheses

v space equals space omega x subscript 0 cos space open parentheses omega t space plus space ϕ close parentheses

a space equals space minus omega squared x subscript 0 sin space open parentheses omega t space plus space ϕ close parentheses

  • If two bodies in simple harmonic motion oscillate with the same frequency and amplitude, but are out of phase by straight pi over 2, then:
    • The displacement of the oscillator starting from the equilibrium position is represented by the equation x space equals space x subscript 0 sin space omega t
    • The displacement of the oscillator which leads by straight pi over 2 is represented by the equation x space equals space x subscript 0 sin space open parentheses omega t space minus space straight pi over 2 close parentheses

3-1-7-phase-angle-shm-example

Two oscillators which are out of phase by ϕ space equals space straight pi over 2. The blue-dotted wave represents an oscillator starting from the equilibrium position and the red wave represents an oscillator leading by straight pi over 2

  • When a sine wave leads by a phase angle of straight pi over 2, this is equivalent to the cosine of the wave

x space equals space x subscript 0 sin space open parentheses omega t space minus space pi over 2 close parentheses space equals space x subscript 0 cos space omega t

  • Alternatively, a sine wave can be described as a cosine wave that lags by straight pi over 2

x space equals space x subscript 0 cos space open parentheses omega t space plus space pi over 2 close parentheses space equals space x subscript 0 sin space omega t

  • Notice: 
    • For a wave that lags the phase difference is bold plus pi over 2
    • For a wave that leads the phase difference is bold minus pi over 2
  • This is the opposite sign to the one you might think.

 

How are sine and cosine functions related?

3-1-7-phase-angle-sine-cosine-relationship3-1-7-phase-angle-sine-cosine-relationship

Sine and cosine functions are simply out of phase by straight pi over 2 radians

  • The general rules for phase shifts of sine and cosine functions are shown in the table below
Graph Equation Phase shift
3-1-7-phase-angle-sine-minus-relationship sin space open parentheses omega t space minus space ϕ close parentheses Shifts by ϕ to the right (positive direction)
3-1-7-phase-angle-sine-plus-relationship sin space open parentheses omega t space plus space ϕ close parentheses Shifts by ϕ to the left (negative direction)
3-1-7-phase-angle-cos-minus-relationship cos space open parentheses omega t space minus space ϕ close parentheses Shifts by ϕ to the right (positive direction)
3-1-7-phase-angle-cos-plus-relationship cos space open parentheses omega t space plus space ϕ close parentheses Shifts by ϕ to the left (negative direction)

Worked example

An object oscillates with simple harmonic motion which can be described by the equation

x space equals space x subscript 0 space cos space open parentheses omega t space minus space straight pi over 2 close parentheses

Which of the following graphs correctly represents this equation?

3-1-7-phase-angle-shm-mcq-worked-example

Answer:  C

  • The equation x space equals space x subscript 0 space cos space open parentheses omega t space minus space straight pi over 2 close parentheses is equivalent to x space equals space x subscript 0 space sin space open parentheses omega t close parentheses
  • This describes an oscillation where x space equals space 0 when t space equals space 0
    • Hence, options A & D are not correct
  • When sin space open parentheses omega t close parentheses is positive, the oscillation will start moving in the plus x direction
    • Hence, option B is not correct

Worked example

A mass attached to a spring is released from a vertical height of h subscript m a x end subscript at time t space equals space 0. The mass oscillates with a simple harmonic motion of period T.

3-1-7-phase-angle-shm-mass-spring-worked-example1

The graph shows the variation of h with t.

3-1-7-phase-angle-shm-mass-spring-worked-example2

(a)
State the equation of motion for this oscillation.
(b)
A second mass-spring system is set up and made to oscillate with the same frequency but with a phase angle of ϕ space equals space minus straight pi over 4. On the graph, sketch the variation of h with t for the second mass-spring system.

 

Answer:

(a)

  • The displacement-time equation for an oscillator released from a maximum displacement has the form

x space equals space x subscript 0 cos space omega t

or

x space equals space x subscript 0 sin space open parentheses omega t space minus space straight pi over 2 close parentheses

As the graph is leading a normal sine graph by pi over 2

  • Where x space equals space h and x subscript 0 space equals space h subscript m a x end subscript
  • Angular frequency omega is equal to

omega space equals space fraction numerator 2 straight pi over denominator T end fraction

  • Therefore, the equation of motion for this oscillation is: 

h space equals space h subscript m a x end subscript cos space open parentheses fraction numerator 2 straight pi over denominator T end fraction t close parentheses

or

h space equals space h subscript m a x end subscript sin space open parentheses fraction numerator 2 straight pi over denominator T end fraction t space minus space straight pi over 2 close parentheses

(b)

  • One complete oscillation is equivalent to 2π rad

SHaGKqtx_3-1-7-phase-angle-shm-mass-spring-worked-example-ma

  • A phase angle of ϕ space equals space minus straight pi over 4 corresponds to a shift to the right (positive direction)

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Katie M

Author: Katie M

Expertise: Physics

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.