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Edexcel IAL - Mechanics 3- 3.2 Simple Harmonic Motion- Study notes  - New syllabus

Edexcel IAL – Mechanics 3- 3.2 Simple Harmonic Motion -Study notes- New syllabus

Edexcel IAL – Mechanics 3- 3.2 Simple Harmonic Motion -Study notes -Edexcel A level Maths- per latest Syllabus.

Key Concepts:

  • 3.2 Simple Harmonic Motion

Edexcel IAL Maths-Study Notes- All Topics

Simple Harmonic Motion

A particle is said to move with simple harmonic motion (SHM) if its acceleration is always directed towards a fixed point and is proportional to its displacement from that point.

Defining Equation of SHM

If the displacement of a particle from its equilibrium position is \( x \), then SHM is defined by the equation

\( \ddot{x} = -\omega^2 x \)

where \( \omega \) is a positive constant called the angular speed.

The negative sign indicates that the acceleration is always directed towards the equilibrium position.

Showing That Motion is SHM

To prove that a particle executes SHM in a given situation, it is sufficient to show that its acceleration satisfies

Acceleration \( \propto – \) displacement

That is, the equation of motion can be written in the form

\( \ddot{x} = -\omega^2 x \)

This may be done using either Newton’s laws, energy methods, or geometrical arguments.

Standard Formulae for SHM

For a particle executing SHM with angular speed \( \omega \):

Displacement: \( x = A\cos(\omega t) \) or \( x = A\sin(\omega t) \)

Velocity: \( v = -A\omega\sin(\omega t) \) or \( v = A\omega\cos(\omega t) \)

Acceleration: \( a = -\omega^2 x \)

The period of the motion is

\( T = \dfrac{2\pi}{\omega} \)

Energy in SHM

The total mechanical energy of a particle executing SHM is constant and equal to

\( \dfrac{1}{2}m\omega^2A^2 \)

This energy continually transforms between kinetic and potential energy.

Example :

A particle moves along a straight line such that its acceleration is given by \( a = -9x \). Show that the motion is simple harmonic and find the angular speed.

▶️ Answer/Explanation

The given equation of motion is

\( \ddot{x} = -9x \)

Comparing with \( \ddot{x} = -\omega^2 x \), we identify

\( \omega^2 = 9 \Rightarrow \omega = 3 \)

Conclusion: The motion is SHM with angular speed \( 3 \,\text{rad s}^{-1} \).

Example :

A particle of mass \( 0.5 \) kg is attached to a horizontal spring of spring constant \( 8 \,\text{N m}^{-1} \). Show that the particle performs SHM and find its period.

▶️ Answer/Explanation

For a spring, the restoring force is

\( F = -kx \)

Using Newton’s second law:

\( m\ddot{x} = -kx \)

\( \ddot{x} = -\dfrac{k}{m}x \)

So

\( \omega^2 = \dfrac{8}{0.5} = 16 \Rightarrow \omega = 4 \)

The period is

\( T = \dfrac{2\pi}{4} = \dfrac{\pi}{2} \)

Conclusion: The motion is SHM with period \( \dfrac{\pi}{2} \) s.

Example :

A particle executes SHM with angular speed \( 5 \,\text{rad s}^{-1} \) and amplitude \( 0.2 \) m. Find its maximum speed and maximum acceleration.

▶️ Answer/Explanation

Maximum speed in SHM is

\( v_{\max} = \omega A \)

\( v_{\max} = 5 \times 0.2 = 1 \)

Maximum acceleration is

\( a_{\max} = \omega^2 A \)

\( a_{\max} = 25 \times 0.2 = 5 \)

Conclusion: The maximum speed is \( 1 \,\text{m s}^{-1} \) and the maximum acceleration is \( 5 \,\text{m s}^{-2} \).

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