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Simple harmonic motionEdexcel International A Level Further Maths: Revision notes

Section 1

What simple harmonic motion is

A particle moves with simple harmonic motion (SHM) about a centre OO if its acceleration is always directed towards OO and is proportional to its displacement from OO: x¨=−ω2x.\ddot x=-\omega^2x. Here ω\omega is the angular frequency in rad s−1^{-1}. The minus sign means the acceleration opposes the displacement. The motion is centred on OO and oscillates between x=±ax=\pm a, where aa is the amplitude.

Key termssimple harmonic motionangular frequencyamplitude

Section 2

Proving that motion is SHM

To prove SHM in a given situation: choose a variable xx for the displacement from the centre (the equilibrium position), use Newton's second law along the line, and show that the equation becomes x¨=−ω2x\ddot x=-\omega^2x for some positive constant ω\omega. Example: a 22 kg particle with force 18x18x N towards OO gives 2x¨=−18x2\ddot x=-18x, so x¨=−9x\ddot x=-9x and ω=3\omega=3. The negative sign and the position of xx are essential: it must be measured from the centre, where the resultant force is zero.

Key termsequilibrium position
Common mistake

Measuring xx from the wrong point. If xx is not measured from the centre you will not get x¨=−ω2x\ddot x=-\omega^2x, only x¨=−ω2x+\ddot x=-\omega^2x+ constant.

Section 3

Standard results

The following may be quoted without proof: x=acos⁡ωt or x=asin⁡ωt,v2=ω2(a2−x2),T=2πω.x=a\cos\omega t\ \text{or}\ x=a\sin\omega t,\qquad v^2=\omega^2(a^2-x^2),\qquad T=\frac{2\pi}{\omega}. Use x=acos⁡ωtx=a\cos\omega t if t=0t=0 at an extreme position and x=asin⁡ωtx=a\sin\omega t if t=0t=0 at the centre OO. The speed is greatest at OO, where vmax⁡=aωv_{\max}=a\omega, and zero at x=±ax=\pm a. The magnitude of the acceleration is greatest at x=±ax=\pm a, where it equals aω2a\omega^2, and zero at OO. The frequency is 1T=ω2π\frac1T=\frac{\omega}{2\pi} hertz.

Key termsperiodmaximum speed
Exam tip

Set your calculator to radians whenever ωt\omega t is an angle in x=acos⁡ωtx=a\cos\omega t.

Section 4

Using the formulae

For speed at a given displacement use v2=ω2(a2−x2)v^2=\omega^2(a^2-x^2). If two (speed, displacement) pairs are given, substitute both and subtract to find ω\omega then aa. For times, solve the trig equation for the smallest positive tt. A time between two points is the difference of the two times measured from the same origin, provided both are on the same side of the centre and you choose the first occurrences.

Key termstrigonometric equation
Common mistake

Taking a time between two points as a single trig solution. Find each time separately and subtract.

Section 5

Worked example

A particle moves with SHM: at x=1.5x=1.5 its speed is 44 and at x=2x=2 it is 33. Then 16=ω2(a2−2.25)16=\omega^2(a^2-2.25) and 9=ω2(a2−4)9=\omega^2(a^2-4), so 7=1.75ω27=1.75\omega^2, ω=2\omega=2 and a2=6.25a^2=6.25, a=2.5a=2.5. Starting at OO, x=2.5sin⁡2tx=2.5\sin2t. At x=1.5x=1.5: t=0.322t=0.322 s; at x=2x=2: t=0.464t=0.464 s; the time between them is 0.1420.142 s.

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Exam questions on Simple harmonic motion

  1. A particle moves in a straight line with simple harmonic motion about a centre OO. The amplitude of the motion is 0.50.5 m and the period is 22 s.
    Find the speed of the particle when it is 0.30.3 m from OO.2 marks
  2. The displacement of a particle PP from a fixed point OO on a straight line, at time tt seconds, is x=0.4cos⁡3tx=0.4\cos3t metres.
    Find the first time at which PP is at x=−0.2x=-0.2 m.2 marks
  3. A particle PP of mass 22 kg moves on a smooth horizontal straight line. When PP is at displacement xx metres from a fixed point OO on the line, the only horizontal force on PP is directed towards OO and has magnitude 18x18x N.
    Show that PP moves with simple harmonic motion, and find the period of the motion.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).