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9702 · 17.1

Simple harmonic oscillations — practice questions

Practice and worked examples for 9702 Simple harmonic oscillations. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

A mass oscillating with SHM has an amplitude of 5.0 cm and a period of 1.2 s. Calculate its angular frequency, maximum velocity, and acceleration when its displacement is 3.0 cm.

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**Step 1: Calculateangularfrequency(Calculate angular frequency (\omega).).** The formula is ω=2π/T\omega = 2\pi / T. ω=2π/1.2 s5.236 rad/s\omega = 2\pi / 1.2 \text{ s} \approx 5.236 \text{ rad/s}. Step 2: Calculate maximum velocity (v0v_0). The formula is v0=ωx0v_0 = \omega x_0. Remember to convert amplitude to metres! x0=5.0 cm=0.050 mx_0 = 5.0 \text{ cm} = 0.050 \text{ m}. v0=5.236 rad/s×0.050 m0.2618 m/sv_0 = 5.236 \text{ rad/s} \times 0.050 \text{ m} \approx 0.2618 \text{ m/s}. Step 3: Calculate acceleration (a) at x=3.0 cmx = 3.0 \text{ cm}. The formula is a=ω2xa = -\omega^2 x. Convert displacement to metres. x=3.0 cm=0.030 mx = 3.0 \text{ cm} = 0.030 \text{ m}. a=(5.236 rad/s)2×0.030 m0.822 m/s2a = -(5.236 \text{ rad/s})^2 \times 0.030 \text{ m} \approx -0.822 \text{ m/s}^2.

Worked example 2

A 0.50 kg mass is attached to a spring and oscillates with SHM. The amplitude of the oscillation is 10 cm, and the period is 0.80 s. Calculate: a) The total energy of the system. b) The kinetic energy of the mass when its displacement is 6.0 cm from the equilibrium position.

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**Step 1: Calculateangularfrequency(Calculate angular frequency (\omega).).** The relationship between period T and angular frequency ωis\omega is \omega = 2\pi / T$$. ω=2π/0.80 s=7.854 rad/s\omega = 2\pi / 0.80 \text{ s} = 7.854 \text{ rad/s}.

Step 2: Calculate the total energy of the system (EtotalE_{total}). The total energy in SHM is constant and can be calculated at the point of maximum displacement (amplitude), where all energy is potential. The formula is Etotal=12mω2x02E_{total} = \frac{1}{2} m \omega^2 x_0^2. Remember to convert amplitude to metres: x0=10 cm=0.10 mx_0 = 10 \text{ cm} = 0.10 \text{ m}. Etotal=12×0.50 kg×(7.854 rad/s)2×(0.10 m)2E_{total} = \frac{1}{2} \times 0.50 \text{ kg} \times (7.854 \text{ rad/s})^2 \times (0.10 \text{ m})^2 Etotal=0.25×61.685×0.010.1542 JE_{total} = 0.25 \times 61.685 \times 0.01 \approx 0.1542 \text{ J}. Rounding to two significant figures, Etotal=0.15 JE_{total} = 0.15 \text{ J}.

Step 3: Calculate the kinetic energy (KE) at x=6.0 cmx = 6.0 \text{ cm}. First, convert displacement to metres: x=6.0 cm=0.060 mx = 6.0 \text{ cm} = 0.060 \text{ m}. We know that total energy is the sum of kinetic and potential energy: Etotal=KE+PEE_{total} = KE + PE. Therefore, KE=EtotalPEKE = E_{total} - PE. The potential energy at displacement x is PE=12mω2x2PE = \frac{1}{2} m \omega^2 x^2. PE=12×0.50 kg×(7.854 rad/s)2×(0.060 m)2PE = \frac{1}{2} \times 0.50 \text{ kg} \times (7.854 \text{ rad/s})^2 \times (0.060 \text{ m})^2 PE=0.25×61.685×0.00360.0555 JPE = 0.25 \times 61.685 \times 0.0036 \approx 0.0555 \text{ J}. Now, calculate KE: KE=0.1542 J0.0555 J0.0987 JKE = 0.1542 \text{ J} - 0.0555 \text{ J} \approx 0.0987 \text{ J}. Rounding to two significant figures, KE=0.099 JKE = 0.099 \text{ J}.