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Questions on simple harmonic motion
Simple harmonic motion is defined by a = −ω²x: the acceleration is proportional to the displacement and directed back towards equilibrium. From that condition follow x = A cos ωt, the speed ±ω√(A² − x²), a maximum speed ωA at the centre and a maximum acceleration ω²A at the extremes. The period is independent of the amplitude.
19 original questions · 55 marks · the simple harmonic motion notes · Periodic motion
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State the defining condition for simple harmonic motion.
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The acceleration is directly proportional to the displacement from the equilibrium position (1) and is always directed towards it: a = −ω2x (a ∝ −x) (1).A body oscillates with a frequency of 2.0 Hz. Calculate its angular frequency.
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ω = 2πf = 2π × 2.0 (1)
ω = 12.6 rad s−1 (1)An oscillator has an angular frequency of 10 rad s−1 and an amplitude of 0.050 m. Calculate its maximum speed.
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vmax = ωA = 10 × 0.050 (1)
vmax = 0.50 m s−1 (1)An oscillator has an angular frequency of 7.0 rad s−1. Calculate the magnitude of its acceleration when its displacement is +0.030 m, and state the direction of this acceleration.
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a = ω2x = 7.02 × 0.030 = 1.5 m s−2 (1). It is directed towards the equilibrium position, opposite to the displacement (1).For a body in simple harmonic motion, state the displacement at which (a) the acceleration is greatest and (b) the speed is greatest.
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(a) At maximum displacement, x = ±A, the extremes of the motion (1). (b) At zero displacement, the equilibrium position (1).A vibrating machine panel completes 50 oscillations in 40 s. Calculate the frequency and the period of the oscillation.
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f = 50/40 = 1.25 Hz (1)
T = 1/f = 0.80 s (1)A body performs SHM at 3.0 Hz with an amplitude of 0.020 m. Calculate its maximum acceleration.
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ω = 2πf = 2π × 3.0 (1)
ω = 18.85 rad s−1 (1)
amax = ω2A = 7.11 m s−2 (1)A glider on an air track performs SHM with amplitude 0.10 m and angular frequency 8.0 rad s−1. Calculate its speed when its displacement is 0.060 m.
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v = ±ω√(A2 − x2) (1)
= 8.0 × √(0.102 − 0.0602) (1)
v = 0.64 m s−1 (1)An oscillator moves as x = A cos ωt with A = 0.15 m and ω = 4.0 rad s−1. Calculate its displacement at t = 0.20 s.
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x = A cos ωt = 0.15 × cos(4.0 × 0.20) (1)
= 0.15 × cos(0.80), with the calculator in radians (1)
x = 0.105 m (1)An oscillator has an angular frequency of 6.28 rad s−1. Calculate its frequency and its period.
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f = ω/2π = 6.28/(2π) = 1.00 Hz (1)
T = 1/f = 1.00 s (1)A buoy bobbing on water performs SHM with amplitude 0.12 m and frequency 0.50 Hz. Timing starts as the buoy passes upwards through its equilibrium position, so its displacement is x = A sin ωt. Calculate its displacement at t = 0.40 s.
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ω = 2πf = 2π × 0.50 = 3.14 rad s−1 (1)
x = 0.12 × sin(3.14 × 0.40), with the calculator in radians (1)
x = 0.114 m (1)A loudspeaker cone reproducing a test tone vibrates in SHM at 250 Hz with amplitude 0.35 mm. The manufacturer claims the cone's maximum acceleration exceeds 50g (g = 9.81 m s−2). Deduce whether the claim is correct.
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ω = 2πf = 2π × 250 = 1571 rad s−1 (1)
amax = ω2A = 15712 × 3.5 × 10−4 (1)
amax = 864 m s−2 (1)
50g = 490 m s−2, and 864 m s−2 is larger, so the claim is correct (1)An oscillator is released from rest at its amplitude of 0.080 m and has a period of 1.2 s, so x = A cos ωt. Calculate the time at which its displacement first falls to 0.020 m.
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cos ωt = 0.020/0.080 = 0.25 (1)
ωt = cos−1(0.25) = 1.32 rad, with ω = 2π/1.2 = 5.24 rad s−1 (1)
t = 1.32/5.24 = 0.25 s (1)A body performs SHM with amplitude 0.080 m and period 0.50 s. Calculate (a) its angular frequency, (b) its maximum speed and (c) its maximum acceleration.
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(a) ω = 2π/T = 2π/0.50 (1)
ω = 12.57 rad s−1 (1)
(b) vmax = ωA = 1.01 m s−1 (1)
(c) amax = ω2A = 12.6 m s−2 (1)An object performs SHM of amplitude 0.10 m. Calculate the displacement at which its speed is half of its maximum speed.
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v = ½vmax: ½ωA = ω√(A2 − x2) (1)
¼A2 = A2 − x2 (1)
x = (√3/2)A (1)
x = 0.087 m (1)Describe the phase relationship between the displacement, velocity and acceleration in SHM.
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Velocity is a quarter of a cycle (90°) ahead of displacement (1), and is greatest when displacement is zero (1). Acceleration is exactly out of phase (180°) with displacement, being greatest and opposite when displacement is at a maximum (1).A student measures the acceleration of an oscillating trolley at three displacements. At x = 0.020 m, a = −0.50 m s−2; at x = 0.040 m, a = −1.00 m s−2; at x = 0.060 m, a = −1.50 m s−2. Deduce whether the motion is simple harmonic and, if it is, determine the angular frequency.
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a/x is the same for every pair: −0.50/0.020 = −1.00/0.040 = −1.50/0.060 = −25 s−2, so a ∝ x (1)
The acceleration is opposite in sign to the displacement, that is directed towards equilibrium, so the motion is SHM (1)
Comparing with a = −ω2x gives ω2 = 25 s−2 (1)
ω = 5.0 rad s−1 (1)An oscillator of period T passes through its equilibrium position at t = 0, so x = A sin ωt. Show that the time it takes to travel from the equilibrium position to a displacement of A/2 is T/12.
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A/2 = A sin ωt gives sin ωt = ½ (1)
The first solution is ωt = π/6 (1)
With ω = 2π/T, t = (π/6)/(2π/T) = T/12 (1)A component in a machine oscillates with SHM. Sensors record a maximum speed of 0.90 m s−1 and a maximum acceleration of 14 m s−2. Determine the angular frequency, the amplitude and the frequency of the oscillation.
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amax/vmax = ω2A/(ωA) = ω (1)
ω = 14/0.90 = 15.6 rad s−1 (1)
A = vmax/ω = 0.90/15.6 = 0.058 m (1)
f = ω/2π = 2.5 Hz (1)
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