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Vibrations and waves · Vibrations

Simple harmonic motion

A swing in a playground in Galway, a tuning fork, an engine piston, the needle of a seismograph: all of them oscillate about an equilibrium position and always return to it. If the motion is sufficiently "clean" —the force that causes it is proportional to the displacement and acts in the opposite direction— a single type of mathematical equation describes it precisely: simple harmonic motion (SHM). This page gives you the language and the equations for it, and shows you how to measure it in the lab, as you will do in your Physics in Practice Investigation.

Displacement, amplitude, period and frequency

If you attach a marker to the end of a mass oscillating on a spring and pull a strip of paper beneath it at a constant rate, the tip draws a smooth, periodic curve identical to a sine function: how can we describe, with mathematical precision, the position, the rhythm and the reach of that back-and-forth motion at every instant?

Sinusoidal graph of the displacement x against time t, with the amplitude A measured from equilibrium to a crest and the period T as one complete oscillation. x t 0 A T 1 oscillation
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A swing oscillates freely after a push. Timing with a stopwatch, it completes $15$ full oscillations in $30\ \text{s}$. The figure shows the swing in three positions…

A swing oscillates freely after a push. Timing with a stopwatch, it completes $15$ full oscillations in $30\ \text{s}$. The figure shows the swing in three positions during its oscillation.

equilibrium displacement x amplitude A
  1. a) Define, applying them to the swing, the concepts of displacement, amplitude, period and frequency.
  2. b) Calculate the period $T$ and the frequency $f$ of the oscillation.
Solve
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An electrocardiogram records a heart rate of $75$ beats per minute, perfectly regular. The figure represents the recorded signal. a) Calculate the frequency of the…

An electrocardiogram records a heart rate of $75$ beats per minute, perfectly regular. The figure represents the recorded signal.

75 beats/min beat T = ? t
  1. a) Calculate the frequency of the heartbeat, in $\text{Hz}$.
  2. b) Calculate its period, in seconds: how much time passes between two consecutive beats?
Solve
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The mains voltage in Ireland oscillates with a frequency of $50\ \text{Hz}$. Calculate its angular frequency $\omega = 2 \times \pi \times f$, in $\text{rad/s}$.

The mains voltage in Ireland oscillates with a frequency of $50\ \text{Hz}$. Calculate its angular frequency $\omega = 2 \times \pi \times f$, in $\text{rad/s}$.

Solve

Extension: the equation of motion x(t) = A·sin(ω·t+φ₀)

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The displacement of a mass oscillating on a horizontal spring is given, in SI units, by $x = 0.1 \times \sen(20 \times \pi \times t)$. a) What are the amplitude $A$ and…

The displacement of a mass oscillating on a horizontal spring is given, in SI units, by $x = 0.1 \times \sen(20 \times \pi \times t)$.

  1. a) What are the amplitude $A$ and the angular frequency $\omega$?
  2. b) Calculate the period $T$ and the frequency $f$ of the motion, remembering that $T = \frac{2 \times \pi}{\omega}$ and $f = \frac{1}{T}$.
Solve
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An oscillator describes simple harmonic motion with equation $x = 0.08 \times \sen(\pi \times t)$, in SI units. a) Calculate the displacement at the instant…

An oscillator describes simple harmonic motion with equation $x = 0.08 \times \sen(\pi \times t)$, in SI units.

  1. a) Calculate the displacement at the instant $t = 0.5\ \text{s}$.
  2. b) What is the maximum value that the displacement can take? At what times is it reached?
Solve
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Two identical oscillators vibrate according to the equations, in SI units, $x_1 = 0.05 \times \sen(3 \times \pi \times t)$ and…

Two identical oscillators vibrate according to the equations, in SI units, $x_1 = 0.05 \times \sen(3 \times \pi \times t)$ and $x_2 = 0.05 \times \sen(3 \times \pi \times t + \frac{\pi}{2})$.

  1. a) What quantities do the two motions have in common?
  2. b) Calculate the initial displacement (at $t = 0$) of each and explain how they differ.
Solve
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The piston rod of a combustion engine vibrates according to the equation $x = 0.04 \times \sen(10 \times \pi \times t + \frac{\pi}{2})$, in SI units. a) State the value…

The piston rod of a combustion engine vibrates according to the equation $x = 0.04 \times \sen(10 \times \pi \times t + \frac{\pi}{2})$, in SI units.

  1. a) State the value of the amplitude $A$, the angular frequency $\omega$ and the initial phase $\varphi_0$.
  2. b) Calculate the period $T$ and the frequency $f$.
  3. c) Calculate the displacement at $t = 0.1\ \text{s}$ and interpret its sign.
Solve
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The needle of a sewing machine moves up and down in simple harmonic motion with an amplitude of $6\ \text{cm}$ and a period of $0.5\ \text{s}$. At the initial instant,…

The needle of a sewing machine moves up and down in simple harmonic motion with an amplitude of $6\ \text{cm}$ and a period of $0.5\ \text{s}$. At the initial instant, the needle passes through the equilibrium position moving in the positive direction, so that $\varphi_0 = 0$.

  1. a) Calculate the angular frequency $\omega$.
  2. b) Write the complete equation of displacement, $x = A \times \sen(\omega \times t + \varphi_0)$, expressing the amplitude in metres.
Solve

Extension: velocity and acceleration, the derivatives of x(t)

Animation of the time graphs of displacement, velocity and acceleration of an SHM: a vertical cursor sweeps across all three curves at once, with a point on each. It shows that the velocity is maximum when x is 0 (phase difference of π/2 rad) and that the acceleration is maximum and opposite in sign to x at the extremes (phase difference of π rad). x(t) v(t) a(t)
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A point at the centre of a guitar string vibrates with simple harmonic motion of amplitude $A = 2\ \text{mm}$ and frequency $f = 440\ \text{Hz}$ (the concert pitch 'A').…

A point at the centre of a guitar string vibrates with simple harmonic motion of amplitude $A = 2\ \text{mm}$ and frequency $f = 440\ \text{Hz}$ (the concert pitch 'A'). The maximum velocity of an oscillator is $v_{max} = A \times \omega$.

  1. a) Calculate the angular frequency $\omega$ of the vibration.
  2. b) Express the amplitude in metres and calculate the maximum speed of the point on the string.
Solve
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On a frictionless air track, a trolley of $m = 0.25\ \text{kg}$ is attached to a spring of constant $k = 400\ \text{N/m}$. The trolley is pulled $10\ \text{cm}$ from the…

On a frictionless air track, a trolley of $m = 0.25\ \text{kg}$ is attached to a spring of constant $k = 400\ \text{N/m}$. The trolley is pulled $10\ \text{cm}$ from the equilibrium position and released from rest at instant $t = 0$. The setup is shown in the figure.

k = 400 N/m x = 0 m = 0.25 kg A = 0.1 m
  1. a) Calculate the angular frequency, $\omega = \sqrt{\frac{k}{m}}$, and the period of oscillation.
  2. b) Taking $x(t) = A\sin(\omega t + \varphi_0)$, explain why the initial phase is $\varphi_0 = \frac{\pi}{2}$: what is the value of the displacement at $t = 0$?
  3. c) Write the complete equation of displacement, in SI units.
  4. d) Calculate the maximum velocity of the trolley, $v_{max} = A \times \omega$.
Solve
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The recording needle of a seismograph oscillates according to the equation $x = 0.06 \times \sen(8 \times \pi \times t)$, in SI units. The velocity in simple harmonic…

The recording needle of a seismograph oscillates according to the equation $x = 0.06 \times \sen(8 \times \pi \times t)$, in SI units. The velocity in simple harmonic motion is $v = A \times \omega \times \cos(\omega \times t + \varphi_0)$. The graph of displacement against time is shown in the figure.

x (m) t (s) A = 0.06 m x = 0.03 m t = ?
  1. a) Calculate the first instant at which the displacement is $x = 0.03\ \text{m}$ (half the amplitude).
  2. b) Calculate the velocity of the needle at that instant.
  3. c) At what position is the velocity maximum and what is its value?
Solve

The dynamics of SHM: springs, pendulums and resonance

When you pull a body attached to a spring $2\ \text{cm}$ away, you feel a slight resistance towards the centre, but if you pull it $4\ \text{cm}$ the force tugging at your hand immediately doubles: how does this restoring force determine the exact time the system takes to complete each swing?

To verify Hooke's law in the lab, hang increasing loads from a spring and measure the extension $s$ for each one. The force is the weight of the load, $F=mg$. Plot $F$ against $s$: a straight line through the origin verifies Hooke's law, and the gradient is the spring constant $k$. Hooke's law only holds up to the elastic limit of the spring.

This restoring force is what produces SHM: applying Newton's second law ($F_{net}=ma$) to $F=-k\cdot x$ and to $a=-\omega^2\cdot x$, we find that the angular frequency of the mass–spring oscillator does not depend on the amplitude, only on $k$ and the mass $m$:

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The period of a mass-spring oscillator is $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$. In the laboratory, a $m = 0.25\ \text{kg}$ block oscillates attached to a spring…

The period of a mass-spring oscillator is $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$. In the laboratory, a $m = 0.25\ \text{kg}$ block oscillates attached to a spring of spring constant $k = 100\ \text{N/m}$. Calculate the period of the oscillation.

Solve
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The period of a simple pendulum is $T = 2 \times \pi \times \sqrt{\frac{l}{g}}$. A lamp in a museum entrance hall hangs from a cable $l = 1\ \text{m}$ long and…

The period of a simple pendulum is $T = 2 \times \pi \times \sqrt{\frac{l}{g}}$. A lamp in a museum entrance hall hangs from a cable $l = 1\ \text{m}$ long and oscillates slightly after a gust of wind (take $g = 9.8\ \text{m/s}^2$). Calculate its period of oscillation.

Solve

A vertical spring

When a mass hangs from a vertical spring, it stretches the spring by $x_0$ until the elastic force balances the weight: $k\cdot x_0 = m\cdot g$. This is the new equilibrium position. If you pull the mass a little from there, the net force is $-k\cdot x$ measured from that point, because the weight is cancelled by the constant part of the spring force. So the motion is SHM about the new equilibrium, with the same $T = 2\cdot\pi\cdot\sqrt{m/k}$ as for a horizontal spring.

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On the International Space Station, weighing scales cannot be used to measure the mass of astronauts. Instead, the astronaut sits on a seat attached to a spring of…

On the International Space Station, weighing scales cannot be used to measure the mass of astronauts. Instead, the astronaut sits on a seat attached to a spring of constant $k = 1000\ \text{N/m}$ and the period of oscillation of the system, $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$, is measured.

  1. a) If the measured period is $T = 1.6\ \text{s}$, rearrange the formula for mass and calculate the astronaut's mass (ignore that of the seat).
  2. b) Explain why this method works in weightlessness and weighing scales do not.
Solve
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In a workshop, a spring with spring constant $k = 250\ \text{N/m}$ is tested by attaching a mass of $0.4\ \text{kg}$ to it and making it oscillate. a) Calculate the…

In a workshop, a spring with spring constant $k = 250\ \text{N/m}$ is tested by attaching a mass of $0.4\ \text{kg}$ to it and making it oscillate.

  1. a) Calculate the period of oscillation, $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$.
  2. b) Calculate the frequency, in $\text{Hz}$.
Solve
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In the laboratory, two oscillators are set up using the same spring, with spring constant $k = 100\ \text{N/m}$: oscillator A has a mass of $0.1\ \text{kg}$ and…

In the laboratory, two oscillators are set up using the same spring, with spring constant $k = 100\ \text{N/m}$: oscillator A has a mass of $0.1\ \text{kg}$ and oscillator B has a mass of $0.4\ \text{kg}$. The figure shows both setups.

k = 100 N/m 0.1 kg oscillator A T = ? k = 100 N/m 0.4 kg oscillator B T = ?
  1. a) Calculate the period of each oscillator and their ratio $\frac{T_B}{T_A}$.
  2. b) Without repeating the calculations, use formula $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$ to reason the relationship between that ratio and the ratio of masses $\frac{m_B}{m_A}$.
  3. c) What spring constant should the spring of oscillator B have so that it oscillates with the same period as A? Justify your answer.
Solve
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A mass of $m = 0.5\ \text{kg}$ is suspended from a vertical spring of constant $k = 200\ \text{N/m}$ (take $g = 9.8\ \text{m/s}^2$). The setup is shown in the figure. a)…

A mass of $m = 0.5\ \text{kg}$ is suspended from a vertical spring of constant $k = 200\ \text{N/m}$ (take $g = 9.8\ \text{m/s}^2$). The setup is shown in the figure.

no mass 0.5 kg with mass at equilibrium natural length x₀ = ? oscillates
  1. a) Calculate how much the spring stretches to reach the equilibrium position, where the elastic force $k \times x_0$ equals the weight $m \times g$.
  2. b) The mass is pulled slightly from that position and released. Calculate the period of the vertical oscillation, $T = 2 \times \pi \times \sqrt{\frac{m}{k}}$.
  3. c) Explain why gravity does not modify the period compared to the same oscillator arranged horizontally: what is the only thing gravity changes in vertical oscillation?
Solve
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A suspension bridge has a natural frequency of oscillation of $0.5\ \text{Hz}$. The wind, passing around the pillars, generates vortices that push the bridge laterally…

A suspension bridge has a natural frequency of oscillation of $0.5\ \text{Hz}$. The wind, passing around the pillars, generates vortices that push the bridge laterally once every $2.0\ \text{s}$. The figure shows how the amplitude of the forced oscillation depends on the frequency of the pushes.

amplitude push frequency f f₀ = 0.5 Hz
  1. a) Calculate the natural period and natural angular frequency of the bridge.
  2. b) Calculate the frequency of the wind pushes and compare it with the natural frequency of the bridge.
  3. c) Explain what resonance is and why it is dangerous in this situation, even if each push is weak.
  4. d) Propose a design modification that avoids the problem and justify it by indicating which physical quantity changes.
Solve

Investigating a model: measuring g with a pendulum

In your Physics in Practice Investigation you may be asked to verify a model for $g$ using primary data. The pendulum model is $g=4\pi^2 l/T^2$, so $T^2=(4\pi^2/g)\,l$. To estimate $g$, set it up like this. Use small oscillations, measure the length $l$ from the point of suspension to the centre of the mass, and time ten complete oscillations to reduce the effect of reaction time. Keep the stand stable and the surroundings clear; share out and rotate the tasks of measuring, recording and cross-checking.

Check any non-zero intercept: it could indicate an error in the length or in the timing. Document the raw data, method, sources and limitations, and state whether you used a simulation instead of an experiment.

In the Leaving Certificate, organise each calculation like this: diagram and data in SI units; model and conditions; law used; algebraic working; substitution with units; rounded result and a check that the answer is reasonable. The SEC marking schemes reward the steps shown, so never give just a number.

The diagram links the main ideas:

Three stages for estimating g with a pendulum: set-up with length L, small angle and timing of ten periods; T² against L line with its gradient b; result g ≈ 9.75 m s⁻² compared with the accepted value. Model and data small θ l 10 oscillations T² = (4π²/g) l Calculation and units T² (s²) l (m) b b = 4.05 s² m⁻¹ g = 4π²/b Critical conclusion g ≈ 9.75 m s⁻² 9.50 9.75 10.00 g (m s⁻²) Compare with the accepted value, 9.8 m s⁻²

Back to the start: the swing is SHM only for small swings, with a period set by its length and $g$, not by who is sitting on it.

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An antique grandfather clock works with a pendulum whose period must be exactly $T = 2.0\ \text{s}$: each complete oscillation advances a tooth of the mechanism (take…

An antique grandfather clock works with a pendulum whose period must be exactly $T = 2.0\ \text{s}$: each complete oscillation advances a tooth of the mechanism (take $g = 9.8\ \text{m/s}^2$). The pendulum is shown in the figure.

l = ? T = 2.0 s
  1. a) Rearrange formula $T = 2 \times \pi \times \sqrt{\frac{l}{g}}$ for length.
  2. b) Calculate the required length of the pendulum.
Solve
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A pendulum of length $l = 1.5\ \text{m}$ is part of an experiment that will be installed on a lunar base. Gravity on the surface of the Moon is $g_L = 1.6\ \text{m/s}^2$…

A pendulum of length $l = 1.5\ \text{m}$ is part of an experiment that will be installed on a lunar base. Gravity on the surface of the Moon is $g_L = 1.6\ \text{m/s}^2$ and on Earth $g_T = 9.8\ \text{m/s}^2$.

  1. a) Calculate the period of the pendulum on Earth.
  2. b) Calculate the period on the Moon.
  3. c) How many times slower does it oscillate on the Moon? Calculate the ratio of both periods.
Solve
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A wave energy converter buoy oscillates vertically with the waves according to the equation $x = 0.1 \times \sen(2 \times \pi \times t)$, in SI units. a) Calculate the…

A wave energy converter buoy oscillates vertically with the waves according to the equation $x = 0.1 \times \sen(2 \times \pi \times t)$, in SI units.

  1. a) Calculate the period and frequency of the oscillation.
  2. b) Calculate the displacement at instant $t = \frac{1}{12}\ \text{s}$.
  3. c) At what instant does it reach its maximum height for the first time?
Solve
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The Foucault pendulum installed in the Panthéon in Paris has a length of $l = 67\ \text{m}$ (take $g = 9.8\ \text{m/s}^2$). a) Calculate its period of oscillation. b)…

The Foucault pendulum installed in the Panthéon in Paris has a length of $l = 67\ \text{m}$ (take $g = 9.8\ \text{m/s}^2$).

  1. a) Calculate its period of oscillation.
  2. b) Calculate how many complete oscillations it performs in one hour.
  3. c) Foucault used a sphere of $28\ \text{kg}$. Justify, using the period formula, why the mass of the sphere does not affect the measurement and why it is advantageous to make the pendulum as long as possible to observe the phenomenon easily.
Solve
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A pendulum with a period of $T = 2.00\ \text{s}$ is to be designed for an experiment operating on the surface of Mars, where $g_M = 3.71\ \text{m/s}^2$. a) Calculate the…

A pendulum with a period of $T = 2.00\ \text{s}$ is to be designed for an experiment operating on the surface of Mars, where $g_M = 3.71\ \text{m/s}^2$.

  1. a) Calculate the required length of the pendulum on Mars.
  2. b) If that same pendulum were brought back to Earth ($g_T = 9.8\ \text{m/s}^2$), what would its period be?
  3. c) Geologists use precision pendulums to measure $g$ at different points on Earth and detect subsurface anomalies. Explain, using the formula, why the period of a pendulum reveals the value of $g$ and which quantities need to be measured most carefully.
Solve
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A group of students measures gravity using a pendulum. The measured length is $l = 1.20\ \text{m}$ and they time $20$ complete oscillations in $44.0\ \text{s}$. a)…

A group of students measures gravity using a pendulum. The measured length is $l = 1.20\ \text{m}$ and they time $20$ complete oscillations in $44.0\ \text{s}$.

  1. a) Calculate the period of the pendulum.
  2. b) Rearrange formula $T = 2 \times \pi \times \sqrt{\frac{l}{g}}$ for $g$ and calculate its experimental value.
  3. c) Compare with the accepted value $g = 9.81\ \text{m/s}^2$ and explain why $20$ oscillations are timed rather than a single one to find the period.
Solve

Summary

See all the exercises in this section