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Introduction to Waves

Why this chapter
Why this chapter exists

Ripples on a pond, a pulse on a rope, the sound of a voice and the light of the Sun are all waves. Each one carries energy from one place to another, yet no material makes the journey. This chapter says exactly what a wave is and sorts waves into their kinds. It then builds the mathematics of a wave on a string, one step at a time. A single function of \(x - vt\) describes any pulse, and a single equation, the wave equation, governs every travelling wave. The chapter ends with the harmonic wave, \(y = A\sin(kx - \omega t)\), the building block of all the waves in this unit.

You will learn
By the end of this chapter you will
  1. Say what a wave carries and what it does not, and why a rope is the simplest wave to study.
  2. Sort waves into mechanical and non-mechanical, and into transverse and longitudinal, with examples of each.
  3. Write a travelling pulse as \(y = f(x - vt)\) or \(g(x + vt)\), and read its speed and direction from the function.
  4. Derive the particle velocity \(-v \times \text{slope}\) and the wave equation, and test a function against the conditions for a valid wave.
  5. Derive \(y = A\sin(kx - \omega t)\) and show that each particle performs SHM with \(\lambda = vT\).
  6. Find every quantity of a harmonic wave from its equation.
Before you begin
Before you begin

From Motion in One Dimension you should know velocity as a derivative and a slope. From the chapter Kinematics of SHM you should know simple harmonic motion, \(x = A\sin(\omega t + \phi)\). Its amplitude, period, frequency, angular frequency and phase should be familiar. You should be able to differentiate a sine and use the chain rule.

Already know this?

Lessons

1
What a Wave Carries
Ripples on a pond, a wave of fans in a stadium and a pulse on a rope are one phenomenon. A wave carries energy and momentum from place to place, while the medium only oscillates. Why the rope is the model for this chapter.
A wave is a travelling disturbanceA wave carries energy and momentum not matterThe rope is the model for this chapter
13 min0%
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2
Kinds of Waves
Waves sorted two ways. By the need for a medium, into mechanical and non-mechanical waves. By the direction in which the particles of the medium move, into transverse and longitudinal waves.
Mechanical waves need a mediumTransverse and longitudinal waves
13 min0%
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3
The Travelling-Wave Function
A pulse on a string described by a function. The shape at \(t = 0\) is \(y = f(x)\); after a time \(t\) the whole shape has moved by \(vt\), so \(y = f(x - vt)\). A wave travelling the other way is \(g(x + vt)\).
The shape of a pulse is a function of xA pulse moving right is f of x minus vt
14 min0%
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4
The Wave Equation
Differentiating \(y = f(x - vt)\). The velocity of a particle is minus the wave speed times the slope of the string. The second derivatives give the wave equation. The four conditions for a valid wave function, tested on three functions.
Particle velocity is minus wave speed times slopeThe wave equationConditions for a valid wave function
15 min0%
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5
Harmonic Waves
The sine wave, the building block of every wave. Its snapshot \(y = A\sin(2\pi x/\lambda)\), the particle at \(x = 0\) in simple harmonic motion, \(\lambda = vT\), and the harmonic wave \(y = A\sin(kx - \omega t)\) with its eight named quantities.
Harmonic waves are the building blocksThe snapshot of a harmonic waveEach particle of a harmonic wave performs shmThe harmonic wave y equals a sin kx minus omega t
16 min0%
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Read in order. The small labels are the topics of each lesson. They take your colour as you answer the checks.

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The Workbook
Questions to solve on paper, marked by you.
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Glossary

The key words of this chapter, with the meaning this chapter gives them.

amplitude
The maximum displacement of a particle of the medium from its equilibrium position, \(A\).
angular frequency
\(\omega = 2\pi/T\), the rate of change of the phase of a wave with time, in rad/s.
compression
A region of a longitudinal wave where the particles of the medium are crowded closer together than at rest.
crest
A point of greatest positive displacement of a wave at one instant, a highest point of the wave.
Fourier series
A way of writing any periodic function as a sum of sines and cosines, so any periodic wave as a sum of harmonic waves.
harmonic wave
A travelling wave whose displacement is a sine function of position and time, \(y = A\sin(kx - \omega t)\). Every particle of the medium performs simple harmonic motion.
longitudinal wave
A wave in which the particles of the medium oscillate parallel to the direction in which the wave travels, as in sound in air.
mechanical wave
A wave that needs a material medium to travel. Sound, water waves, seismic waves and waves on a string are mechanical waves.
medium
The material through which a mechanical wave travels, such as air, water, a rope or the rock of the Earth. Each part of the medium only oscillates about its own place.
non-mechanical wave
A wave that needs no medium and can travel through a vacuum at the speed of light. Electromagnetic waves and gravitational waves are non-mechanical.
partial derivative
The derivative of a function of two or more variables with respect to one of them, the others held fixed. It is written with a curly \(\partial\), as in \(\partial y/\partial t\).
partial differential equation
An equation that relates partial derivatives of an unknown function of two or more variables. The wave equation is one.
phase
The argument of the sine in the equation of a harmonic wave, \(\Phi = kx - \omega t\). It fixes where in its cycle each particle is.
pulse
A single disturbance, such as one bump, that travels along a medium.
rarefaction
A region of a longitudinal wave where the particles of the medium are spread farther apart than at rest.
transverse wave
A wave in which the particles of the medium oscillate perpendicular to the direction in which the wave travels, as on a rope.
trough
A point of greatest negative displacement of a wave at one instant, a lowest point of the wave.
wave function
The function \(y(x, t)\) that gives the displacement of the medium at every position \(x\) and every time \(t\).
wave number
\(k = 2\pi/\lambda\), the rate of change of the phase of a wave with position, in rad/m.
wavelength
The distance between two consecutive crests, or troughs, of a wave at a fixed time, \(\lambda\). The spatial period of the wave.