Loading [MathJax]/jax/output/HTML-CSS/jax.js
Skip to main content
Library homepage
 

Text Color

Text Size

 

Margin Size

 

Font Type

Enable Dyslexic Font
Physics LibreTexts

14.8: Summary

( \newcommand{\kernel}{\mathrm{null}\,}\)

Key Takeaways

A traveling wave is the propagation of a disturbance with a speed, v, through a medium. Particles in the medium oscillate back and forth, about an equilibrium position, as a wave passes through the medium, but they are not carried with the wave. Only energy is transmitted by a wave.

In a transverse wave, the particles in the medium oscillate in a direction that is perpendicular to the velocity of the wave. In a longitudinal wave, the particles of the medium oscillate in a direction that is co-linear with the velocity of the wave.

A sine wave is described by it frequency, f, its wavelength, λ, its amplitude, A, and its speed, v. We can also use the period of the wave, T, in lieu of the frequency. The frequency and wavelength of a wave are related to each other by the speed of the wave:

v=λf

Mathematically, a one-dimensional traveling sine wave moving in the positive x direction can be described by:

D(x,t)=Asin(kxωt+ϕ)

where D(x,t) is the displacement of the particle in the medium at position x at time t. ϕ is the phase of the wave and depends on our choice of when t=0. k is the wave number of the wave, and ω its angular frequency. These are related to the wavelength and frequency, respectively:

k=2πλω=2πf=2πT

If a dynamical model (e.g. Newton’s Second Law) of a system/medium leads to an equation with the following form:

2Dx2=1v22Dt2

then waves with a speed of v can propagate through the system/medium.

The speed of a wave on a rope of linear mass density, μ, under a tension, FT, is given by:

v=FTμ

Generally, the speed of a wave in a medium depends on the elasticity of the medium when it is deformed and the inertia of the particles in the medium. In order for a wave to propagate through a medium, the particles in the medium must be able to be displaced from their equilibrium position.

A pulse traveling through a rope will get reflected at the end of the rope and travel back in the opposite direction. If the end of the rope is fixed, the reflected pulse will be inverted. If the end of the rope can move, the reflected pulse will be in the same orientation as the incoming pulse.

A one-dimensional wave in a rope of linear mass density, μ, will transfer energy at an average rate:

P=12ω2μA2v

A three dimensional spherical wave through a medium with density ρ will transfer energy at an average rate:

P=2πρω2r2v

at a distance r from the source of the wave. The amplitude of a spherical wave will decrease as the distance away from the source increases:

A=1rP2πρω2v

The intensity of a spherical wave is defined as the power per unit area transferred by the wave, and is given by:

I=P4πr2=12ρω2A2v

The superposition principle states that if D1(x,t), D2(x,t), , are functions that satisfy the wave equation, then any linear combination of these functions, D(x,t):

D(x,t)=a1D1(x,t)+a2D2(x,t)+a3D3(x,t)+

will also satisfy the wave equation.

Different waves can interfere constructively or destructively in a medium, and the resulting wave is given by the sum of the functions describing the interfering waves.

Standing waves are formed when waves of the same frequency and amplitude traveling in opposite directions interfere. For standing waves on a string, the displacement of a particle on the string is given by:

D(x,t)=2Asin(nπLx)cos(ωt)

where n is the number of the harmonic and L is the length of the string. In particular, a particle at position x will move up and down as a simple harmonic oscillator with amplitude:

A(x)=2Asin(nπLx)

The condition for a standing wave to exist on a string is that the length of the string must be equal to a multiple of half of the wavelength of the standing wave:

L=nλ2n=1,2,3,λ=2Lnf=nv2L

Important Equations

Traveling 1d waves:

D(x,t)=Asin(kxωt+ϕ)k=2πλω=2πf=2πTv=λf

Wave equation:

2Dx2=1v22Dt2

Wave velocity:

v=FTμv=Eρv=Bρ

Power (1d wave in a rope):

P=12ω2μA2v

Spherical waves:

P=2πρω2r2vA=1rP2πρω2vI=P4πr2=12ρω2A2v

Standing waves:

D(x,t)=2Asin(nπLx)cos(ωt)A(x)=2Asin(nπLx)

Standing waves on a string (both ends fixed):

L=nλ2n=1,2,3,λ=2Lnf=nv2L

Important Definitions

Definition

Wavelength: The distance between two successive maxima ("peaks") or minima (troughs) in a wave. SI units: [m]. Common variable(s): λ.

Definition

Amplitude: The maximal distance that a particle in a medium is displaced from its equilibrium position when a wave passes by. SI units: [m]. Common variable(s): A.

Definition

Frequency: The number of complete oscillations in one second of a particle in a medium as a wave passes by. SI units: [s1]. Common variable(s): f.

Definition

Bulk modulus: A measurement of an object or substance’s resistance to compression. SI units: [Pa]. Common variable(s): B.

Definition

Volume mass density: The mass per unit volume of an object. SI units: [kgm3]. Common variable(s): ρ.

Definition

Intensity: The power per unit area transmitted by a wave. SI units: [Wm2]. Common variable(s): I.


This page titled 14.8: Summary is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Ryan D. Martin, Emma Neary, Joshua Rinaldo, and Olivia Woodman via source content that was edited to the style and standards of the LibreTexts platform.

Support Center

How can we help?