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Linear and nonlinear waves

Graham W. Griffiths, +1 more
- 09 Jul 2009 - 
- Vol. 4, Iss: 7, pp 4308
TLDR
The study of waves can be traced back to antiquity where philosophers, such as Pythagoras, studied the relation of pitch and length of string in musical instruments and the subject of classical acoustics was laid down and presented as a coherent whole by John William Strutt in his treatise Theory of Sound.
Abstract
The study of waves can be traced back to antiquity where philosophers, such as Pythagoras (c.560-480 BC), studied the relation of pitch and length of string in musical instruments. However, it was not until the work of Giovani Benedetti (1530-90), Isaac Beeckman (1588-1637) and Galileo (1564-1642) that the relationship between pitch and frequency was discovered. This started the science of acoustics, a term coined by Joseph Sauveur (1653-1716) who showed that strings can vibrate simultaneously at a fundamental frequency and at integral multiples that he called harmonics. Isaac Newton (1642-1727) was the first to calculate the speed of sound in his Principia. However, he assumed isothermal conditions so his value was too low compared with measured values. This discrepancy was resolved by Laplace (1749-1827) when he included adiabatic heating and cooling effects. The first analytical solution for a vibrating string was given by Brook Taylor (1685-1731). After this, advances were made by Daniel Bernoulli (1700-82), Leonard Euler (1707-83) and Jean d’Alembert (1717-83) who found the first solution to the linear wave equation, see section (3.2). Whilst others had shown that a wave can be represented as a sum of simple harmonic oscillations, it was Joseph Fourier (1768-1830) who conjectured that arbitrary functions can be represented by the superposition of an infinite sum of sines and cosines now known as the Fourier series. However, whilst his conjecture was controversial and not widely accepted at the time, Dirichlet subsequently provided a proof, in 1828, that all functions satisfying Dirichlet’s conditions (i.e. non-pathological piecewise continuous) could be represented by a convergent Fourier series. Finally, the subject of classical acoustics was laid down and presented as a coherent whole by John William Strutt (Lord Rayleigh, 1832-1901) in his treatise Theory of Sound. The science of modern acoustics has now moved into such diverse areas as sonar, auditoria, electronic amplifiers, etc.

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Linear and nonlinear waves, by G. B. Whitham. Pp.636. £50. 1999. ISBN 0 471 35942 4 (Wiley).

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References
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Journal ArticleDOI

Hodograph transformations of linearizable partial differential equations

TL;DR: In this article, an algorithmic method is developed for transforming quasilinear partial differential equations of the form $u_t = g( u )u-nx + f( u, u_x, \cdots,u_{( n - 1)x } ),\, u_{mx} \equiv \partial ^m u/\partial x^m $, where dg/du ot\equiv 0, where $dg/d is not\equivaliv 0.
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Computational Mathematics in Engineering and Applied Science: ODEs, DAEs, and PDEs

TL;DR: The General Problem in Ordinary and Partial Differential Equations The Numerical Integration of Initial Value Ordinary DDE/DAE/PDE Applications as discussed by the authors The general problem in ODE and PDE applications.
Journal ArticleDOI

Linear and Nonlinear Waves

K J Whiteman
- 01 Nov 1975 - 
TL;DR: Whitham's book as mentioned in this paper is a comprehensive account of the mathematics of wave motion written with great knowledge and enthusiasm and contains material that one would expect in such a text; a discussion of characteristics and the formation of shocks; application to water waves and gas dynamics; group velocity, dispersion and wave patterns; the classical nonlinear results.
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Why are solitons stable

TL;DR: The theory of linear dispersive equations predicts that waves should spread out and disperse over time, but it is observed both in theory and practice that once nonlinear effects are taken into account, solitary wave or soliton solutions can be created, which can be stable enough to persist indefinitely as discussed by the authors.