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<record version="4" id="258">
 <title>wave equation</title>
 <name>WaveEquation</name>
 <created>2007-08-10 13:53:15</created>
 <modified>2008-10-14 14:47:01</modified>
 <type>Definition</type>
 <creator id="1" name="bloftin"/>
 <modifier id="441" name="bci1"/>
 <comment>physical perturbation' or `signal'</comment>
 <author id="441" name="bci1"/>
 <author id="1" name="bloftin"/>
 <classification>
	<category scheme="msc" code="02.30.Jr"/>
 </classification>
 <related>
	<object name="WaveEquations"/>
	<object name="QuantumHamiltonianOperator"/>
 </related>
 <keywords>
	<term>types of wave equations</term>
 </keywords>
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 <content>Any \emph{wave equation} describes the propagation in space-time of a wave (or periodic motion, oscillation, `physical pereturbation' or 'signal') in terms of certain types of differential equations (such as partial differential ones); the solutions of such wave equations--usually with additonal boundary conditions-- are either propagating or stationary waves; there are numerous types of waves, and thus, there are many different types of wave equations.
The following is a short list of such wave equations, that is however not intended to be comprehensive.

\subsection{Types of Wave Equations}

\begin{enumerate}

\item Elastic wave equation and Hook's Law

\item Equation for sound wave propagation

\item Wave equation for heat transfer;

\item Laplace wave equation;

\item Maxwell's equations for electromagnetic wave propagation;

\item Schr\"odinger 'wave' equation for electrons (see also \PMlinkname{Hamiltonian operator}{QuantumHamiltonianOperator});

\item Heisenberg's quantum dynamic equations (see also \PMlinkname{Hamiltonian operator}{QuantumHamiltonianOperator} and \PMlinkname{quantum harmonic oscillator and Lie algebra}{QuantumHarmonicOscillatorAndLieAlgebra});

\item Dirac relativistic wave equation;

\item Soliton wave equations;

\item Spin wave equations;

\item Einstein's gravitational wave equations;

\end{enumerate}

\subsection{Examples:}

In its simplest form, the wave equation refers to a scalar function $w$ that satisfies:

$ \partial^2 (w) \over {\partial t^2}$  = $c^2 \nabla^2 u,$

where $ \nabla^2$ is the Laplace operator, and where $c$ is a fixed constant equal to the propagation speed of the wave.</content>
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