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The Wave Equation and its Connections with the Laplace and Heat Equations

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Part of the book series: Graduate Texts in Mathematics ((GTM,volume 214))

Abstract

The wave equation is the PDE

$$ \frac{{\partial ^2 }} {{\partial t^2 }}u(x,t) - \Delta u(x,t) = 0 for x \in \Omega \subset \mathbb{R}^d , t \in (0,\infty ) or t \in \mathbb{R}. $$
((6.1.1))

As with the heat equation, we consider t as time and x as a spatial variable. For illustration, we first consider the case where the spatial variable x is one-dimensional. We then write the wave equation as

$$ u_{tt} (x,t) - u_{xx} (x,t) = 0. $$
((6.1.2))

Let ϕ, ψC2(ℝ). Then

$$ u(x,t) = \phi (x + t) + \psi (x - t) $$
((6.1.3))

obviously solves (6.1.2).

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© 2007 Springer Science+Business Media, LLC

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(2007). The Wave Equation and its Connections with the Laplace and Heat Equations. In: Partial Differential Equations. Graduate Texts in Mathematics, vol 214. Springer, New York, NY. https://doi.org/10.1007/978-0-387-49319-0_7

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