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Part of the book series: Mathematische Leitfäden ((MLF))

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Abstract

According to (1.24), the wave equation in R 1 is of the form

$$ {u_{xx}} - \frac{1} {{{\gamma |2}}}{u_{tt}} = 0,\quad where\quad \gamma = const > 0 $$
(2.1)

The symbol x denotes a real variable here. Introduction of a new time scale t̃ = γt shows that we may restrict ourselves to the case γ = 1. Therefore we base (2.1) on the form

$$ {u_{xx}} - {u_{tt}} = 0,\quad or\quad {u_{\bar x\bar t}} = 0 $$
(2.2)

where the last equation results from the transformation x = x + t, t̄ = x - t. By integration we find all solutions of (2.2):

$$ u\left( {x,t} \right) = {w_1}\left( {\bar x} \right) + {w_2}\left( {\bar t} \right) = {w_1}\left( {x + t} \right) + {w_2}\left( {x - t} \right) $$
((2.3))

where the w i ε C 2(i = 1, 2) are arbitrary functions.

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© 1964 Springer Fachmedien Wiesbaden

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Hellwig, G. (1964). The Wave Equation. In: Partial Differential Equations. Mathematische Leitfäden. Vieweg+Teubner Verlag, Wiesbaden. https://doi.org/10.1007/978-3-663-11002-6_2

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  • DOI: https://doi.org/10.1007/978-3-663-11002-6_2

  • Publisher Name: Vieweg+Teubner Verlag, Wiesbaden

  • Print ISBN: 978-3-519-12213-5

  • Online ISBN: 978-3-663-11002-6

  • eBook Packages: Springer Book Archive

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