Abstract
In the context of transient dynamic problems the symbol \( \left( {x,\hat x \in \mathbb{R}^3 } \right) \) is used to denote a spatial and temporal Fourier transformed quantity, i.e. we define in analogy to (4.1):
t, x k , k = 1, 2, 3 are the time and the spatial coordinates. The corresponding differentiations are denoted by ∂ t , ∂ k .
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© 2002 Springer-Verlag Berlin Heidelberg
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Rayleigh, L. (2002). Waves. In: Fourier BEM. Lecture Notes in Applied Mechanics, vol 5. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-45626-1_8
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DOI: https://doi.org/10.1007/978-3-540-45626-1_8
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-07727-2
Online ISBN: 978-3-540-45626-1
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