1991
DOI: 10.2307/3619030
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Wave theory and applications, by D. R. Bland. Pp 317. £15 (paperback), £40 (hardback). 1988. ISBN 0-19-859669-3, -859654-5 (Oxford University Press)

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Cited by 14 publications
(21 citation statements)
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“…This was also shown by Doetsch 2 and by Bland. 3 Thus Eq. ͑4.2͒ admits, at most, only one form of dispersion.…”
Section: ͑43͒mentioning
confidence: 98%
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“…This was also shown by Doetsch 2 and by Bland. 3 Thus Eq. ͑4.2͒ admits, at most, only one form of dispersion.…”
Section: ͑43͒mentioning
confidence: 98%
“…Observe from Tables I and II that in every case the magnitude of the discontinuity is independent of k. Furthermore, in the case of rectangular pulse signal, we see that S ͓u͔ at and Ϫp gives the signal strength of the pulse at the leading and trailing edges, respectively, without having to solve for the time-domain solution of the problem. Finally note that, with the exception of F()ϭ␦(), all the boundary data considered resulted in strong discontinuities 3 in u. For the telegraph equation, which is of second order, strong discontinuities are jump discontinuities which occur in u, or u x and u .…”
Section: ͑55͒mentioning
confidence: 99%
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“…The solution for v A L in Eq. (46) at low frequency can be obtained by the perturbation method (Bland, 1988;Mal and Singh, 1991) …”
Section: Lamb Wavesmentioning
confidence: 99%