2013
DOI: 10.1016/j.jsv.2013.08.030
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Commentary on Discussion of ‘On the theory of standing waves in tyres at high vehicle speeds’ by V.V. Krylov and O. Gilbert, Journal of Sound and Vibration 329 (2010) 4398–4408

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Cited by 4 publications
(3 citation statements)
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“…Huang and Maradudin get the conclusion that surface roughness leads to the attenuation of surface acoustic wave in two polarization directions through studying on the acoustic surface wave propagation over the inserted groove [5]. V. V. Krylov and Z. A. Smimova measure the relative change of velocity surface acoustic wave on rough surface in the two dimensional and three dimensional and the results can match well with the theoretical results [6]. In this paper the effect of dispersion curves of the wave from rough surface are investigated using the finite element method based on surface acoustic wave dispersion theory.…”
Section: Introductionmentioning
confidence: 55%
“…Huang and Maradudin get the conclusion that surface roughness leads to the attenuation of surface acoustic wave in two polarization directions through studying on the acoustic surface wave propagation over the inserted groove [5]. V. V. Krylov and Z. A. Smimova measure the relative change of velocity surface acoustic wave on rough surface in the two dimensional and three dimensional and the results can match well with the theoretical results [6]. In this paper the effect of dispersion curves of the wave from rough surface are investigated using the finite element method based on surface acoustic wave dispersion theory.…”
Section: Introductionmentioning
confidence: 55%
“…Berthet et al (2003) noted this for the case close to case PWPV, yet with the vorticity localised within a region long compared with the acoustic wavelength. The cause is the analogy between the representation (3.6) and two-dimensional Kirchhoff's diffraction formula (see Schot (1992) and Krylov (1989), S 3), both of which are based on the Helmholtz equation (3.1), though a source is distributed for scattering by a flow and localised on a one-dimensional surface for diffraction by an aperture. On the forward direction, where the diffraction pattern is typically of interest, the far field can be identified with the Fraunhofer region, while the near field with the Fresnel region.…”
Section: Leading-order Solution Asmentioning
confidence: 99%
“…However, the linearisation procedure adopted in [28] is discussable. Recent contributions to the discussion on the existence of resonance speeds can be found in [29][30][31].…”
Section: Introductionmentioning
confidence: 99%