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Propagation of acoustic waves and shock waves radiated by a sinusoidal pulsation of a sphere during a single period
Institution:1. Istituto Nazionale di Geofisica e Vulcanologia, Sezione di Catania – Osservatorio Etneo, Piazza Roma 2, 95125 Catania, Italy;2. Università Roma Tre, Dipartimento di Ingegneria, via Vito Volterra 62, 00146 Roma;1. Dipartimento di Scienze della Terra, Università degli Studi di Firenze, via Giorgio La Pira, 4, 50121, Firenze, Italy;2. Item s.r.l., Firenze, Italy;3. Istituto Nazionale di Ottica – Consiglio Nazionale delle Ricerche (INO-CNR), Largo E. Fermi, 6, 50125 Firenze, Italy;4. Osservatorio Vesuviano, INGV, via Diocleziano, 328, 80124 Napoli, Italy;5. Dipartimento di Scienze della Terra, Univerità di Pisa, Pisa, Italy;6. Département des Sciences de la Terre, Université de Genève, CH-1205 Genève, Switzerland;7. Max Planck Institute for Dynamics and Self-Organization, 37077 Goettingen, Germany;8. Université Clermont Auvergne, CNRS, IRD, OPGC, Laboratoire Magmas et Volcans, F-63000 Clermont-Ferrand, France;9. Department of Earth and Environmental Sciences, Ludwig-Maximilians-Universität, München, Germany;10. Earth Sciences, University of Iceland, 102 Reykjavík, Iceland
Abstract:A spherical sound wave is emitted by a sphere which executes a small sinusoidal pulsation of a single period at high frequency in an inviscid fluid. Nonlinear propagation of the waves is formulated as an initial boundary value problem and is analysed in detail. The governing equation is linear near the sphere, while it is a nonlinear hyperbolic equation in a far field. The nonlinearity has a significant effect there, leading to the formation of two shocks. The exact solution to match the near field solution can easily be obtained for the far field equation. The nonlinear distortion of waveform and the shock formation distance are evaluated from the representation of the solution with strained coordinates. The evolution and nonlinear attenuation of the two shock discontinuities are also examined by making use of the equal-areas rule. In its asymptotic form the entire profile is an N wave with a long tail.
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