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This work addresses the problem of the struck piano string. This system is highly nonlinear, and a sound representation of the energy balance is therefore necessary in any time stepping routine used in simulation, in order to preserve stability. Many
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=od______4094::ad318a012adb8d8b3e845669284f1bf6
https://hdl.handle.net/11585/883682
https://hdl.handle.net/11585/883682
Publikováno v:
Acta Mechanica
Acta Mechanica, Springer Verlag, 2014, 225 (1), pp.213-232. ⟨10.1007/s00707-013-0931-1⟩
Acta Mechanica, Springer Verlag, 2014, 225 (1), pp.213-232. ⟨10.1007/s00707-013-0931-1⟩
Nonlinear vibrations of thin rectangular plates are considered, using the von kármán equations in order to take into account the effect of geometric nonlinearities. Solutions are derived through an expansion over the linear eigenmodes of the system
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::922764e5b58b715543f5170b0443d41e
http://hdl.handle.net/11585/836441
http://hdl.handle.net/11585/836441
Autor:
Craig J. Webb, Stefan Bilbao
Publikováno v:
ICASSP
In seeking to model realistic room acoustics, direct numerical simulation can be employed. This paper presents 3D Finite Difference Time Domain schemes that incorporate losses at boundaries and due to the viscosity of air. These models operate within
Autor:
Craig J. Webb, Alan Gray
Publikováno v:
The Journal of the Acoustical Society of America. 133:3613-3613
The computation of large-scale virtual acoustics using the 3D finite difference time domain (FDTD) is prohibitively computationally expensive, especially at high audio sample rates, when using traditional CPUs. In recent years the computer gaming ind
Publikováno v:
The Journal of the Acoustical Society of America. 133:3490-3490
Binaural room impulse responses are important for auralisation as well as for objective research in room acoustics. In geometrical room simulation methods, obtaining such responses is easily achieved by convolving each computed reflection tap with a