Free and forced vibrations of a tyre using a wave/finite element approach
Free and forced vibrations of a tyre using a wave/finite element approach
Free and forced vibrations of a tyre are predicted using a wave/finite element (WFE) approach. A short circumferential segment of the tyre is modelled using conventional finite element (FE) methods, a periodicity condition applied and the mass and stiffness matrices post-processed to yield wave properties. Since conventional FE methods are used, commercial FE packages and existing element libraries can be utilised. An eigenvalue problem is formulated in terms of the transfer matrix of the segment. Zhong's method is used to improve numerical conditioning. The eigenvalues and eigenvectors give the wavenumbers and wave mode shapes, which in turn define transformations between the physical and wave domains. A method is described by which the frequency dependent material properties of the rubber components of the tyre can be included without the need to remesh the structure. Expressions for the forced response are developed which are numerically well-conditioned. Numerical results for a smooth tyre are presented. Dispersion curves for real, imaginary and complex wavenumbers are shown. The propagating waves are associated with various forms of motion of the tread supported by the stiffness of the side wall. Various dispersion phenomena are observed, including curve veering, non-zero cut-off and waves for which the phase velocity and the group velocity have opposite signs. Results for the forced response are compared with experimental measurements and good agreement is seen. The forced response is numerically determined for both finite area and point excitations. It is seen that the size of area of the excitation is particularly important at high frequencies. When the size of the excitation area is small enough compared to the tread thickness, the response at high frequencies becomes stiffness-like (reactive) and the effect of shear stiffness becomes important
737-756
Waki, Y.
555aaeaa-459e-4af1-8fd6-615c4a583c90
Mace, B.R.
cfb883c3-2211-4f3a-b7f3-d5beb9baaefe
Brennan, M.J.
87c7bca3-a9e5-46aa-9153-34c712355a13
19 June 2009
Waki, Y.
555aaeaa-459e-4af1-8fd6-615c4a583c90
Mace, B.R.
cfb883c3-2211-4f3a-b7f3-d5beb9baaefe
Brennan, M.J.
87c7bca3-a9e5-46aa-9153-34c712355a13
Waki, Y., Mace, B.R. and Brennan, M.J.
(2009)
Free and forced vibrations of a tyre using a wave/finite element approach.
Journal of Sound and Vibration, 323 (3-5), .
(doi:10.1016/j.jsv.2009.01.006).
Abstract
Free and forced vibrations of a tyre are predicted using a wave/finite element (WFE) approach. A short circumferential segment of the tyre is modelled using conventional finite element (FE) methods, a periodicity condition applied and the mass and stiffness matrices post-processed to yield wave properties. Since conventional FE methods are used, commercial FE packages and existing element libraries can be utilised. An eigenvalue problem is formulated in terms of the transfer matrix of the segment. Zhong's method is used to improve numerical conditioning. The eigenvalues and eigenvectors give the wavenumbers and wave mode shapes, which in turn define transformations between the physical and wave domains. A method is described by which the frequency dependent material properties of the rubber components of the tyre can be included without the need to remesh the structure. Expressions for the forced response are developed which are numerically well-conditioned. Numerical results for a smooth tyre are presented. Dispersion curves for real, imaginary and complex wavenumbers are shown. The propagating waves are associated with various forms of motion of the tread supported by the stiffness of the side wall. Various dispersion phenomena are observed, including curve veering, non-zero cut-off and waves for which the phase velocity and the group velocity have opposite signs. Results for the forced response are compared with experimental measurements and good agreement is seen. The forced response is numerically determined for both finite area and point excitations. It is seen that the size of area of the excitation is particularly important at high frequencies. When the size of the excitation area is small enough compared to the tread thickness, the response at high frequencies becomes stiffness-like (reactive) and the effect of shear stiffness becomes important
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Published date: 19 June 2009
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Local EPrints ID: 79098
URI: http://eprints.soton.ac.uk/id/eprint/79098
ISSN: 0022-460X
PURE UUID: 04ed3320-598f-4bf4-bb2c-50961daf0f29
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Date deposited: 12 Mar 2010
Last modified: 14 Mar 2024 00:28
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Author:
Y. Waki
Author:
M.J. Brennan
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