1992
DOI: 10.2346/1.2139507
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Tire Modeling by Finite Elements

Abstract: Recent advances in the development of a general three-dimensional finite element methodology for modeling large deformation steady state behavior of tire structures is presented. The new developments outlined here include the extension of the material modeling capabilities to include viscoelastic materials and a generalization of the formulation of the rolling contact problem to include special nonlinear constraints. These constraints include normal contact load, applied torque, and constant pressure-volume. S… Show more

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Cited by 41 publications
(29 citation statements)
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“…Finite element simulations are well established in tire industries for the product development with special focus on stationary rolling properties [2,8,17,29]. For these stationary rolling analysis the relative kinematic Arbitrary Lagrangian Eulerian (ALE) description has been established, and the theoretical foundations are summarized in [19].…”
Section: Introductionmentioning
confidence: 99%
“…Finite element simulations are well established in tire industries for the product development with special focus on stationary rolling properties [2,8,17,29]. For these stationary rolling analysis the relative kinematic Arbitrary Lagrangian Eulerian (ALE) description has been established, and the theoretical foundations are summarized in [19].…”
Section: Introductionmentioning
confidence: 99%
“…A non-linear sidewall element is described in [35], while a model focused on the simulation of the contact is presented in [36]. A detailed discussion on discretized modelling approaches can be found in [37,38].…”
Section: Discretized Tyre Modelling Approachmentioning
confidence: 99%
“…Many previous works [22,4,24,26,19,12,20,27,14] use a change of variables X = R(t)X, where R(t) is the rotation matrix describing the rotation of the tire up to time t. The equations of motion are then reformulated with this change of variables, and the steady state solution to the spinning tire becomes a static problem, i.e. the transformed motion of the tire under this change of variables, φ, satisfies φ( X, t) = φ( X, 0) for all time.…”
Section: Layout Of the Present Workmentioning
confidence: 99%
“…We show below that z 0 satisfying ∂ t F(z 0 , 0) = 0 are steady state solutions. We follow a common approach in the literature for solving the steady state problem (see [4,24,26,19,12,20,27,14]) and introduce a new spatial variable X defined by…”
Section: Steady State Solutionsmentioning
confidence: 99%
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