Steady-state rolling analysis of a tire

This example illustrates the use of steady-state transport in Abaqus to model the steady-state dynamic interaction between a rolling tire and a rigid surface.

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Steady-State Transport Analysis

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A steady-state transport analysis uses a moving reference frame in which rigid body rotation is described in an Eulerian manner and the deformation is described in a Lagrangian manner. This kinematic description converts the steady moving contact problem into a pure spatially dependent simulation. Thus, the mesh need be refined only in the contact region—the steady motion transports the material through the mesh. Frictional effects, inertia effects, and history effects in the material can all be accounted for in a steady-state transport analysis.

The purpose of this analysis is to obtain free rolling equilibrium solutions of a 175 SR14 tire traveling at a ground velocity of 10.0 km/h (2.7778 m/s) at different slip angles on a flat rigid surface. The slip angle is the angle between the direction of travel and the plane normal to the axle of the tire. Straight line rolling occurs at a 0.0° slip angle. For comparison purposes we also consider an analysis of the tire spinning at a fixed position on a 1.5 m diameter rigid drum. The drum rotates at an angular velocity of 3.7 rad/s, so that a point on the surface of the drum travels with an instantaneous velocity of 10.0 km/h (2.7778 m/s). Another case presented examines the camber thrust arising from camber applied to a tire at free rolling conditions. This also enables us to calculate a camber thrust stiffness.

An equilibrium solution for the rolling tire problem that has zero torque, T, applied around the axle is referred to as a free rolling solution. An equilibrium solution with a nonzero torque is referred to as either a traction or a braking solution depending upon the sense of T. Braking occurs when the angular velocity of the tire is small enough such that some or all of the contact points between the tire and the road are slipping and the resultant torque on the tire acts in an opposite sense from the angular velocity of the free rolling solution. Similarly, traction occurs when the angular velocity of the tire is large enough such that some or all of the contact points between the tire and the road are slipping and the resultant torque on the tire acts in the same sense as the angular velocity of the free rolling solution. Full braking or traction occurs when all the contact points between the tire and the road are slipping.

A wheel in free rolling, traction, or braking will spin at different angular velocities, ω, for the same ground velocity, v0. Usually the combination of ω and v0 that results in free rolling is not known in advance. Since the steady-state transport analysis capability requires that both the rotational spinning velocity, ω, and the traveling ground velocity, v0, be prescribed, the free rolling solution must be found in an indirect manner. One such indirect approach is illustrated in this example. An alternate approach involves controlling the rotational spinning velocity using user subroutine UMOTION while monitoring the progress of the solution through a second user subroutine URDFIL. The URDFIL subroutine is used to obtain an estimate of the free rolling solution based on the values of the torque at the rim at the end of each increment. This approach is also illustrated in this example.

A finite element analysis of this problem, together with experimental results, has been published by Koishi et al. (1997).