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Vehicle System Dynamics
International Journal of Vehicle Mechanics and Mobility
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Research Article

Constructing critical control parameters to keep vehicle away from divergent loss of stability

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Received 26 Sep 2023, Accepted 30 Apr 2024, Published online: 07 May 2024

Figures & data

Figure 1. Two degrees of freedom bicycle model.

Figure 1. Two degrees of freedom bicycle model.

Figure 2. Graphical representation obtained using the Pevsner function Y¯=Y¯(δ2δ1) for the geometrical analysis of a set of stationary states for the vehicle model described by Equations (1) and (2).

Figure 2. Graphical representation obtained using the Pevsner function Y¯=Y¯(δ2−δ1) for the geometrical analysis of a set of stationary states for the vehicle model described by Equations (1) and (2).

Figure 3. The points of intersection between a moving straight line and a fixed curve indicate a divergent loss of stability in the corresponding multiple stationary regime, i.e. a bifurcation of a fold.

Figure 3. The points of intersection between a moving straight line and a fixed curve indicate a divergent loss of stability in the corresponding multiple stationary regime, i.e. a bifurcation of a fold.

Figure 4. Bifurcation diagram (solid curve) defined by the Equations (23)-(24) and the (dash curve) obtained using the numerical continuation method.

Figure 4. Bifurcation diagram (solid curve) defined by the Equations (23)-(24) and the (dash curve) obtained using the numerical continuation method.

Figure 5. Steering Angle θ as function of time for the realisation of straight-line motion where θ(t)θ(q)=0.0315rad.

Figure 5. Steering Angle θ as function of time for the realisation of straight-line motion where θ(t) → θ(q)=0.0315rad.

Figure 6. The stabilisation of straight-line motion generated by the steering angle θ(t) as solved by Equation (33).

Figure 6. The stabilisation of straight-line motion generated by the steering angle θ(t) as solved by Equation (33).

Figure 7. Analysis of divergent loss stability on the handling curve (with turning radius of R = 30 m); The long-dash curves are the handling curves and indicate the change in steering angle required for the vehicle to remain on a circlular trajectory of fixed radius if a change in the speed V occurs. The smooth solid curves are the bifurcation sets with the critical values of the control parameters (θ, V) corresponding to a divergent loss in stability for the stationary states of the system: (a) represents q =  μ = 0; (b) represents q =  0.3, μ = 0; (c) represents q =  0.3, μ = 0.03.

Figure 7. Analysis of divergent loss stability on the handling curve (with turning radius of R = 30 m); The long-dash curves are the handling curves and indicate the change in steering angle required for the vehicle to remain on a circlular trajectory of fixed radius if a change in the speed V occurs. The smooth solid curves are the bifurcation sets with the critical values of the control parameters (θ, V) corresponding to a divergent loss in stability for the stationary states of the system: (a) represents q =  μ = 0; (b) represents q =  0.3, μ = 0; (c) represents q =  0.3, μ = 0.03.

Figure 8. Graphical illustration of corrective steering angles under external lateral force; (a): the condition k¯1>k¯2, κ1=κ2; (b): the condition k¯1<k¯2, κ1=κ2; (c) and (d): k¯1>k¯2, κ1<κ2.

Figure 8. Graphical illustration of corrective steering angles under external lateral force; (a): the condition k¯1>k¯2, κ1=κ2; (b): the condition k¯1<k¯2, κ1=κ2; (c) and (d): k¯1>k¯2, κ1<κ2.

Figure 9. Graph of Y¯(δ2δ1,μ) for different values of parameter μ (1.μ1=0.01;2.μ2=0.0242;3.μ3=0.0342).

Figure 9. Graph of Y¯(δ2−δ1,μ) for different values of parameter μ (1.μ1=0.01;2.μ2=0.0242;3.μ3=0.0342).

Figure 10. Determination of the corrective steering angle for straight-line motion with a moment of the external force acting about the centre of mass vehicle (μ = 0.0242, q = 0.3, v = 18 m/s).

Figure 10. Determination of the corrective steering angle for straight-line motion with a moment of the external force acting about the centre of mass vehicle (μ = 0.0242, q = 0.3, v = 18 m/s).

Figure 11. (a): Stability diagram with an additional moment of the external lateral forces acting about a vertical axis at the vehicle of mass centre (μ = 0.0242, q = 0.3); (b): Fragment of stability diagram with an additional moment of the external lateral forces acting about a vertical axis at the vehicle of mass centre (μ = 0.0242, q = 0.3).

Figure 11. (a): Stability diagram with an additional moment of the external lateral forces acting about a vertical axis at the vehicle of mass centre (μ = 0.0242, q = 0.3); (b): Fragment of stability diagram with an additional moment of the external lateral forces acting about a vertical axis at the vehicle of mass centre (μ = 0.0242, q = 0.3).

Figure 12. The loss of divergent stability for straight-line vehicle motion (μ = 0.0242, q = 0.3) for critical values of the parameters θ(1)(q,μ)=0.01928rad, V×=21.91 m/s.

Figure 12. The loss of divergent stability for straight-line vehicle motion (μ = 0.0242, q = 0.3) for critical values of the parameters θ(1)(q,μ)=0.01928rad, V×=21.91 m/s.