Motorcycle with a rider a physical system and mathematical model.
of the motorcycle with a rider as indicated in Fig. 1.17(b). In this model, the equivalent stiffness includes the stiffnesses of the tires, struts, and rider. The equivalent damping constant includes the damping of the struts and the rider. The equivalent mass includes the masses of the wheels, vehicle body, and the rider. This model can be refined by representing the masses of wheels, elasticity of the tires, and elasticity and damping of the struts separately, as shown in Fig. 1.17(c). In this model, the mass of the vehicle body and the mass of the rider are shown as a single mass, When the elasticity (as spring constant ) and damping (as damping constant ) of the rider are considered, the refined model shown in Fig. 1.17(d) can be obtained.
Motorcycle with a rider a physical system and mathematical model.of the motorcycle with a rider as indicated in Fig. 1.17(b). In this model, the equivalent stiffness includes the stiffnesses of the tires, struts, and rider. The equivalent damping constant includes the damping of the struts and the rider. The equivalent mass includes the masses of the wheels, vehicle body, and the rider. This model can be refined by representing the masses of wheels, elasticity of the tires, and elasticity and damping of the struts separately, as shown in Fig. 1.17(c). In this model, the mass of the vehicle body and the mass of the rider are shown as a single mass, When the elasticity (as spring constant ) and damping (as damping constant ) of the rider are considered, the refined model shown in Fig. 1.17(d) can be obtained.
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