I. Introduction
The maglev system carries out suspending function and is the core part of the maglev train. Fig. 1 gives its working principle. The guideway is flexible in the engineering environment [1]–[4]; thus, the oscillation induced by Bernoulli–Euler (B–E) beam equation must be considered. Dynamic responses of maglev vehicle/guideway system have great influence on running safety, ride comfort, and system costs, which are crucial factors for a maglev train's commercial application [1]. Cai et al. [2] built a dynamic model of the maglev system with multiple degrees of freedom (DOF) and guideway interaction, and numerically studied the elastic deformation of the guideway and dynamic behavior of the vehicle. Zheng et al. [3] discussed the stable and dynamic properties of the system coupled with the vehicle movements, guideway vibration, and control subsystem on the basis of a second-order suspension body with 5 DOF. By investigating the effects of the nonlinear spring on the dynamic behavior of such systems, Zheng et al. noted that nonlinear terms of spring, velocity of the vehicle, and control parameters influence the stable region of the maglev system, and chaos response may appear [4]. But resonant response of the maglev system induced by the guideway does not receive enough attention.