“…For a suspended chain, its dynamic equation is generally solved using Bessel functions and Neumann functions to obtain its natural frequency of vibration, energy distribution, chain tension, composite vibration, standing wave characteristic points, etc., [ 33 , 34 , 35 ]. As shown in Figure 10 , for a chain with length L and density ρ , suspended along the x -axis, with endpoint A undergoing sinusoidal vibration in the y-direction, the vibration displacement of any point B on the chain at time t is u ( x , t ), and point C at a distance dx ( dx approaching 0) from point B is subject to tension FT ( x ), FT ( x + dx ), and external force dF .…”