Magneto-elastic dynamics and bifurcation of rotating annular plate
Hu Yu-Da1, 2, †, Piao Jiang-Min1, 2, Li Wen-Qiang1, 2
       

In region 4 of Fig. 4, the motion of the system becomes a quasi-period motion again when B0z = 3 T, which is reflected in (a) Poincaré map that is mapping circle formed by a number of points, (b) time history diagram, (c) power spectrum, and (d) phase diagram.