The PDF gives initial position and initial rotating-frame velocity zero. Use those values; the TeX erroneously places dots over the position coordinates.
For rotation about the third axis, the supplied acceleration relation and Newton's second law give the equations of motion in a rotating frame
Thus . Set to combine the planar equations:
The two characteristic roots are and . From and ,
The triple-angle formulas therefore give the particularly simple astroid motion of a harmonic oscillator in a rotating frame
The orbit satisfies ; the zero speed at each cusp is consistent with the smooth time-parametrized motion.
Its rotating-frame speed is
Hence, for , the first maximum occurs at , and
The maximum repeats periodically. For a signed negative angular frequency, use and ; at the particle remains at rest.
Figure 1.
Astroid orbit and the first maximum speed in the rotating frame
.

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