The Hamilton's equations of gyroscopic systems are derived.;It is pointed o
ut that gyroscopic forces are derived from kinetic energy and/or potential
energy, so they should be regarded as a part of Hamiltonian systems rather
than externally generalized forces. A symplectic transformation matrix is p
roposed to decouple the Hamilton's equations of linear gyroscopic systems.
It is shown that the exact stationary solution of a stochastically excited
and dissipated gyroscopic system is not affected by the gyroscopic forces w
hen the gyroscopic system as a Hamiltonian system is non-integrable. When t
he gyroscopic system is integrable, the stationary probability density and
the statistics for various generalized coordinates vary with the gyroscopic
forces while the mean total energy of the system is unchanged. A stochasti
cally excited and dissipated gyropendulum is studied in detail to demonstra
te the inferences. (C) 2000 Elsevier Science Ltd. All rights reserved.