Abstract:
A nonlinear equation of motion for a pendulum-type system is investigated. It differs from the
classical equation of a mathematical pendulum in the presence of a parametric disturbance. The
potential energy of the «pendulum» is a two-stage periodic step function of time. The equation
depends on two parameters that characterize the time-averaged value of a parametric disturbance
and the depth of its «ripple». These parameters can take on arbitrary values. There exist two
equilibrium configurations corresponding to the hanging and inverse «pendulum». The problem
of stability of these equilibria is considered. In the first approximation it necessitates an analysis
of the well-known linear Meissner equation. A detailed investigation of this equation is carried out
supplementing and specifying the known results. The nonlinear problem of stability of equilibria
is solved.