The displacement \(x\) of a spring-mounted mass under the action of dry friction is assumed to satisfy \[ m\ddot {x}+kx=-F_0\sgn (\dot {x}) \] An example would be a mass \(m\) connected to a fixed support by a spring of stiffness \(k\) and resting on a surface with frictional force \(F_0\), \(F_0>0\). Set \(m=k=1\) for convenience and let \(y=\dot {x}\).
- Consider the initial conditions \(x=x_0>0\), \(\dot {x}=0\) at \(t=0\). Show that the phase path will spiral exactly \(n\) times before reaching equilibrium if \[ (4n-1)F_0<x_0<(4n+1)F_0. \]
- Suppose the initial conditions at \(t=0\) are \(x=x_0>3F_0\) and \(\dot {x}=0\). Subsequently, whenever \(x=-\alpha \), where \(2F_0-x_0<-\alpha <0\) and \(\dot {x}>0\), a trigger operates to increase suddenly the forward velocity so that the kinetic energy increases by a constant amount \(E\). Show that if \(E>8F_0^2\) then a periodic motion is approached, and show that the largest value of \(x\) in the periodic motion is equal to \(F_0+E/(4F_0)\).