The displacement \(x\) of a spring–mounted mass under the action of dry friction is assumed to satisfy \[ \ddot {x}+x=F_0\operatorname {sgn}(v_0-\dot {x}) \]
- Calculate the phase paths in the \((x,y)\) plane and draw the phase diagram. Deduce that the system ultimately converges into a limit cycle oscillation. What happens when \(v_0=0\)?
- Suppose \(v_0=0\) and the initial conditons 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 \(F_0+E/(4F_0)\).