All the links of the chain have the same displacement, velocity and acceleration. The corner only produces a change of direction. We therefore consider the chain to be a single mass with an applied force that depends on the length x of the overhanging part. Thus, with a = ¨x,the equation of motion is
This differential equation of second order with constant coefficients has the solution
we calculate the integration constants from the intial conditions :
This solution is valid only for x ≤ l. We may also solve the problem by making an imaginary section cut at the corner. then the equations of motion for each part of the chain are
if we eliminate S we again obtain the differential equation