A uniform heavy chain of length 'a' initially has length 'b' hanging off of a table. The remaining part of chain a - b, is coiled on the table. If the chain is released, the velocity of the chain when the last link leaves the table is
√2ga3−b33a2
This is a variable mass problem, so momentum is constantly changing:
Fext=m(t)g=dPdt=d(m(t)v(t))dt=ma+v˙m
mg=ma+v˙m
Simplying the differential equations, we will get the answer