Since the direction and magnitude of force is constant, we have
Fsin a - m1 g ? T sin a = m1 a y ---------- (1)
Where m1 is the mass of that part of the chain, which already got lifted and T is the tension in that part of the chain, which is the intersection of the hanging part, and the part still on the ground. ?m2? is that part of the chain which is still on the ground.
Fcos a - T cos a = m1 a x -------------- (2)
T cos a = m2 ax -------------- (3)
From 2 and 3 we get
Ax = Fcos a / m ---------------- (4)
Putting 4 in 3 we get
T = m2 F / m ----------------------- (5)
Putting 5 in 1 we get
Ay = (F sin a / m) ? g -------------------- (6)
From 4 and 6 we get the velocities in x and y directions as
Vx = F cos a t / m --------------- (3)
Vy = (Fsin a - mg) t / m --------------- (4)
Also since a y is constant by the time the chain is totally lifted the C.M. of the entire chain will be at a height of h = L sin a / 2. And from the equation of
h = a y t2 / 2 , we get the value of ?t?. Therefore from 3 and 4 we get the values of
Vx and Vy . Then the resultant velocity is given by the square root of the sum of the squares of Vx and Vy