The descending part of the chain is in free fall, it has speed
v=√2gh at the instant, all its points have descended a distance
y. The length of the chain which lands on the floor during the differential time interval
dt following this instant is
vdt.
For the incoming chain element on the floor,
From
dpy=Fvdt (where y - axis is directed down)
0−(λvdt)v=Fydtor
Fy=−λv2=−2λgyHence, the force exerted on the falling chain equals
λv2 and is directed upward. Therefore from third law the force exerted by the falling chain on the table at the same instant of time becomes
λv2 and is directed downward. Since a length of chain of weight (
λyg) already lies on the table the total force on the floor is
(2λyg)+(λyg)=(3λyg) or the weight of a length
3y of chain.