They specified a chain here for a reason. Chains cannot sustain a compressive force. The force on the table is produced only by the latest link to strike the table. The part of the chain that has not yet hit the table is in freefall.
Since they are asking for force over time, this really sounds like a momentum transfer problem. Momentum has units like newton-seconds (force x time). The force is then the momentum per second tansferred to the table. Of course, the momentum is also mass x velocity.
When the distance fallen is x, the link striking the table has fallen a distance of x. It has a velocity based on the usual freefal relation:
v^2 = 2gx
Call the total chain mass M, the length L and there are n links. The mass and length of a link are M/n and L/n.
The momentum transferred by a link is P = (M/n) * v
The time it takes from one link to hit until the next one is the link length divided by velocity:
t = (L/n)/v
The momentum is the product of force and time:
P = F*t so F= P/t
Substituting from above:
F = ((M/n) * v) / (L/n)/v) = (M*v^2)/L
Substuting in the realtion between fall distance and velocity:
F = 2Mgx/L
After reading subsequent answers, I notice that I completely forgot about the static potion of the problem, that is the dead weight of the chain on the table. Since x length is on the table, that amounts to Mgx/L, which is exactly one half the static load. Adding the two gives:
F = 3Mgx/L
You can also work this via energy methods where you assume an elastic but stiff table. The result is the same.