I was thinking that a picture could help...
https://www.physicsforums.com/attachment.php?attachmentid=59224&stc=1&d=1370226389
(above) the head of the hammer is mass M, it starts out height h above the ground as the player puts their effort into bringing it down.
The player, here, adopts a strategy of raising the hammer as high as possible and bringing it down as straight as they can - so the trajectory of the hammer-head (light green) is not going to be circular. The hammer strikes the lever a time t
0, a distance r from the pivot - the lever moves through angle θ (which we will consider small enough to approximate sinθ≈θ and cosθ≈1 to keep the math simple) and strikes the ground at time t
1 where it stops turning.
The mass being lifted is m, a distance r on the other side of the lever to the hammer.
In this picture, I am constraining it to move vertically (vertical dotted line) only so I don't have to worry too much about friction.
The mass remains stationary until time t=t
0, when it starts to rise.
At t=t
1 it has risen through height y=y
1 and the lever stops pushing it up.
It continues, however, due to the law of inertia, until it reaches a final height y=y
2 at time t=t
2, where it starts to fall again.
We want to consider two situations
1. where y
2 > y
1
2. where y
2 = y
1
The assertion in post #1 and subsequently is that both these situations can be achieved using the same constant force from t0-t1, but for different lengths of time.
Hopefully this will be suitable for OPs discussion.
In the energy picture, the hammer delivers energy to the mass as W = Mgh + E where E is supplied by the muscles of the player. The mass is, therefore, able to rise a total of y
2 = W/mg.
If follows that for y
2 > y
1 the work supplied must be greater ... but, if a constant force has been applied both times, then the work is the same, and this cannot have happened. This is the contradiction that so confuses Adjacent (OP).
The answer, of course, is that the same force cannot have been applied both times.
The contradiction
proves it.
@Adjacent: you should do the math.
Real life hammer blows are quite complicated.
Lets forget the hammer for a bit and just say there is some mechanism that acts to provide a constant force F where the hammer would otherwise strike, for a time period T = t
1 - t
0.
This force is delivered, via the lever, directly to the bottom of the mass m.
So the free body diagram for mass m for t
0 ≤ t < t
1 has two forces, and for t ≥ t
1 has one force.
ƩF =ma will get the acceleration for each time-period.
The suvat (or "kinematic") equations can be used to find the distance the mass moves in each time period.
A simpler situation will help you understand what is happening ... a force F applied to mass m for time T will produce an acceleration a=F/m
If the mass starts at rest so u=0, then you can work out the equation for the distance s traveled as a function of T and F. Do it.
In order to double the time to travel the same distance, what has to happen to the force?