I think this problem would be solved by breaking the movement down into three phases.
For the case of the slow movement, for theoretical purposes, say the weightlifter lifts a weight vertically upward for a given distance (say 2 feet this for example). In order to get the weight moving, the force exerted by the lifter must be
more than the gravitational force (From
F = ma. Since the
net acceleration is upward, the
net force must also be upward.) Here, the weightlifter exerts the greatest force of the lift. Once the weight is moving upward, it reaches some intermediate velocity (the max speed at which the weight moves upward. If the lifter takes 2 seconds to lift the weight from initial to final position, then this velocity is 1 foot per second.) During this stage of movement, the net acceleration of the weight is zero, since it is moving at constant velocity, until the lifter nears the top of his movement. Now the weight will be slowed by the downward acceleration due to gravity, with the lifter no longer exerting any counteracting upward force. In this third phase, the weight would have acquired a kinetic energy of 0.5 m v
2, and gravity must convert this kinetic energy to potential energy until the kinetic energy equals zero, where the weight will be at a stop (at rest). Therefore the work done by the lifter would have only been done in the first and second phases of the lift, whereas in the third phase, gravity does the work of slowing the weight to a stop.
In the case of the fast moving weight, all the things are the same, except that the
initial force exerted by the weightlifter is greater (since it reaches a greater acceleration), and the time of the second phase is
shorter (since it has a higher velocity but the same total distance as in the slow case), so the weightlifter exerts the force for less time. Not to mention, the weight would take
longer to stop since it has a higher kinetic energy than in the slow case, so the lifter must stop his rep sooner to allow more time for the weight to come to a full stop. This means that the distance traveled by the weight in this phase would be shorter than in the slow case. So in this example, a greater force is exerted for less time, and so I suspect that the equations would work out to be the same no matter which formula was used.
To show it another way:
(top = finish)...SLOW...FAST
|......[3]...[3]
|......[2]...[3]
|......[2]...[3]
|......[2]...[2]
|......[2]...[1]
|......[1]...[1]
|......[1]...[1]
(bottom = start)
Where phase [1] is the weightlifter pushing the weight to its max velocity (in phase [2]), so the weight is accelerating upward
In phase [2] the weight has reached a constant velocity (the speed of the weight during the lift), and so it has no net acceleration, and the force exerted by the lifter is equal to the force of gravity on the weight (which is the weight
of the weight)
And in phase [3], the lifter is doing NO work and could essentially let go of the weight as the weight slows to its final velocity (zero) and its kinetic energy gets converted to potential energy by the work done by Earth's gravity
In the real world, of course the force exerted by the lifter will not be constant, nor will the acceleration nor the upward velocity of the weight. But for an idealized model I believe this is correct.
The profiles of the two cases are different and so I suspect that the equations will work out to show equal work done in both cases, but I have already spent like 20 minutes typing this so I'm done and I'll leave the math to someone else
