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As the smoke cleared, Kyle Mcallister <[email protected]>
mounted the barricade and roared out:

> > Since a = f/m, and m is constant, if there is a
> > force in one direction only,
> > then that force should accelerate the mass while it
> > operates. That acceleration
> > should increase the speed, which should then remain
> > constant until the next
> > acceleration pulse. IOW the speed should increase in
> > steps.
> 
> It may be that there is a way to make it accelerate. I
> don't know. But what Laithwaite/Dawson say, and as far
> as I can tell, what happens in their setup is this:
> 
> 1. Mass M is moved say 10 units to the right by
> precession, thus (supposedly) forcelessly. F=0 at this
> point.
> 2. M is moved back to the left, to the starting point
> inertially. As it accelerates, the trolley moves to
> the right, say, ultimately 2 units. Velocity of the
> entire system is towards the right.
> 3. When M reaches the starting point, it is stopped,
> decelerating, thus cancelling the previous
> acceleration. The velocity is now zero again, but the
> trolley is 2 units to the right.
> 4. Repeat.
> 
> Each cycle, the velocity ends as zero, but a 'net'
> constant velocity is attained based on the
> acceleration imparted to M, and its mass ratio versus
> the rest of the trolley. As far as I see, there is not
> a net gain in velocity over time, so no additive
> acceleration. You get 'displacement' over time,
> however, each cycle moving the trolley's center of
> mass 2 units to the right. Assuming, of course, that
> it does work. I don't know if it does or not.
> 
> --Kyle

Is there an animation of this?
There should be.


- -- grok.






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