I used the term ‘Gravity Wheel’ in the title of this blog in place of ‘Bessler’s Wheel’ to show that gravity wheels might have different configurations to Bessler’s Wheels, although from what I know I don’t think the basics will differ very much.
Fletcher made a comment in my last blog which touched upon a point which most of us will be aware of but which maybe some people missed the potential beneficial consequences of including its actions in our designs. I know its action is used in Bessler’s wheel.
fletch wrote, “ By my reasoning, therefore, for a Bessler wheel to gain in Angular Momentum and be everlasting in motion etc, then some part of the local available Angular Momentum pool must be compensatorily depleted to give the runner Rotational Kinetic Energy.”
A couple of years ago I realised the importance of something connected with gravity wheels which I had been aware of all my life but never considered it’s potential as a source of free energy, additional to that which we already know about, i.e, gravity enabled falling weights.
We design weights to be able to move around with the intention of causing the wheel to overbalance. We can calculate the work done by gravity in making the weights fall, but of course the path of the falling weight is not needed because we only need the perpendicular height of the fall. But if the weight is required to do work as it falls, and still overbalance the wheel, the extra time which the weight takes to fall because it’s doing work, does not affect the calculation, because in the simplest terms, time is not a necessary ingredient.
Therefore if we simply configure the mechanism to react to the position change of the wheel and use gravity to make a weight move into position which overbalances the wheel, we miss the opportunity to use the weight’s action or motion under the force of gravity, to do some work during its fall.
If the weight is in free-fall, it has no potential energy to unleash as kinetic energy, until it lands, but if it does work as it falls then it is using kinetic energy as it does so and it can still cause the desired overbalance by its eventual completion of its fall. The argument is similar that used in describing the friction generated in a brick sliding down a slope but in this case the work/friction could be used to help lift a fallen weight. This action may explain von Erlach’s description of each weight “landing gently on the side towards which the wheel turned”. There was little or no padding because the weights were slowed down by doing work, and made reduced noise as they landed.
This idea I believe might correspond to fletch’s comment that “….some part of the local available Angular Momentum pool must be compensatorily depleted to give the runner Rotational Kinetic Energy.”
JC
