Try to imagine the spatial existence of a magnetic field.. how it 'flows' (for lack of a better term), and what the field's geometry would look like.
Magnetic fields are toroidial. That is to say... Like a doughnut. The doughnut could be tall or short, stretched way out, or flat like a pancake.. But the field will always travel in that donut shape.. out from the top center of one pole on the magnet.. around the outside of the magnet, and back in to the bottom center of the other pole on the magnet.
If we shield one pole of the magnet, one of two things will happen, depending on the material used- The field will either pass through the shielding, totally unaffectedly as if the shielding weren't even there... or the field will accept the material as part of the magnet itself, and will travel along the outside of the shielding, and into the center end of the shielding. You will have a slight manipulation of the geometry of the field itself, but not significantly enough to do anything practical with it in terms of a spinning wheel.
But this is really an un-necessary element of discussion when we talk about gaining energy from a magnetic wheel, because only two poles are significant in the system.
To gain acceleration, you have to use either attractive effect, or repulsive effect. One or the other at any point in the rotor's rotation. You can flip them around, but if we freeze-frame the rotor at any point in it's rotation, you'll either see a net attraction, or a net repulsion acting on the rotor.
Let's examine a hypothetical magnet with only one pole.. a sphere with either a N charge, or an S charge, representing the North or South pole of a magnet.
You have two of them, coming closer together, and the change they experience will either be repulsive or attractive. Either way you look at it, you'll have the same net effect-
If an N sphere nears an S sphere, you will have an initial 'pull' until they reach equilibrium. Much like a pendulum, and Earth's gravity. It will fall, until it can't fall any more, at which point it will either stop, or begin trying to leave the field in the opposite direction.
When the N and S try to separate from one another, they both experience an identical attraction. The very same attraction that pulled them together to start with. If the wheel gains 'x' units of energy on the way in, it will lose 'x' units of energy on the way out.
The same goes for a repulsive effect, only in reverse... It takes 'x' units of energy to push them together, and they will gain the same 'x' units of energy as they push each other away.
This is how I understand the reality of permanent magnets. I wish it were different, but I have not been able to observe any evidence that suggests they will behave any other way.
However, there is one thing to consider... And I'm not sure if this could be applied to an OU design at all, since I haven't been able to experiment significantly with it yet.
If we wrap a magnet in copper wire.. building an electromagnet, with a permanent magnet core. You could theoretically nullify the net effect of the magnet core for a brief moment, at the rotor's apex... producing a net gain in rotational energy experienced by the rotor.
How much energy it takes to reduce the magnetic field of the magnet core is up for debate at this point, but it's something to think on for the moment.Statistics: Posted by Cryptonic26 — Wed May 21, 2008 11:46 am
]]>