Thomas Conway said:
How does the physical torque and speed(rpm) of the flywheel affect the voltage and amperage of the outputting electricity?
From what I can gather it seems the only important factors in generating current is the speed of fluctuations in the magnetic field (directly caused by the velocity of the wheel) and the number of windings in the coil. if torque power has no relation to magnetic fields theoretically could you not create a step-down gear ratio system making the output wheel spin much faster than the driving wheel at the cost of non-relevant torque which would increase the wattage/ efficiency overall? or
Am I missing something??
Yes, you're missing the principle of conservation of energy. We can't create or destroy energy.
Hence your scheme for free energy from nowhere by adding gears (which is effectively what you are suggesting) fails, as all such schemes fail.
You sound as though you are already familiar with the principles involved. To sort out what's happening we just need to consider them in the correct order, which turns out to be backwards, from the electrical load back through the system.
For each step in the generating process the energy needs to be supplied by the previous step, along with any losses in each step.
We have a generator providing electrical energy to some electrical load. The generator is getting that energy, along with a bit extra for losses, as mechanical energy from the flywheel. In order to keep turning, the flywheel is presumably receiving mechanical energy from some source, usually known as a prime mover in electrical generation circles.
As you note, the voltage, V, generated in the generator is determined by the speed of the generator, and hence the speed of the attached flywheel. (There are some other factors, but we'll assume they are constant.)
The current, I, flowing in the electrical load is then determined by the generator voltage and the impedance, Z, of the load.
These are related by Ohm's Law, of course: I = V/Z Amps
The electrical power supplied to the load, P = V * I * PF Watts
(where PF = Power Factor of the load. This will be 1 for a resistive load or DC generation.)
If the voltage, V, increases, the power P will also increase because V appears in the formula for P. However the current, I, will also increase because V also appears in the Ohm's Law formula for I, hence the power increases again as I also appears in the formula for P.
We can combine these two formulae to show both effects:
P = V * I * PF = V * (V/Z) * PF = V^2 * PF/Z Watts.
If we keep the load constant the power factor and impedance will stay the same and the electrical power supplied will vary in proportion to the square of any changes in the voltage.
The generator will need mechanical power to drive it. Ignoring the small losses in the generator the required mechanical power will equal the electrical output power.
Mechanical power in a rotating system = torque * rotational speed * k
(where k is a constant dependent on the system of units you are using.)
So
torque * rotational speed * k = P = V * I * PF (Watts)
In a practical AC mains generation system we keep the rotational speed constant so the generated supply frequency is constant and we keep V constant (via a mechanism I haven't discussed). Taking out the constant parts from the above equation we get that:
torque is proportional to I.
Note that in a mains-style generation system the torque is determined by the load current, not the other way round.
So, what happens with your proposed gearing arrangement? If you add gears to spin the generator faster (whilst, we will assume, keeping the flywheel/prime mover running at constant speed) you will increase the generated voltage (in proportion to the speed of the generator). The power supplied to the load and hence the power demanded by the generator from the flywheel will increase, in proportion to the square of the ratio of the voltage increase. The torque demanded by the generator from the flywheel will increase to supply the extra power. No free energy will be created.