Energy Generation Using Cyclically Asymmetrically Distributed Charges

Abstract

Cyclically asymmetrically distributed charges introduced to explain a cause of gravity produce significant directed forces for useful safe energy generation, as harnessed by the Electric Kinetic Pulse generator, an experiment to illustrate cyclically asymmetrically distributed charges. This is established by analysing solutions to the equations of motion and energy of 4 charges in the Electric Kinetic Pulse generator, as they alternately move close to and from electric field singularities using repulsion in each of the 4 cylinders; with extensions to several charges. The system is shown to be robust against transverse vibrations. The theoretical validity of the generator and the principles underlying cyclically asymmetrical charge distributions is established. The theoretical verification proposes an iterative process for solving first order differential equations which requires continuity but no separation of variables. Ample useful nuclear energy independent of heat phenomena or the atmosphere can be generated with no harmful radiation or radioactive waste.

Appendix

Fig. 1

EKP generator diagram

Figure 1 Key:

• 1. Source of charges, with + for positive charges and − for negative charges. The arrow indicates the required direction towards the target plate (4). There is an insulator between the charge source and the metal cylinder (8) holding it. The outlet for the charges needs to be closed or open as required, to regulate the number of charges in the cylinder. The positive charges may be ionised argon, and the negative charges may be electrons from thermionic emission.

• 2. Programmable logic controller (PLC), with input and output shown by the arrows. The input is the pulse from the charge detector(s) via its circuit (3). The outputs of the PLC are the switches enclosed within dotted boxes. The PLC need to be programmable with a high level language (e.g. VB6) to take advantage of the computations of charge dynamics.

• 3. The circuit D of the charge detector, with antenna (6) insulated from the prism holding it. The charge detector seems best to be an FET gate, and the circuit would probably have a filter to remove the noise, and an operational amplifier to magnify the signal from the charge radiation. There may be more than one detector, in which case the charge signals need to combined in an AND gate before they are inputted into the PLC.

• 4. Target plate, insulated (7) from the rest of the cylinder.

• 5. A combination of switches to various resistances. These switches may each be at the gate terminal of an FET used as a resistor.

• 6. The antenna of the charge detector, which may be an FET gate.

• 7. The insulation between the target plate and the rest of the metal cylinder.

• 8. The metal cylinder, probably of copper, holding a vacuum.