DEVICE AND CONTROL SYSTEM FOR PRODUCING ELECTRICAL POWER
20170012571 ยท 2017-01-12
Inventors
Cpc classification
H02M3/158
ELECTRICITY
H02P29/60
ELECTRICITY
H02K35/00
ELECTRICITY
International classification
Abstract
Briefly, the invention involves a system and method for generating electrical power. The system includes an electromagnet positioned with one pole directed toward a like pole of a permanent magnet. The permanent magnet is preferably mounted for oscillating movement toward the pole of the electromagnet. A control system for the electromagnet is provided to supply direct current (DC) power in the form of square wave pulses which coincide with the position of the permanent magnet. Power is collected upon the collapse of the magnetic field within the electromagnetic magnet. In some embodiments the present device is supplied in the form of a reciprocating engine which provides rotary motion in addition to the electrical power generated.
Claims
1. A method of controlling the temperature of an electrical device comprising: providing a core for an electromagnet assembly; positioning a coil sized for placement about said core forming an electromagnet assembly having a first positive magnetic pole and a first negative magnetic pole defining a longitudinal axis of said electromagnet assembly; providing a permanent magnet having a second positive pole and a second negative pole; positioning said first positive magnetic pole in alignment with said second magnetic pole; delivering an electrical signal to said coil to energize said electromagnet assembly causing said electromagnet assembly to generate a magnetic field; connecting an output cable to said electromagnet assembly for distributing an electrical pulse generated upon the collapse of said magnetic field.
2. The method of controlling the temperature of an electrical device of claim 1 wherein said electrical signal is an electrical pulse.
3. The method of controlling the temperature of an electrical device of claim 2 wherein said electrical pulse is in the form of a square wave.
4. The method of controlling the temperature of an electrical device of claim 3 wherein said square pulses are delivered at a rate of at least one kilohertz.
5. The method of controlling the temperature of an electrical device of claim 1 wherein said core is longer than said coil.
6. The method of controlling the temperature of an electrical device of claim 5 wherein said core is twice as long as said coil.
7. The method of controlling the temperature of an electrical device of claim 1 wherein said first negative pole is aligned with said second negative pole.
8. The method of controlling the temperature of an electrical device of claim 1 wherein one of said electromagnet assembly or said permanent magnet assembly is oscillated with respect to the other during delivery of said electrical signal.
9. The method of controlling the temperature of an electrical device of claim 1 wherein both of said electromagnet assembly and said permanent magnet assembly is oscillated with respect to the other delivery of said electrical signal.
10. The method of controlling the temperature of an electrical device of claim 1 including an external electrically powered device, said external device being in electrical communication with said distributed electrical pulse.
11. The method of controlling the temperature of an electrical device of claim 10 wherein said external electrical device is a fusion reactor.
12. The method of controlling the temperature of an electrical device of claim 10 wherein said external electrical device is a low energy nuclear reaction.
13. The method of controlling the temperature of an electrical device of claim 10 wherein said external electrical device is an electrolysis reaction.
14. The method of controlling the temperature of an electrical device of claim 1 including the step of connecting a signal controller to said electromagnet assembly for varying said electrical signal supplied to electromagnet assembly.
15. The method of controlling the temperature of an electrical device of claim 14 wherein said electrical signal is varied based upon a temperature of an external electrical device in electrical communication with said distributed electrical pulse.
Description
BRIEF DESCRIPTION OF THE FIGURES
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DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0034] While the present invention is susceptible of embodiment in various forms, there is shown in the drawings and will hereinafter be described a presently preferred embodiment with the understanding that the present disclosure is to be considered an exemplification of the invention and is not intended to limit the invention to the specific embodiments illustrated.
[0035] Referring to
[0036] Referring to
[0037] Referring to
[0038] Referring to
[0039] Referring to
[0040] The high voltage system (HVDC) 104 is preferably a plurality of batteries 130 and capacitors 132. In a most preferred embodiment the array of batteries 130 comprises ten 12V DC batteries 134 hooked up in series to provide a total of 120V DC power 136 to the electromagnetic coils. The array of capacitors 132 preferably comprises about twelve 10,000 Pico Farad capacitors 138. The capacitors are generally constructed and arranged to smooth the draw on the batteries to provide extended run times, reduce heat build-up in the batteries 134 and provide a smoother power signal to the coils. The positive polarity of the battery array 140 connects to the line side of a single pole single throw switch which acts as the main power switch 142 and can either energize or shut down all of the 120V DC supplied components throughout the HVDC system. From the load side of the main power switch 142, the 120 v DC positive polarity is divided into two separate HVDC supply legs 144, 146. A first leg 144 connects to the collector 149 of the first insulated gate bipolar transistor (IGBT) 148 supplying power to coil bank 1 150, including coils 1 and 4 156, 158, while the second leg 146 connects to the collector 151 of the second IGBT 152 supplying power to coil bank 2 154, including coils 2 and 3 160, 162.
[0041] In a preferred embodiment, the first and second IGBTs 148, 152 are MITSUBISHI part no. CM1200DC 34N and are each rated at 1,700 Volts 1,200 Amps. The first and second IGBTs 148, 152 are configured to include dual switching (two channels) capability and can be operated either independently, in tandem, or in an alternating pattern. When two IGBTs are utilized, Channel one 164, 166 respectively of each IGBT provides independent switching of the coil banks 1 & 2. It should also be noted that while the preferred embodiment includes two IGBTs, more or less IGBTs may be utilized without departing from the scope of the invention. From the Channel one 164 emitter of the first IGBT 148 the 120 v DC power passes through blocking diode 168; and from the Channel 1 166 emitter of the second IGBT 152 the 120 v DC power passes through a blocking diode 170. Diodes 168 and 170 are preferably power diodes, VISHAY part no. SDIIOOC16 B-PUK, rated at 1400 Amp 1600 Volts. Diode 168 is connected to coil bank 1 150, and diode 170 is connected to coil bank 2 154. Diodes 168 and 170 prevent any back EMF caused by a failure in fly-back diodes 172 or 174 from reaching the first or second IGBTs.
[0042] Still referring to
[0043] Referring to the firing system 100, the Fiber Optically Interfaced IGBT Driver 200,202 is constructed and arranged to control the opening and closing of the IGBT gates, thus switching on or off the HVDC power to the coil banks. Power supplied to the IGBT driver board 200, 202 is a filtered and conditioned 15 v DC 0.5 Amp. via shield twisted pair wires 124 extending from power supplies 112, 114. The IGBT Driver 200, 202 is also constructed and arranged to include features that can be incorporated as torque power output IC Controller/Sensors that allow the shift from a push-push system between the electromagnets and the permanent magnets to a system that pushes on one coil bank while the other coil bank pulls (attracts) thus adding more torque to the power stroke. Shifting from a push-push mode to a push-pull mode may be accomplished on the fly.
[0044] High voltage DC switching is accomplished by two high voltage, high amperage insulated gate bipolar transistors (IGBT) 148, 152 and are preferably HVIGBT MODULES MITSUBISHI part no. CM1200DC 34N, each rated at 1700 volts 1200 amps. Each IGBT is controlled by a driver board 200, 202 that is fiber optically interfaced to a respective TB opto-coupler component 184, 186 located in the low voltage power modulator and pulse controller. Each IGBT gates power to a respective coil bank or cylinder independently of other IGBTs being utilized. Each electromagnetic coil bank 150, 154 preferably include a flyback diode 204, 206 across its positive and negative connection. It has been found that VISHAY part no. SDI500030L B-PUK is rated at 1600A 3000V diodes, and is suitable to eliminate flyback. Flyback is the sudden voltage spike seen across the inductive load presented by the coil banks when its supply voltage is abruptly changed by the systems pulsing and switching frequency. From each coil bank the high voltage DC continues through another isolation diode 208, 210, preferably VISHAY part no. SD1500030L B-PUK 1600A 3000V. Isolation diodes 208, 210 are to be considered legacy components; their primary function is to isolate the magnetic coil banks from one another. Isolation diodes 208, 210 connect to a common copper buss 212 which connects to the negative terminal of the high voltage DC 120V Power Supply battery array.
[0045] Referring to
[0046] Referring to
[0047] The present system comprises a highly polarized permanent magnet (PM) 16 adjacent to or in close proximity to a metallic magnon gain medium (MMGM), e.g. the core 24. The magnetic field imparted on the adjacent MMGM forms a localized spin accumulation, also known as a spin bias, or accumulation of non-equilibrium electrons. Since the spin accumulation in the MMGM is greatest in close proximity to the magnet, a spin diffusion gradient is formed through the length of the MMGM. Due to the elements present in the MMGM and the Fermi energies associated with the elements within the MMGM, the spin diffusion gradient sets up a preferred direction for the movement of magnon waves in the MMGM (magnon bias). The coil 28 that surrounds the MMGM is energized; preferably with DC square wave pulses from the firing system 100. The DC pulses provide an EMF in the direction of the interface between the PM and MMGM. Since the PM has already exerted a magnetic field great enough to spin polarize electrons in the nearby MMGM, equilibrium electrons (the ones that have not been spin biased) within this spin diffusion zone are already under EMF from the PM that brings them close to the spin-flip transition point (as described by the Zeeman Effect and Paschen Back Effect). The introduction of DC pulsed current at specific frequencies, voltages and currents provides the extra current needed to accomplish the spin-flip transition so that electron pairs in equilibrium (equal spin up and spin down) become non-equilibrium and become spin polarized for the duration of the square wave pulse. This is known as the spin-flip transition, and it takes place in the MMGM when the coil is energized. Magnon waves are already present due to the ambient heat in the atmosphere, the room or any location where the power generation apparatus resides. Therefore, magnon waves are present in the MMGM since it is at approximately the same temperature as the environment surrounding it. By nature, magnon waves are randomly oriented and cause random lattice vibrations between the atoms in any solid, including the MMGM. Magnon waves are present in any material that is warmer than absolute zero. When the coil around the MMGM turns on, inducing a magnetic field with sufficient intensity to exceed the localized Zeeman energy or spin-flip transition energy for equilibrium electrons in the metal atoms in the MMGM, electrons in these become spin biased and absorb a magnon to conserve energy during the spin flip. Therefore, with sufficient current delivered to the coil, the MMGM can saturate causing the maximum number of electrons to become spin biased and absorb magnons in the MMGM. As the square wave pulse falls to zero thus de-energizing the coil, normal spin relaxation occurs within the MMGM allowing substantially all of the magnons absorbed to be released at the same time, as a large percentage of the electrons in the MMGM flip back to their original spin orientation. Since all the magnons are dumped at once, they create an avalanche effect much like photons in a laser. When all of these magnons waves are released at the same time they are released toward the permanent magnet due to the polarization force of the magnet creating a spin bias or gradient in the MMGM, thus creating a preferred direction for the magnons to travel when they are released. As the magnons saturate or overload the MMGM with magnon waves in one direction, they collide with the end of the material at the point where the MMGM ends and the PM is positioned (known as the interface). The collapse of the magnetic field and the magnon bias direction is responsible for annihilating magnon waves through wave collision at the interface. When the magnon waves are destroyed, heat is destroyed making the temperature of the material drop. Since energy cannot be created or destroyed per the laws of thermodynamics, the ambient heat energy that caused the original randomly moving magnons in the MMGT core is converted back to a forceful spin wave in the MMGT core. This spin wave is propagated through the MMGT core as a strong electromagnetic pulse that can be collected via classical induction by the coil around the MMGT core. Once collected, the electrical power can be stored and applied to perform useful work.
[0048] It has also been discovered during experimentation that the temperature of the electromagnet(s), core(s) and an external assembly operating from the power generated by the present device can be manipulated by the application of specific tones, generated by varying the square wave power inputs to the coils. In these experiments, the external assemblies comprised electrolysis systems being operated by the power generation device. In these combined systems, the present power producing device was equipped with various sensors including, but not limited to, temperature sensors, voltage sensors, amperage sensors, and pressure sensors. The sensors were secured to measuring and recording equipment including an Astro-Med R TMX-18 portable data recorder as well as various video devices directed at mechanical gauges and the reaction within the electrolysis tank. The TMX is available from Astro-Med Inc. of 600 East Greenwich Ave. West Warwick R.I. 02893. Sweeps of various square wave patterns were supplied to the power producing device. Thereafter, the data was analyzed whereby correlations were found between power production and temperature within the system. The tones, e.g. frequencies of the square wave which produced desirable cooling or power production were then fed back into the power producing device as a constant or narrow band sweep signal to increase the desired effect. During this process it was discovered that specific frequencies caused cooling in the electrolysis portion of the system while other frequencies caused cooling in the electromagnet coils and cores of the electromagnets. Due to the speed in which the heat was eliminated, it is believed that this phenomenon is due to magnon conversion and/or annihilation around that portion of the system. Temperature drops of one hundred degrees Fahrenheit were observed to occur in 1 to 2 seconds in the coils and cores which have an included mass of about 20 pounds.
[0049] Referring to
[0050] This system also has application for driving fusion and/or LENR reactions which are extremely prone to runaway heat related failures. The present system can be utilized to cool or throttle the fusion or LENR reaction in the same manner as the electrolysis reaction to prevent the unwanted runaway failures related to excessive heat production. In operation, the system can monitor the heat production of the fusion or LENR reactions and vary the frequency of the pulse being supplied to the coil(s) assembly to provide a periodic or constant cooling cycle to the reaction. The excess heat is converted to electrical power which can be directed away from the system for useful work or can be redirected into the system for use by the reaction. The present system may also have application for refrigeration and heating systems whereby the power generation could be utilized for heat while the magnon conversion/destruction could be utilized for cooling or refrigeration.
[0051] All patents and publications mentioned in this specification are indicative of the levels of those skilled in the art to which the invention pertains. All patents and publications are herein incorporated by reference to the same extent as if each individual publication was specifically and individually indicated to be incorporated by reference.
[0052] It is to be understood that while a certain form of the invention is illustrated, it is not to be limited to the specific form or arrangement herein described and shown. It will be apparent to those skilled in the art that various changes may be made without departing from the scope of the invention and the invention is not to be considered limited to what is shown and described in the specification and any drawings/figures included herein.
[0053] One skilled in the art will readily appreciate that the present invention is well adapted to carry out the objectives and obtain the ends and advantages mentioned, as well as those inherent therein. The embodiments, methods, procedures and techniques described herein are presently representative of the preferred embodiments, are intended to be exemplary and are not intended as limitations on the scope. Changes therein and other uses will occur to those skilled in the art which are encompassed within the spirit of the invention and are defined by the scope of the appended claims. Although the invention has been described in connection with specific preferred embodiments, it should be understood that the invention as claimed should not be unduly limited to such specific embodiments. Indeed, various modifications of the described modes for carrying out the invention which are obvious to those skilled in the art are intended to be within the scope of the following claims.