TWI646762B - Electromagnetic energy-flux reactor - Google Patents

Abstract

The present invention provides systems and methods for providing power to a load. A system includes a first reactor comprising a first plurality of coils. One of the first plurality of coils is configured to generate a first magnetic field, and the plurality of second coils of the first plurality of coils are configured to generate a plurality of second magnetic fields and to change the first magnetic field One of the strengths. The system further includes a second reactor, the second reactor including a second plurality of coils, wherein the second plurality of coils are configured to tune the first reactor to the load. The first reactor is configured to provide the power to the load, and the second reactor is configured to increase the intensity of one of the second magnetic fields generated by the second coils and The first reactor is tuned to the load to increase the power supplied to the load.

Description

Electromagnetic energy flux reactor Cross-reference to related applications

This application is a continuation-in-part of the International Patent Application No. PCT/PH2011/000015, filed on Sep. 23, 2011, which is incorporated herein by reference.

This section is intended to provide a background or context of the invention as set forth in the claims. This description may contain concepts that are practicable, but without the concept that has been previously conceived or practiced. Therefore, unless otherwise indicated herein, what is described in this section is not the description of the present invention and the prior art of the claims. In addition, any reference to the subject matter discussed in this section is discussed by way of example only, and the inclusion of such references in this section is not an admission that

The power supply and/or conversion system is typically configured to supply power to one or more types of loads, such as a power grid or one or more electrical devices (eg, motors). These systems can receive power from one or more power sources, such as batteries. These systems convert power into one form for use by the load and transmit the converted power to the load for use by the load.

One method for increasing the efficiency of such systems is to drive the load using electricity obtained from an electromagnetic field. Katargin et al ( "Katargin") of US Patent No. 8,363,426 discloses a device for the ineffective power for electricity generation facility. The reactive power is provided by a high frequency, high voltage electromagnetic oscillator source. The inductive coil is placed in close proximity to the source of electromagnetic radiation (SEMR), loosely coupled to the SEMR, and tuned to resonate at the same frequency as the SEMR. The coils do not have a ferromagnetic core. The energy emitted by the electromagnetic oscillation source is transmitted to the inductor, and the reactive current induced in the coil is collected from the inductor and converted to a standard AC voltage. The inductor coil is tuned to the SEMR and placed in close proximity to the SEMR, and the SEMR is a high frequency, high voltage source.

There is a need for a system for supplying electrical power to a load that utilizes the power obtained using electromagnetic induction and overcomes the disadvantages associated with known systems.

One embodiment of the present disclosure is directed to a system for providing power to a load. The system includes a first reactor including a first coil configured to generate a first magnetic field and configured to generate a plurality of second magnetic fields and varying at least one of the strengths of the first magnetic field a second coil. The system further includes a second reactor comprising at least one second reactor coil configured to tune the first reactor to a load. The first reactor is configured to provide electrical power to the load, and the second reactor is configured to increase the intensity of one of the plurality of second magnetic fields generated by the at least one second coil and to tune the first reactor The power supplied to the load by the first reactor is increased to the load.

Another embodiment of the present disclosure is directed to another system for providing power to a load. The system includes a first plurality of coils. One of the first plurality of coils is configured to generate a first magnetic field, and the plurality of second coils of the first plurality of coils are configured to generate a plurality of second magnetic fields and change one of the first magnetic fields . The system further includes a second plurality of coils. The second plurality of coils are configured to couple at least one of the first plurality of coils to the load. The first plurality of coils are configured to provide power to the load, and the second plurality of coils are configured to increase the intensity of one of the plurality of second magnetic fields generated by the plurality of second coils and to tune the tuned coil Tuning to the load increases the power supplied to the load by the first plurality of coils.

Yet another embodiment relates to another system for providing power to a load. Department A first reactor comprising a first coil configured to generate a first magnetic field and at least one configured to generate a plurality of second magnetic fields and to change an intensity of one of the first magnetic fields The second coil. The system further includes a second reactor comprising at least one second reactor coil configured to tune the first reactor to a load. The system further includes a rectifier configured to receive AC output power at the output of at least one of the first reactor and the second reactor and to convert the AC output power to DC output power. The system further includes an output converter configured to synchronize the system with the load, wherein the output converter is further configured to receive DC output power to convert the DC output power to AC load power, The AC load power is supplied to the load. The first reactor is configured to provide electrical power to the load, and the second reactor is configured to increase the intensity of one of the plurality of second magnetic fields generated by the at least one second coil and to tune the first reactor The power supplied to the load by the first reactor is increased to the load.

1‧‧‧Excitation source

2‧‧‧Microprocessor-based power module (MPM)

3‧‧‧Resistance coil

3A‧‧‧Reactance coil

3B‧‧‧Reactance coil

3C‧‧‧Reactance coil

4‧‧‧Regeneration coil

4A‧‧‧Regeneration coil

4B‧‧‧Regeneration coil

4C‧‧‧Regeneration coil

5‧‧‧ Collector coil

5A‧‧‧ Collector coil

5B‧‧‧ Collector coil

5C‧‧‧ Collector coil

6‧‧‧Microprocessor-based control module (MCM)

8‧‧‧Control cable

10‧‧‧Control cable

11‧‧‧Hall Effect Current Sensor

12‧‧‧Regeneration coil

12A‧‧‧Regeneration coil

12B‧‧‧Regeneration coil

12C‧‧‧Regeneration coil

13‧‧‧Regeneration coil

13A‧‧‧Regeneration coil

13B‧‧‧Regeneration coil

13C‧‧‧Regeneration coil

14‧‧‧ Collector coil

14A‧‧‧ Collector coil

14B‧‧‧ Collector coil

14C‧‧‧ Collector coil

15‧‧‧terminal

16‧‧‧terminal

17‧‧‧ Terminal

18‧‧‧Microprocessor-based power module (MPM)

19‧‧‧ Terminal

20‧‧‧ terminals

21‧‧‧ terminals

22‧‧‧ Terminal

23‧‧‧Auxiliary Switching Module

24‧‧‧Auxiliary Switching Module

27‧‧‧Excitation current

28‧‧‧Reverse magnetic field

29‧‧‧Feedback current

30‧‧‧Reverse magnetic field

32‧‧‧Reactor

33‧‧‧Reactor

34‧‧‧ signal

35‧‧‧ terminals

100‧‧‧ system

102‧‧‧Directional (DC) power supply

105‧‧‧Converter

110‧‧‧Load disconnect switch (LBS)

115‧‧‧Reactor system

120‧‧‧Rectifier

125‧‧‧DC (DC) combiner terminal box

130‧‧‧Output converter

135‧‧‧load

200‧‧‧ system

202‧‧‧AC (AC) source

300‧‧‧Reactor system

305‧‧‧Main reactor

310‧‧‧Resonance reactor

315‧‧‧Neutral reactor

320‧‧‧Switch Module

325‧‧‧Regeneration coil

330‧‧‧ Collector coil

335‧‧‧Resistance coil

340‧‧‧First Resonant Reactor Coil

345‧‧‧Second resonant reactor coil

350‧‧‧Reactance coil

355‧‧‧Input power cord

360‧‧‧Rectifier

370‧‧‧Output power cord

400‧‧‧Program

405‧‧‧Steps

410‧‧‧Steps

415‧‧‧ steps

420‧‧ steps

1 is a block diagram of a system for supplying power to a load using a direct current (DC) power source, in accordance with an exemplary embodiment.

2 is a block diagram of a system for supplying power to a load using an alternating current (AC) power source, in accordance with an exemplary embodiment.

3 is a circuit diagram of one of the reactor systems that can be used to supply power to a load, in accordance with an illustrative embodiment.

4 is a flow diagram of one method for supplying power to a load using a reactor system, in accordance with an illustrative embodiment.

FIG. 5 is a block diagram of another system for supplying power to a load in accordance with another exemplary embodiment.

Figure 6 is a circuit diagram of a single phase, two stage reactor assembly in accordance with an exemplary embodiment.

Figure 7 is a diagram of a single phase, two stage reactor as shown in Figure 6 in accordance with an exemplary embodiment. One of the single-level circuit diagrams.

Figure 8 is a circuit diagram of a single phase, single stage reactor assembly in accordance with an illustrative embodiment.

Figure 9 is a circuit diagram of a single stage of one of a three phase, two stage reactor assembly, in accordance with an illustrative embodiment.

Figure 10 is an illustration of one of the reactor assemblies having a coil wound around a two-column R-core according to an exemplary embodiment.

Figure 11 is an illustration of one of the reactor assemblies having a coil wound around a three-column R-core according to an exemplary embodiment.

Figure 12 is an illustration of one of the reactor assemblies having a coil wound around a toroidal core, in accordance with an illustrative embodiment.

The present disclosure is directed to systems and methods that can be used to provide power to a load using electromagnetic induction. A system according to some embodiments of the present disclosure may comprise at least two reactors. A primary reactor can be configured to receive excitation power from an excitation source, such as a wind or solar source or one or more batteries, and provide power to drive a load (eg, a grid, a motor, etc.) . A resonant reactor can be coupled to the main reactor and to the load and can be configured to resonate the main reactor with the load. The main reactor can include a regenerative coil configured to receive an excitation current and generate a magnetic field. The primary reactor may also include two or more reactive coils configured to generate a magnetic field and change the strength of the magnetic field generated by the regenerative coil (eg, causing expansion and contraction). The primary reactor may also include a collector coil magnetically coupled to the regeneration coil and configured to generate an opposite magnetic field. The resonant reactor can use a collector coil to automatically tune the main reactor (eg, the regenerative coil) to the load. The resonant reactor may comprise two coils magnetically coupled to each other, one of the two coils being connectable to one of the reactance coils of the main reactor and to the load, and the other of the two coils may be shunted to the main The collector coil of the reactor.

In some embodiments, the system can include an output converter configured to synchronize the system to a load or grid and draw output power to a load or grid (eg, a distribution grid). The adjustment of the system can be controlled by a smart output converter. The smart converter output power can be determined based on one of the maximum design capacity and/or parameters of the reactor. In some embodiments, the smart converter can limit the power transmitted to the grid based on program parameters. In some embodiments, the smart converter can be programmed to operate at one of 50 Hz and/or 60 Hz or another frequency, and/or can be adapted to the specific load requirements of the grid. In some embodiments, the smart converter output can be limited by a maximum output capacity.

Some components of the two reactors may be physically connected to each other, and the system may be configured to operate in conjunction with any voltage and/or frequency load (eg, high or low voltage/frequency load). In some embodiments, system parameters, such as the maximum temperature of a particular component, can be adjusted by the system.

Referring now to Figure 1, a block diagram of a system 100 for providing power to a load 135 is shown in accordance with an illustrative embodiment. System 100 is configured to receive power from a direct current (DC) power source 102 (such as one or more batteries, a solar panel, etc.) and use the power as excitation power for a reactor system 115. The received DC power can be converted to alternating current (AC) power using a converter 105. In some embodiments, the converter 105 has a pure sine wave output power and is grid compatible (e.g., operating at the same frequency as one of the grids to which it is connected). In some embodiments, the converter 105 can be a smart converter and can generate/regulate voltage, frequency, and/or current with the ability to synchronize with the grid. The AC input power may be received by a load disconnect switch (LBS) 110 configured to allow input power to be selectively coupled to and/or disconnected from the reactor system 115. In some embodiments (eg, when a solar panel is used to provide excitation energy), the LBS 110 can sense that the output converter 130 has its power synchronized with the grid and can automatically draw power from the excitation source to the output. The output power of the streamer 130.

The AC input power is then provided to the reactor system 115 and used as the excitation current for the plurality of coils of the reactor system 115. Reactor system 115 can be configured to utilize the slave load The electrical energy of the electromagnetic field generated by 135 and/or other sources of electromagnetic radiation (eg, environmental sources). Reactor system 115 can include a primary reactor configured to receive input power and generate a magnetic field using a first coil (eg, a regenerative coil). Two or more other coils (eg, reactance coils) of the primary reactor may be configured to vary the intensity of one of the magnetic fields generated by the first coil. Reactor system 115 may also include a resonance reaction configured to resonate the main reactor with load 135 (e.g., to tune the main reactor to a resonant frequency that is approximately the same as one of the electromagnetic fields generated by load 135). Device. The resonant reactor can also cause an increase in the strength of the magnetic field generated by the reactance coil, thereby causing an increase in the strength of the varying magnetic field generated by the regenerative coil. The variation in the magnetic field can be related to the magnitude of one of the connected loads 135. Reactor system 115 is described in further detail below with respect to FIG. 3 in a detailed embodiment.

The output of reactor system 115 can be provided to a rectifier 120 that can convert the AC output of reactor system 115 to a DC output. The DC output can be received by a DC combiner terminal box 125 (e.g., to combine the outputs of several reactor systems). In some embodiments, in the case of multiple parallel reactor systems, the DC combiner terminal box 125 can balance the voltage outputs of the various reactor systems connected in parallel, thereby enabling load current balancing by each reactor system .

The output of the box 125 can be provided to an output converter 130. Output converter 130 is configured to synchronize reactor system 115 with load 135. Output converter 130 is further configured to convert DC output power to AC power for use by the load and to transmit AC power to the load. In some embodiments, the output converter 130 can be configured to feed a portion of the AC output power back into the reactor system 115 (eg, to compensate for system losses and/or to ensure that the magnetic force in the reactor system 115 can be maintained) ). In some embodiments, output converter 130 can be a smart grid converter that is configured to synchronize with a grid. The output converter 130 can be composed of several modules (eg, five modules) connected in parallel. In some embodiments, a module can operate as a master module, and other modules can operate as slave modules whose operating parameters are controlled by the master module. The main control module can contain the load according to the load or the distribution network. A programmable load management software system that automatically adjusts the parameters of each slave module. In some embodiments, output converter 130 can be configured to generate its own voltage source, current source, and/or frequency source. Output converter 130 may be capable of powering one of the connected systems or operating in synchronization with the grid. In some embodiments, output converter 130 can operate in an off-network mode and/or in synchronization with other output converters connected within the same network. In some embodiments, the output converter 130 can seamlessly switch between a grid-connected mode and an off-net mode without interruption. In some embodiments, the output converter 130 can be synchronized with other converters in the system (eg, during off-grid mode) and/or when the grid or network fails when in the grid-connected mode A source reference (for example, voltage and / or frequency).

Referring now to FIG. 2, a block diagram of a system 200 that can be used to provide power to a load 135 is shown in accordance with an illustrative embodiment. System 200 includes the same components as system 100, and similar components in both systems can function in a similar manner. System 200 is configured to receive excitation energy from an AC source 202 rather than a DC source. Accordingly, the input power need not be inverted for use by the reactor system 115 in the system 200.

Referring now to Figure 3, a circuit diagram of one of the reactor systems 300 that can be used to supply power to a load is shown in accordance with an illustrative embodiment. Reactor system 300 can be an embodiment of reactor system 115 shown in Figures 1 and 2 in accordance with an illustrative embodiment. In the illustrated embodiment, the three-phase AC excitation current is received via input power line 355. Each set of input power lines 355 can be coupled to two sets of reactor modules through a switching module 320, including a main reactor 305 and a resonant reactor 310. The output AC power is provided to a rectifier 360 that converts the AC power to DC output power that is transmitted via the output power line 370. Although the reactor system 300 is shown as having six sets of reactor modules for simplicity, the function of a single set of reactor modules will be described below.

Different settings and stylization of parameters of the reactor system 300 and/or other components of the overall power supply system can be performed prior to the components of the reactor system 300 being energized. E.g, Parameters may be provided to allow an output converter to synchronize with a grid or other load and/or draw output power to the load. The output converter can be programmed according to parameters associated with the grid or other loads. For example, such parameters may include the frequency range, voltage range, correct phase sequence, etc. of the grid to be synchronized with the output converter. In some embodiments, a protection system can be programmed (eg, fault protection, overvoltage protection and/or undervoltage protection, overfrequency protection and/or underfrequency protection, maximum voltage and/or current of the converter output) Wait). In some embodiments, a programmable load management system built into the system can manage operational parameters of individual modules within the converter system (eg, in the case of multiple modules).

Once the initial stylization and setup has been completed, the load disconnect switch can be activated and the components of the reactor system 300 can be energized. Switching module 320 receives input power from input power line 355. A neutral reactor 315 can also receive power from input power line 355 and/or switching module 320. Neutral reactor 315 can be used to feed excess power back into input power line 355 when it is not immediately available to the reactor modules of the group. One of the main reactors 305, the regeneration coil 325, is energized. The regenerative coil 325 is shunted between one of the terminals of a reactance coil 335 and one of the neutral points of the neutral reactor 315. Reactance coil 335 is then energized, which is coupled to an excitation source (e.g., through regenerative coil 325) and to one of first resonant reactor coils 340 of resonant reactor 310. The collector coil 330 shunted to a second resonant reactor coil 345 and magnetically coupled to the regenerative coil 325 is also energized. The first resonant reactor coil 340 is energized (eg, through the reactance coil 335). The first resonant reactor coil 340 is connected in series with the reactance coil 335 and is directly connected to one of the terminals of a rectifier 360. The second resonant reactor coil 345, shunted to the collector coil 330 and magnetically coupled to the first resonant reactor coil 340, is energized. A reactance coil 350 magnetically coupled to the regenerative coil 325 and directly connected to one of the terminals of a rectifier 360 is also energized. Reactance coil 335 is also magnetically coupled to regenerative coil 325.

The output converter can be programmed similarly to the excitation converter and activated to synchronize with the grid or other load and feed power to the grid or other load. In the output converter After synchronizing with the grid, a current of a certain magnitude will flow through the components of system 300. The magnitude of the current can be proportional to the magnitude of the connected load. The current flowing through the regenerative coil 325 causes the regenerative coil 325 to generate a first magnetic field. The current flowing through the reactance coil 335 causes the reactance coil 335 to generate a second magnetic field, and the reactance coil 335 is configured to expand (eg, increase) the first magnetic field generated by the regenerative coil 325 based on the output load of the converter. One of its strengths changes the strength of the magnetic field generated by the regenerative coil 325. The current flowing through the reactance coil 350 causes the reactance coil 350 to generate a third magnetic field, and the reactance coil 350 is configured to reduce the first magnetic field generated by the regenerative coil 325 based on the output load of the converter (eg, reduce it) One of the ways to change the strength of the magnetic field generated by the regenerative coil 325.

The current flowing in the reactance coil 335 having the polarity of the reference regenerative coil 325 configuration and the coil winding direction produces a higher magnetic field than the magnetic field generated by the regenerative coil 325. The current flowing in the reactance coil 350 having the polarity of the reference regenerative coil 325 configuration and the coil winding direction produces a magnetic field that is weaker than the magnetic field generated by the regenerative coil 325. When the rotor is combined with a DC excitation rotation (the north magnetic pole and the south magnetic pole are generated on the rotor), the effect of the strongening and weakening magnetic field in the regenerative coil 325 simulates the expansion and contraction of the magnetic field in the stator winding of a generator. Since the output load of the converter increases, the current and voltage generated by the resonant reactor coil 345 (eg, the ratio of the current drawn by the load is one to one or slightly higher) is coupled to the magnetic coupling to the regenerative coil. The collector coil 330 of 325 is induced to resonate. This energy induced by the resonant reactor coil 345 maintains and tunes the magnetic field strength of the regenerative coil 325 to any given specific load.

A current on the first resonant reactor coil 340 produces a fourth magnetic field that is inductively magnetically coupled to one of the second resonant reactor coils 345 of the first resonant reactor coil 340. In some embodiments, the first resonant reactor coil 340 and the second resonant reactor coil 345 can be designed to be substantially identical (eg, the same material, the same number of turns, etc.). Due to the initial excitation from the excitation source, the voltage drop across the second resonant reactor coil 345 can be slightly higher than the cross The initial voltage drop of the regenerative coil 325, and a current substantially equivalent to the magnitude of the current flowing through one of the reactance coils 335 and 350, may flow through the collector coil 330, which may generate another magnetic field and induce Magnetically coupled to one of the regenerative coils 325 of the collector coil 330. Thus, the resonant reactor 310 can take over as an excitation source, or supplement the excitation source, and can resonate the main reactor 305 with a load connected to the system.

In some embodiments, the regeneration coil 325 can collect more current than the current that can be collected by the reactance coil 335 and delivered to the rectifier 360 for transmission to the load (eg, via induction from the resonant reactor 310). In some such embodiments, the regeneration coil 325 can transfer excess energy back to a neutral reactor 315. Neutral reactor 315 can deliver energy back to input power line 355 (e.g., in a feedback loop) to prevent energy from being lost as waste energy. In some embodiments, the neutral reactor 315 can be a zigzag three-phase transformer designed according to a specific voltage of the excitation source (eg, equal to the voltage output by the output converter) and excess extraction current generated by the regeneration coil 325. . Excess current on the regenerative coil 325 can flow through the neutral point to the neutral point of the neutral reactor 315. The current flowing from the neutral point of the neutral reactor 315 can be induced to the three-phase excitation source via the three-phase zigzag winding of the neutral reactor 315. In some embodiments, to help ensure that the magnetic force in the main reactor 305 and/or the resonant reactor 310 is maintained and/or compensates for system losses, one of the feedback circuits from the output converter can be used to supply a portion of the output power back to Inspire the input.

Referring now to FIG. 4, a flow diagram of a program 400 for providing power to a load (e.g., using a system, such as systems 100, 200, and/or 300) is shown in accordance with an illustrative embodiment. A reactor system can receive excitation energy from a power source (405). The excitation energy can be used to excite one or more coils of a first reactor to produce a first magnetic field (410). In some embodiments, the first reactor can include a coil configured to change (eg, expand and/or contract) the magnetic field. A second reactor can be energized and can be configured to resonate (415) the coil of the first reactor with one of the outputs connected to the second reactor. In some embodiments, the second reactor can be configured to be produced by the first reactor, for example by modification The magnetic field is expanded and/or reduced by the strength of the magnetic field generated by the coil of the first reactor to change the magnetic field generated by the first reactor (e.g., increase its intensity) (420).

Some embodiments of the present disclosure, such as illustrated in Figures 5 through 12, relate to one of the high energy efficiency output regenerative electromagnetic energy flux reactors (EERs). Such embodiments may utilize an alternating current power source as an excitation to generate electromagnetic interaction with the reactor assembly, the reactor assembly being operable to regenerate electromagnetic energy induced by a reactive coil to one or more regenerative coils and may be directly An electrical load connection coupled to the output of one or more collector coils. The maximum load of the collector coil can be determined by referring to the ratio of the reactance coil to the regenerative coil. For stable performance and maximum energy regeneration at the regenerative coil, the collector coil can be an independent and distinct reactive reactor coil assembly (eg, a resonant reactor) (connected to one of the main assembly's reactance coil outputs) ) Automatic tuning.

In some embodiments, the EER can be one or more microprocessor-based power modules (MPMs), one-stage, two-stage or two-stage reactor systems including one of three (3) or more coils (RS), a microprocessor-based control board (MCB) and one or more Hall Effect current sensors (HECS). For example, the system can be configured as a cascading system in which the output of the first EER can be used as one of the second largest EER excitation sources. For example, a 100 kW EER can be used as an excitation source for a 1 MW EER. Once the two EERs are running, they can be synchronized with the grid to produce an output with a total of 1.1 MW. The increased efficiency of the output can be dictated by the electrical load of the reactance coil assembly connected to the direct coupling or via one of the voltage outputs that regulate the EER. The EMF and the current flowing on the reactance coil induce electromagnetic energy on the regenerative coil that produces a magnetic field on the reactor core opposite the magnetic field generated by the regenerative coil itself (when excited by an excitation source). The opposite magnetic field in the regenerative circuit applies pressure to the atoms in the system to bring them into a coherent state. The coherent state of the atoms causes the electron flow between the atoms to continue to be exchanged by magnetic induction in the reactor system. Since electrons are hardly flowable in the atmosphere due to the high resistance of different kinds of gases, they will be attracted to flow on the surface of the conductor with less resistance. according to In some embodiments, in the EER, the less resistive conductor can be a regenerative coil and a reactive coil that causes electrons to be attracted to the conductors. As the electrical load on the reactive circuit (eg, the reactance coil) increases, the magnitude of the electromagnetic energy in the regenerative circuit (eg, the regenerative coil) increases proportionally and the efficiency of delivery to the output of the electrical load also increases. An increase in the electrical load capacity of the collector coil is also achieved. The collector coil can be independently loaded but can be tuned according to the transformation ratio of one of the reactance coil and the regenerative coil. The collector coil can also be excited by a dissimilar reactive (e.g., resonant) reactor that is independently tuned by one of the output reactance coils that are independent of the main reactor and connected to the main reactor assembly. The HECS monitors the operating parameters of the resonant reactor and initiates and deactivates the starting system when it is within preset operating parameters or exceeds preset operating parameters. During the withdrawal of the startup process, the system will automatically transfer to a bypass mode. In the bypass mode, the reactor may be shut down due to overload and a bypass circuit may be connected to connect the load directly to an alternate source. The bypass mode can be eliminated when the HECS identifies that the load is within the normal parameters of the reactor. One of the maximum load capacity of the reactive circuit, the regenerative circuit, and the collector circuit can be limited by one design factor and current rating of the conductor coil. To maximize design output ratio efficiency, a second stage reactor can be integrated to regulate the desired voltage output of the electrical load. In some embodiments, the smallest of the two reactance coils can be used to provide high intensity electromagnetic energy sensing of the regenerative coil. The core of the EER can be made of a film material. The reactor system core can be made of a high-grade silicon steel sheet configured in a grain orientation. The thickness of the grain oriented silicon steel sheet can be the thinnest available product size for better performance and efficiency. The stack depth of the core regions can be based on the maximum depth calculated by the design to maximize the Casimir effect on the laminated laminate. The copper conductor can be 99.99% oxygen-free and wound on a core to create a reactive coil, a regenerative coil, and a collector coil. The reactance coil, the regenerative coil, and the collector coil may be wound on the same strut of each reactor core independently or together. The reactance coil, the regenerative coil and the collector coil may be made of a copper magnet wire which can be 99.9% oxygen-free rectangular or circular cross section. MPM and MCM can withstand a temperature rise of 65 degrees Celsius. The structure of the reactor core can be a two-column R-core or a three-column R-core.

Referring now to Figure 5, a block diagram of another system for supplying power to a load is shown in accordance with an illustrative embodiment. The system of Figure 5 includes an excitation source 1 that is used as a microprocessor-based power module (MPM) 2 and 18, a microprocessor-based control module (MCM) 6 and in a bypass mode. Reactors 32 and 33 for power. The microprocessor-based power modules 2 and 18 drive the control circuits of the auxiliary switching modules 24 and 23, as shown in FIG. The microprocessor based power modules 2 and 18 are controlled and actuated by the microprocessor based control module 6 based on a signal received from the Hall effect current sensor 11. In the embodiment shown in FIG. 6, the excitation source 1 supplies the power requirements of the microprocessor based power modules 2 and 18 and the microprocessor based control module 6.

At zero electrical load at terminal 15, Hall effect current sensor 11 senses zero current and sends a signal to microprocessor based control module 6. The microprocessor based control module 6 will process and actuate the signal and relay the processed signals to the microprocessor based power modules 2 and 18 via control cables 8 and 10, as shown in FIG. The microprocessor based power modules 2 and 18 will deactivate the start up reactors 32 and 33.

In the embodiment shown in FIG. 9, the excitation source 1 supplies power to the microprocessor based power modules 2 and 18 and the microprocessor based control module 6. At zero voltage loads at terminals 15, 16, and 19, Hall effect current sensor 11 senses zero current and sends a signal to microprocessor based control module 6. The microprocessor based control module 6 will process the signal and actuate the processing signal to the microprocessor based power modules 2 and 18. The microprocessor based power modules 2 and 18 will process the received signals and activate the auxiliary switching modules 24 and 23. The auxiliary switching modules 24 and 23 will deactivate the reactors 32 and 33.

When switching one of the terminals 15 (in FIG. 6) and/or terminals 15, 16, and 19 (in FIG. 9), the Hall effect current sensor 11 will send a signal 34 to the microprocessor based control module. 6. The microprocessor based control module 6 will receive and process the signal 34 transmitted by the Hall effect current sensor 11. If the signal 34 sent by the Hall effect current sensor 11 is equal to or greater than the preset minimum current trigger signal, the microprocessor based control module 6 will relay the The signals are processed to the microprocessor based power modules 2 and 18. In the embodiment shown in FIG. 6, microprocessor based power modules 2 and 18 will activate reactors 32 and 33. In the embodiment shown in FIG. 9, microprocessor based power modules 2 and 18 will relay the processed signals to auxiliary switching modules 24 and 23. The auxiliary switching modules 24 and 23 will deactivate the bypass mode and simultaneously activate the reactors 32 and 33.

When the reactors 32 and 33 are energized, an electromagnetic energy and a magnetic field of opposite directions are generated at the regenerative coil 4 (as in FIG. 6) or the regenerative coils 4A, 4B and 4C (as in FIG. 8) and a reverse diamagnetic field 28 is generated. An excitation current 27 (see Figure 10). A current at the reactance coil 3 (as in FIG. 6) or the reactance coils 3A, 3B, and 3C (as in FIG. 9) is generated almost simultaneously on the regenerative coil 4 (as in FIG. 6) or the regenerative coils 4A, 4B, and 4C (eg, One of the feedback currents 29 in FIG. 9 and one of the inverse counter magnetic fields 30 (as shown in FIG. 10) is exactly opposite to the magnetic field 28.

In the embodiment shown in Figures 6 and 9, the excitation current 27 and the feedback current 29 (as shown in Figure 10) collide, thereby pressurizing the atoms in the system to co-enter each other. The cohesive state of the atoms causes an exchange of electrons between the atoms, resulting in a continuous flow of electrons in the regenerative coil and consumed by the electrical load. Since electrons are hardly able to flow in space due to the high resistance of gases in the atmosphere, they are attracted to one of the lesser paths. In the exemplary EER shown in FIGS. 5 to 10, the reactance coil 3 and the regenerative coil 4 (as in FIG. 6), and the reactance coils 3A, 3B, and 3C and the regenerative coils 4A, 4B, and 4C (as shown in FIG. 9) It is a circuit with less resistance and electrons will be attracted to its conductor coil. As long as the excitation source 1 continues to supply the required excitation voltage and current, the cohesion of the atoms passing through the magnetic induction will continue. Collector coil 5 (as in Figure 6) or collector coils 5A, 5B and 5C (as in Figure 9) will be electrically loaded to increase regenerative coil 4 (as in Figure 6) or regenerative coils 4A, 4B and 4C The intensity of the inverse diamagnetic field 28 in (as in Figure 9) and the current in the reactance coil 3 (as in Figure 6) or in the reactance coils 3A, 3B and 3C (as in Figure 9). This is to maintain or increase the atomic cohesive strength produced in the reactor system. When the magnetic field expands/strengths, the atoms expand, and they may need to attract electrons in the near field to fill or fill the holes, thereby converting this atom into a basic state (receiving electrons). When the magnetic field is closed When shrinking/weakening, the atom then shrinks, and this forces the atom to release an electron, thereby converting the atom into a transitional state (eg, transmitting electrons). The rate at which electrons are transferred from one atom to another can be referred to as atomic cohesive strength. Once there is an electron flow, it may be necessary to maintain a (strong/weakened) magnetic field that varies with respect to a particular magnitude of the load.

The microprocessor-based power module 18 controls and adjusts the reactor 33 via the auxiliary switching module 23 with respect to the regenerative coils 12 and 13 (as in FIG. 6) and the regenerative coils 12A, 12B, 12C and 13A, 13B, 13C ( As shown in Fig. 9), the voltages outputted at terminals 15, 16 and 17 (as in Fig. 6) and 15, 16, 19, 20, 21 and 22 (as in Fig. 9) are adjusted. In some embodiments, this can be a multi-joint design, and once the module senses that the voltage is above or below a preset value, it can be programmed to adjust the joint. In some embodiments, the output converter can regulate the voltage output. The inter-line single-phase output system terminals 15 and 16 of the embodiment shown in Fig. 6, the line-to-ground terminals 15 and 35, 16 and 35, and 17 and 35. The three-phase output terminals of the embodiment shown in Fig. 9 are 15, 16, 19 and 20, 21, 22, respectively. Collector coils 14 (as in Figure 6) or collector coils 14A, 14B, and 14C (as in Figure 9) are used to maximize the output load of the reactor system. Two loads can be connected to the system (eg, primary and secondary loads). The primary load can be directly connected to the output of the reactance coil, and the secondary load can be directly connected to the collector coil. The primary load can be configured to create a contracted magnetic field on the regenerative coil, and the load on the collector coil can be configured to produce a strong magnetic field on the regenerative coil. An independent and distinct reactive reactor coil assembly can be introduced to excite the collector coil for self-tuning rather than loading it with an electrical load. The reactive reactor coil assembly is coupled to one of the outputs of the primary reactor reactance coil.

In some embodiments, an EER assembly can include an external exciter input source (eg, a utility grid, a power generation device such as a hydroelectric generator, a thermal generator, a nuclear power generator and a geothermal generator, a wind turbine, Fuel cell generators, solar power and tidal power generation). The assembly can further include one or more auxiliary switching modules that revoke the start-up and start-up reactor. The system can be a single or dual level system and/or can be a single stage or Three-level system. The assembly can further include a microprocessor based power module that controls one of the auxiliary switching modules and a microprocessor based control module that processes the signals fed by the Hall effect current sensor. The assembly can include a Hall effect current sensor that senses the output current of the output electrical load of the system. The assembly may further comprise one or more systems of electromagnetic reactors (eg, single or two stages) and may include the following coils: (1) a reactive inductive coil for receiving electrical energy and sensing a regenerative coil One of the opposite magnetic fields; (2) a regenerative inductive coil that absorbs electromagnetic energy and a magnetic field induced by the reactance coil and produces a magnetic field opposite to the direction of the magnetic field induced by the reactance coil when excited by an external source; (3) a set of pole inductors configured to be independently loaded by an electrical load tuned to the ratio of the reactance coil to the regenerative coil and/or to be connected to a separate and distinct reactive/resonant reactor (connected to a One of the main reactor reactance coils outputs an excitation to automatically tune the main reactor without increasing the intensity of a magnetic field generated by the regenerative coil when connected to an external electrical load connected to the collector coil; (4) an independent An inductive reactor assembly that induces an excitation current and voltage to a collector coil of the main reactor to increase a magnetic field at a regenerative coil of the main reactor and/or to automatically modulate the main reactor assembly; and/or (5) a compensation reactor for The section of the output voltage system.

In some embodiments, the microprocessor based control module receives signals from the Hall effect current sensor, processes the signals, activates the microprocessor based power module, and relays the processed signals to cancel the startup. Either initiating a reactor system (eg, in the embodiment of FIG. 6), or controlling the operation of the auxiliary switching module to based on signals processed by the microprocessor-based control module from the Hall effect current sensor and The processed signal is relayed to the microprocessor based power module to deactivate or start the reactor system (e.g., in the embodiment of FIG. 9).

In some embodiments, the EER can be configured to undo the start-up reactor once the level of the current at the output or load side sensed by the Hall effect current sensor drops below the preset minimum current signal. system. The EER can be configured to sense that the Hall effect current sensor is greater than a minimum preset current signal and less than or equal to one of the maximum preset current signals The current starts the reactor system. In some embodiments, the EER can be configured to undo the start-up reactor once the Hall effect current sensor senses a current signal that is greater than one of the maximum preset current level signals and/or switches the system into a bypass mode system.

In some embodiments, the EER can be loaded when the regenerative circuit/coil is loaded at the output terminals of the reactance coil and/or the collector coil and/or the collector coil is comprised of a separate dissimilar reactive reactor assembly. When excited for self-tuning, two opposing magnetic fields are generated at the regenerative circuits/coils, resulting in an increase in the strength of the opposing magnetic field and a current collision, forcing the atoms in the system to cohesive. The cohesive procedure enables electron exchange between the atoms, resulting in continuous flow of electrons through the reactance coil and the regenerative coil and as long as the regenerative coil is excited to be absorbed by the connected electrical load.

In some embodiments, the EER can comprise only a single reactor assembly. In some such embodiments, the output and collector coils can be loaded separately.

In some embodiments, the EER can utilize electromagnetic induction to regenerate a significant amount at the regenerative coil using induced EMF and current in the reactance coil generated by the increased magnetic field strength at the regenerative circuit and the tuned load of the collector coil. The energy of the value. The amount of regenerative energy at the regenerative coil may be based on the ratio of the reactance coil to the regenerative coil and/or one of the regenerative coil to the reactance coil (eg, turns ratio).

In some embodiments, the EER can utilize electromagnetic induction theory to pass the induced EMF and current in the reactance coil and by an independent and distinct reactive/resonant reactor assembly (connected to one of the outputs of the reactive circuit) The excitation of the collector coil regenerates a considerable amount of energy at the regenerative coil. The excitation of the independent and distinct reactor assembly increases the strength of the opposing magnetic field induced by the reactive coil of the primary reactor at the regeneration circuit. The reactive/resonant reactor assembly can be configured to automatically tune the main reactor assembly to a load connected to one of the reactive/resonant reactor assemblies. The amount of regenerative energy at the regenerative coil may be based on the ratio of the reactance coil to the regenerative coil and/or one of the regenerative coil to the reactance coil (eg, turns ratio).

In some embodiments, when an AC power source is installed and energizes the EER, The EER can regenerate a significant amount of energy based on the ratio of the reactance coil to the regenerative coil and/or one of the regenerative coil and the collector coil. In some embodiments, the energy can be delivered to an AC load group (eg, a resistive or inductive AC load and/or a rectifier assembly to convert to DC).

In some embodiments, the EER can receive excitation energy from a DC source through a converter. The DC source can include renewable energy sources such as wind, solar, fuel cells, and/or other forms of DC sources (eg, batteries/batteries). In some embodiments, the EER can be configured to output energy to an AC load group (eg, a resistive or inductive AC load and/or a rectifier assembly to convert to DC) in an AC waveform. EER can regenerate a considerable amount of energy. In some embodiments, the regenerative energy may be based on a ratio of the reactive coil to the regenerative coil and/or one of the regenerative coil and the collector coil.

In some embodiments, the EER aspect can operate according to the following exemplary formula:

P(in) - power input to EER

P(out) - the power that is output to and consumed by the electrical load

P(reg)-regeneration circuit regenerative power

P (rea) - the power sensed by the reactive circuit to the regenerative circuit

P(rea-sr) - power consumed by an independent and distinct reactor in exciting the collector coil of the main assembly

P(sys) - power consumed by system losses

N (rea) - the number of turns of the reactance coil

N(reg)-number of turns of the regenerative coil

Number of turns of N(col)-collector coil

Number of N (rea-sr)-independent reactive reactor

Load current of I(L)-EER connected load

p.f.-EER connected load power factor

V (rea) - voltage drop at the reactance coil

V(rea-sr)-voltage drop at the reactance coil of the independent reactive reactor

Note: The voltage of each main reactor and each independent and distinct reactive reactor assembly can be the same.

The disclosure is described above with reference to the drawings. The drawings illustrate specific details of specific embodiments of the systems and methods and programs that implement the present disclosure. However, the disclosure of the present disclosure is not to be construed as imposing any limitation to the present disclosure. The present disclosure contemplates methods, systems, and/or program products on any machine readable medium for performing the operations thereof. Embodiments of the present disclosure may be implemented using a conventional computer processor, or a dedicated computer processor incorporated for this purpose or another purpose, or by a fixed line system. Any type of processor (eg, FPGA, ASIC, ASIP, CPLD, SDS, etc.) can be used. The claimed components should not be construed in accordance with the provisions of paragraph 6 of 35 U.S.C. § 112, unless the component is explicitly stated in the phrase "components of". In addition, the elements, components, or method steps in the present disclosure are not intended to be dedicated to the full text, regardless of whether the elements, components, or method steps are explicitly recited in the claims.

As mentioned above, embodiments within the scope of the present disclosure may comprise a program product comprising a machine for executing a machine executable instruction or data structure stored thereon or having a machine executable instruction or data structure stored thereon. Read the storage media. The machine-readable storage medium can be any available media that can be accessed by a general purpose or special purpose computer or other machine. For example, the machine-readable storage medium can include RAM, ROM, EPROM, EEPROM, CD ROM or other optical disk storage device, disk storage device or other magnetic storage device, or any other medium that can be used to implement or store Machine can be executed The form of a line of instructions or data structure and which may be accessed by a general purpose or special purpose computer or other machine. Combinations of the above devices are also included within the scope of machine readable storage media. A machine-readable storage medium contains non-transitory media but does not contain purely transitory media (ie, spatial signals). Machine-executable instructions include, for example, instructions and materials that cause a general purpose computer, special purpose computer, or special purpose processing machine to perform a particular function or group of functions.

It should be noted that although the flowcharts provided herein show a particular order of method steps, it should be understood that the order of the steps may be different from the order of the description. Also, two or more steps may be performed simultaneously or partially simultaneously. This change will depend on the software and hardware system chosen and the designer's choice. It should be understood that all such variations are within the scope of the present disclosure. Similarly, the software and web page implementations of the present disclosure can be accomplished using standard stylization techniques in conjunction with rule-based logic and other logic to accomplish different database search steps, association steps, comparison steps, and decision steps. It should also be noted that the words "component" as used herein and in the scope of the claims are intended to cover embodiments using one or more lines of software code, and/or hardware embodiments, and/or devices for receiving manual input. .

The previous description of the embodiments of the present disclosure has been presented for purposes of illustration and description. The previous description is not intended to be exhaustive or to limit the scope of the disclosure. The embodiments were chosen and described in order to explain the principles of the invention,

Claims (20)

A system for providing electrical power to a load, comprising: a first reactor including a first coil configured to generate a first magnetic field and configured to generate a plurality of second magnetic fields and to change At least one second coil of one strength of the first magnetic field; and a second reactor comprising at least one second reactor coil configured to tune the first reactor to the load; wherein the first The reactor is configured to provide the electrical power to the load, and wherein the second reactor is configured to increase the intensity of one of the plurality of second magnetic fields generated by the at least one second coil and The first reactor is tuned to the load to increase the power supplied to the load by the first reactor. The system of claim 1, wherein the at least one second reactor coil comprises: a third coil connected to the first reactor and to the load; a fourth coil magnetically coupled to the third coil; Wherein the first reactor includes a fifth coil, and wherein the fourth coil of the second reactor is split to the fifth coil of the first reactor, and wherein the second reactor is configured to The fifth coil of the first reactor is tuned to the load. The system of claim 2, wherein the first coil is configured to generate an AC current in response to a third magnetic field generated by the load, wherein the first coil is coupled to the second reactor and the fifth The coil is tuned to the load. The system of claim 1, further comprising a third reactor configured to receive excess energy from the first reactor and feed the excess energy back to the first reactor Input in. A system as claimed in claim 1, further comprising an input converter configured to receive power from a DC power source and convert the power to AC power Used as excitation energy for at least one of the first reactor and the second reactor. The system of claim 1, further comprising a rectifier configured to receive AC output power at an output of at least one of the first reactor and the second reactor and to convert the AC output power DC output power. The system of claim 6, wherein the load comprises one of a grid or a distribution grid, and wherein the system further comprises a converter configured to synchronize the system with the load, wherein the converter Further configured to receive the DC output power, convert the DC output power to AC load power, and provide the AC load power to the load. A system for providing power to a load, comprising: a first plurality of coils, wherein a first coil of the first plurality of coils is configured to generate a first magnetic field, and wherein the first plurality of coils a plurality of second coils of the coil configured to generate a plurality of second magnetic fields and varying one of the first magnetic fields; and a second plurality of coils, wherein the second plurality of coils are configured to the first plurality At least one of the coils is tuned to the load via a tuning coil; wherein the first plurality of coils are configured to provide the power to the load, and wherein the second plurality of coils are configured to be increased by the plurality The intensity of one of the plurality of second magnetic fields generated by the second coils and tuning the tuned coil to the load increases the power supplied to the load by the first plurality of coils. The system of claim 8, wherein the second plurality of coils comprises: a third coil coupled to one of the plurality of first coils and to the load; and a fourth coil magnetically coupled to the first a third coil; wherein the first plurality of coils includes a fifth coil, and wherein the fourth coil is shunted to the fifth coil, and wherein the fourth coil is configured to the fifth coil Tune to this load. The system of claim 9, wherein the first coil is configured to generate an AC current in response to a third magnetic field generated by the load, wherein the first coil is coupled to the second plurality of coils and the first coil Five coils are tuned to the load. The system of claim 8, further comprising a reactor configured to receive excess energy from the first coil and feed the excess energy back into one of the first plurality of coil inputs. The system of claim 8, further comprising an input converter configured to receive power from a DC power source and convert the power to AC power for use as the first plurality of coils One of the second plurality of coils excites energy. The system of claim 8, further comprising a rectifier configured to receive AC output power at an output of at least one of the first plurality of coils and the second plurality of coils and to output the AC Power is converted to DC output power. The system of claim 13, wherein the load comprises one of a grid or a distribution grid, and wherein the system further comprises a converter configured to synchronize the system with the load, wherein the converter Further configured to receive the DC output power, convert the DC output power to AC load power, and provide the AC load power to the load. A system for providing electrical power to a load, comprising: a first reactor including a first coil configured to generate a first magnetic field and configured to generate a plurality of second magnetic fields and to change At least one second coil of one strength of the first magnetic field; a second reactor comprising at least one second reactor coil configured to tune the first reactor to the load; a rectifier configured to receive AC output power at an output of at least one of the first reactor and the second reactor and convert the AC output power to DC output power; and an output converter Configuring the system to synchronize the system with the load, wherein the output converter is further configured to receive the DC output power, convert the DC output power to AC output power, and provide the AC output power to The load; wherein the first reactor is configured to provide the power to the load, and the second reactor is configured to increase the plurality of second magnetic fields generated by the at least one second coil One of the strengths and tuning the first reactor to the load increases the power supplied to the load by the first reactor. The system of claim 15 wherein the at least one second reactor coil comprises: a third coil coupled to one of the plurality of first coils and to the load; and a fourth coil magnetically coupled to The third coil; wherein the first reactor includes a fifth coil, and wherein the fourth coil of the second reactor is branched to the fifth coil of the first reactor, and wherein the second reactor passes Configured to tune the fifth coil of the first reactor to the load. The system of claim 16, wherein the first coil is configured to generate an AC current in response to a third magnetic field generated by the load, wherein the first coil is coupled to the second reactor and the fifth The coil is tuned to the load. The system of claim 15 further comprising a third reactor configured to receive excess energy from the first reactor and feed the excess energy back to the first reactor Input in. The system of claim 15 further comprising an input converter configured to receive power from a DC power source and convert the power to AC output power for use as the first reactor and Exciting at least one of the second reactors can. The system of claim 15, wherein the output converter is further configured to transmit a portion of the AC output power to one of the inputs of the first reactor.