# US 2019/0246482 A1 · Cyclotronic plasma actuator with arc-magnet for active flow control > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2019/0246482 A1 - Document ID: US20190246482A1 - Status: Published application - Kind: A1 - Application number: 16/387,777 - Filed: 2019-04-18 - Published: 2019-08-08 - Earliest claimed: 2017-03-17 - Assignees: CU Aerospace, LLC; The Board of Trustees of the University of Illinois - Applicants: CU Aerospace, LLC; The Board of Trustees of the University of Illinois - Inventors: Joseph W. Zimmerman; David L. Carroll; Phillip J. Ansell; Georgi Hristov - Web page: https://patentgrep.com/patent/US20190246482A1 ## CPC - H01J 37/32064: {Circuits specially adapted for controlling the arc discharge (for plasma torches H01H1/36)} - B64C 23/005: {by other means not covered by groups B64C23/02 - B64C23/08, e.g. by electric charges, magnetic panels, piezoelectric elements, static charges or ultrasounds} - H01J 37/32449: {Gas control, e.g. control of the gas flow} - H01J 37/32568: {Relative arrangement or disposition of electrodes; moving means} - H01J 37/32678: {Electron cyclotron resonance} - H04L 27/1563: {using transition or level detection} - H05H 1/50: and using applied magnetic fields, e.g. for focusing or rotating the arc - B64C 2230/12: by using electromagnetic tiles, fluid ionizers, static charges or plasma - H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H) - B64C: AEROPLANES; HELICOPTERS - H04L: TRANSMISSION OF DIGITAL INFORMATION, e.g. TELEGRAPHIC COMMUNICATION (arrangements common to telegraphic and telephonic communication H04M) - H05H: PLASMA TECHNIQUE (apparatus or processes specially adapted for producing X-rays H05G2/00); PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS ## Abstract In an embodiment of the invention there is a cyclotronic actuator utilizing a high-voltage plasma driver connected to a first electrode. A second electrode is grounded and the two are isolated from each other by a dielectric plate. A magnet is positioned beneath the dielectric plate such that a coaxial dielectric barrier discharge plasma is formed outwardly between the first electrode across the dielectric plate. The magnet positioned beneath the dielectric plate introduces a magnetic field transverse to the plasma current path, such that the plasma discharge discharges radially and the local magnetic field is oriented vertically in a direction perpendicular to the dielectric plate to create a Lorentz Force, which forces the plasma discharge to move radially outwardly in a curved radial streamer mode pattern. ## Claims ### Claim 1 A cyclotronic actuator comprising: a high-voltage plasma driver; a first electrode being connected to the high-voltage plasma driver and having an upper portion and an upper section connected to the upper portion; a dielectric barrier defined by a dielectric plate connected to a dielectric cylinder, the dielectric cylinder having a bore through to define an inner surface of the dielectric cylinder, the bore being sized to receive the first electrode within the dielectric cylinder and wherein the upper section of the first electrode is positioned against a portion of the dielectric plate adjacent the bore; a ring magnet having an inner diameter and an outer circumference, wherein the inner diameter of the ring magnet is sized to position adjacent an outside side surface of the dielectric cylinder such that the dielectric cylinder and the dielectric plate isolates the ring magnet from the first electrode; a second electrode grounded and configured to surround the outer circumference of the ring magnet and the ground electrode being positioned beneath the dielectric plate, such that when the high-voltage plasma driver circuit is activated, a coaxial dielectric barrier discharge plasma is formed outwardly between the upper section of the first electrode across a top surface of the dielectric plate that is positioned above the second electrode; and wherein the ring magnet being positioned beneath the dielectric plate introduces a local magnetic field transverse to the coaxial dielectric barrier discharge plasma current path, such that the coaxial dielectric plasma barrier discharge discharges radially and the local magnetic field is oriented vertically in a direction perpendicular to the dielectric plate to create a Lorentz Force, combining electric field and magnetic field forces, which forces charged particles within the coaxial dielectric barrier discharge plasma to move in a curved path along the dielectric top surface, radially outward from the upper section of the first electrode and to cause the coaxial dielectric plasma barrier discharge to discharge out in a curved radial streamer mode pattern, whereby three-dimensional vortical structures are produced by the plasma discharge. ### Claim 2 (depends on 1) The actuator of claim 1, wherein the high-voltage AC plasma driver produces a plasma discharge with a voltage of the arc gap within the 500 V to 20 kV range or a variable frequency range of the plasma discharge within a 10 Hz5 to 100 kHz range and a current of the plasma discharge between 5 and 500 mA. ### Claim 3 (depends on 1) The actuator of claim 1, wherein the high-voltage pulsed plasma driver produces a plasma discharge with a voltage of the arc gap within the 2 kV to 12 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 10 and 50 A. ### Claim 4 (depends on 1) The actuator of claim 1, wherein the high-voltage electrical plasma driver is selected from one or more of the following: a high-voltage AC plasma driver, a high-voltage RF circuit, a high-voltage pulsed DC plasma driver, or a bipolar high-voltage circuit. ### Claim 5 A cyclotronic actuator comprising: a dielectric barrier defined by a dielectric plate connected to a dielectric base, the dielectric base having a cavity; a high-voltage plasma driver; a first electrode being connected to the high-voltage plasma driver and having an annular upper portion, positioned on a top surface of the dielectric plate; a magnet placed in the cavity of the dielectric base and positioned beneath the dielectric plate such that the dielectric plate isolates the magnet from the first electrode; a second electrode grounded and configured to include a portion extending across the annular upper portion of the first electrode and further positioned between the dielectric plate and the magnet, such that when the high-voltage plasma driver is activated, a coaxial dielectric barrier discharge plasma is formed inwardly between the annular upper portion of the first electrode across the top surface of the dielectric plate that is positioned above the second electrode; and wherein the magnet being positioned beneath the dielectric plate introduces a local magnetic field transverse to the coaxial dielectric barrier discharge plasma current path, such that the coaxial dielectric plasma barrier discharge discharges radially and the local magnetic field is oriented vertically in a direction perpendicular to the dielectric plate to create a Lorentz Force, combining electric field and magnetic field forces, which forces charged particles within the coaxial dielectric barrier discharge plasma to move in a curved path along the top surface of the dielectric plate, radially inward from the annular upper portion of the first electrode and to cause the coaxial dielectric plasma barrier discharge to discharge inwardly in a curved radial streamer mode pattern, whereby three-dimensional vortical structures are produced by the plasma discharge. ### Claim 6 (depends on 5) The actuator of claim 5, wherein the magnet can be a ring magnet, bar magnet, or cylindrical magnet. ### Claim 7 (depends on 5) The actuator of claim 5, wherein the magnet is positioned against the second electrode beneath the annular upper portion of the first electrode or include a dielectric spacer positioned between the magnet and the portion of the second electrode extending beneath the first electrode. ### Claim 8 (depends on 5) The actuator of claim 5, wherein the high-voltage AC plasma driver produces a plasma discharge with a voltage of the arc gap within the 500 V to 20 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 5 and 500 mA. ### Claim 9 (depends on 5) The actuator of claim 5, wherein the high-voltage pulsed plasma driver produces a plasma discharge with a voltage of the arc gap within the 2 kV to 12 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 10 and 50 A. ### Claim 10 (depends on 5) The actuator of claim 5, wherein the high-voltage electrical plasma driver is selected from one or more of the following: a high-voltage AC plasma driver, a high-voltage RF circuit, a high-voltage pulsed DC plasma driver, or a bipolar high-voltage circuit. ### Claim 11 A cyclotronic actuator comprising: a dielectric barrier plate having a top surface; a high-voltage plasma driver; a first electrode connected to the high-voltage plasma driver, and the first electrode positioned on the top surface of the dielectric plate; a second electrode grounded and positioned on the top surface of the dielectric plate; wherein both the first and second electrodes are separately configured to have profile edges created from starting edges to ending edges defined in the first and second electrodes and further configured to face each other to create a defined channel there between; a magnet positioned beneath the dielectric plate such that the dielectric plate isolates the magnet from the electrodes, and wherein the magnet is further positioned beneath the defined channel created between the profile edges on the first and second electrodes, such that when the high-voltage plasma driver is activated, a plasma discharge filament is formed between the channel created between the first and second electrodes across the top surface of the dielectric plate; and wherein the magnet being positioned beneath the dielectric plate introduces a local magnetic field transverse to the plasma filament current path, such that the plasma filament discharge discharges in the electrode gap and the local magnetic field is oriented vertically in a direction parallel to the orientation of the first electrode to create a Lorentz Force which forces charged particles within the plasma discharge to move in a direction travelling from the starting edges to ending edges of the first and second electrodes and then repeating the pattern, whereby three-dimensional vortical structures are produced by the moving plasma discharge. ### Claim 12 (depends on 11) The actuator of claim 11, wherein the profile edges are defined as symmetrical and defined to create a divergent channel from the defined starting edges to ending edges in the first and second electrodes. ### Claim 13 (depends on 11) The actuator of claim 11, wherein the profile edges are defined as asymmetrical wherein the first electrode has an inwardly facing concave arcuate profile and the second electrode has an outwardly facing convex arcuate profile such that the first and second electrodes create an asymmetrical curved channel for the plasma discharge filament to travel. ### Claim 14 (depends on 11) The actuator of claim 11, wherein the high-voltage AC plasma driver produces a plasma discharge with a voltage of the arc gap within the 500 V to 20 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 5 and 500 mA. ### Claim 15 (depends on 11) The actuator of claim 11, wherein the high-voltage pulsed plasma driver produces a plasma discharge with a voltage of the arc gap within the 2 kV to 12 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 10 and 50 A. ### Claim 16 (depends on 11) The actuator of claim 11, wherein the high-voltage electrical plasma driver is selected from one or more of the following: a high-voltage AC plasma driver, a high-voltage RF circuit, a high-voltage pulsed DC plasma driver, or a bipolar high-voltage circuit. ### Claim 17 A cyclotronic actuator comprising: a dielectric barrier plate having a top surface; a high-voltage plasma driver; a first electrode connected to the high-voltage plasma driver, and the first electrode positioned on the top surface of the dielectric plate and having an inwardly facing concave arcuate edge; a second electrode grounded and positioned on the top surface of the dielectric plate, and the second electrode having an outwardly facing convex arcuate edge, and wherein the inwardly facing concave arcuate edge of the first electrode is positioned at a distance from and facing the outwardly facing convex arcuate edge of the second electrode to define a channel there between; a magnet positioned beneath the dielectric plate such that the dielectric plate isolates the magnet from the electrodes, and wherein the magnet is further positioned beneath the defined channel created between edges on the first and second electrodes, such that when the high-voltage plasma driver is activated, a plasma filament is formed between the channel created between the first and second electrodes across the top surface of the dielectric plate; and wherein the magnet being positioned beneath the dielectric plate introduces a local magnetic field transverse to the plasma filament current path, such that the plasma filament discharge discharges in the electrode gap and the local magnetic field is oriented vertically in a direction parallel to the orientation of the first electrode to create a Lorentz Force which forces charged particles within the plasma discharge to move in a direction travelling from the starting edges to ending edges of the first and second electrodes and then repeating the pattern, whereby three-dimensional vortical structures are produced by the moving plasma discharge. ### Claim 18 (depends on 17) The actuator of claim 17, wherein the high-voltage AC plasma driver produces a plasma discharge with a voltage of the arc gap within the 500 V to 20 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 5 and 500 mA. ### Claim 19 (depends on 17) The actuator of claim 17, wherein the high-voltage pulsed plasma driver produces a plasma discharge with a voltage of the arc gap within the 2 kV to 12 kV range or a variable frequency range of the plasma discharge within a 10 Hz to 100 kHz range and a current of the plasma discharge between 10 and 50 A. ### Claim 20 (depends on 17) The actuator of claim 17, wherein the high-voltage electrical plasma driver is selected from one or more of the following: a high-voltage AC plasma driver, a high-voltage RF circuit, a high-voltage pulsed DC plasma driver, or a bipolar high-voltage circuit.