1 / 84

Wireless Power Transmission

Wireless Power Transmission. Alan Chun-yip Yeung Leanne Cheung Jeff Samandari Wehibe Belachew Tesfa Mael Jose A. Becerra. EE563-Graduate Seminar Fall 2004 Group 5. Presentation Outline. 1. Introduction / Background. 2. Theory of Wireless Power Trans. 3. Major Research Projects.

kalil
Télécharger la présentation

Wireless Power Transmission

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Wireless Power Transmission Alan Chun-yip Yeung Leanne Cheung Jeff Samandari Wehibe Belachew Tesfa Mael Jose A. Becerra EE563-Graduate Seminar Fall 2004 Group 5

  2. Presentation Outline 1. Introduction / Background 2. Theory of Wireless Power Trans. 3. Major Research Projects 4. Comparison of Efficiency … 5. Proposed Project/Experiment 6. Conclusion

  3. 1. Introduction / Background

  4. Outline • History/Background • Solar Power Satellite • Microwave Power Transmission • Conclusion Reference: http://www.kentlaw.edu/classes/fbosselm/Spring2004/PowerPoints/Wireless%20Power%20Transmission%20-%20Soubel.ppt

  5. Background, Nikola Tesla • 1856-1943 • Innovations: • Alternating current • Wireless power transmission experiments at Wardenclyffe

  6. Wardenclyffe • 1899 • Able to light lamps over 25 miles away without using wires • High frequency current, of a Tesla coil, could light lamps filled with gas (like neon)

  7. 1940’s to Present • World War II developed ability to convert energy to microwaves using a magnetron, no method for converting microwaves back to electricity • 1964 William C. Brown demonstrated a rectenna which could convert microwave power to electricity

  8. Solar Power from Satellites • 1968’s idea for Solar Power Satellites proposed by Peter Glaser • Would use microwaves to transmit power to Earth from Solar Powered Satellites • Idea gained momentum during the Oil Crises of 1970’s, but after prices stabilized idea was dropped • US Department of Energy research program 1978-1981

  9. Problems • Issues identified during the DOE study • Complexity—30 years to complete • Size—6.5 miles long by 3.3 miles wide • Transmitting antenna ½ mile in diameter(1 km) • Cost—$74 billion • Interference

  10. From the Satellite • Solar power from the satellite is sent to Earth using a microwave transmitter • Received at a “rectenna” located on Earth • Recent developments suggest that power could be sent to Earth using a laser

  11. Microwaves • Frequency 2.45 GHz microwave beam • Retro directive beam control capability • Power level is well below international safety standard

  12. Microwave More developed High efficiency up to 85% Beams is far below the lethal levels of concentration even for a prolonged exposure Cause interference with satellite communication industry Laser Recently developed solid state lasers allow efficient transfer of power Range of 10% to 20% efficiency within a few years Conform to limits on eye and skin damage Microwave vs. Laser Transmission

  13. Rectenna “An antenna comprising a mesh of dipoles and diodes for absorbing microwave energy from a transmitter and converting it into electric power.” • Microwaves are received with about 85% efficiency • Around 5km across (3.1 miles) • 95% of the beam will fall on the rectenna

  14. 5,000 MW Receiving Station (Rectenna). This station is about a mile and a half long.

  15. 2. Theory of Wireless Power Trans.

  16. Theory of Operation • Electromagnetic Radiation • Antenna basics • Phased-array antenna • Diffraction analogy • Energy distribution • Rectenna • Physical limitations & relationships

  17. Physics of Wireless Power Transmission • Forms of Electromagnetic radiation • Travel at same speed • F = frequency • C = velocity of light • L =wavelength • http://imnh.isu.edu/digitalatlas/clima/atmosph/images/waves.jpg

  18. Dipole Antenna • Transmission of power is simpler than TV & Radio • Transmitter: wire half a wavelength • Pushes electrons back and forth • Receiver: wire half a wavelength http://www.zorg.org/radio/dipole_antenna.shtml

  19. Antenna Radiation Pattern http://www.astromag.co.uk/portable/dipole.gif

  20. Phased-array antenna • The λs for microwaves are small  dipoles small • Beam focusing: phased-array antenna • Electronically steered by varying the timing or phase • Waves will merge together http://www.mcs.harris.com/oceannet/features/antenna.html

  21. Phased-Array Antenna http://www.cea.com.au/products/phasedarray/i2_ceafar.html

  22. Diffraction analogy • Light same properties • Laser beam shinning trough a narrow opening & spreads out or diffracts • Bright spot in the center w/fainter spots on the side http://planetquest.jpl.nasa.gov/technology/diffraction.html

  23. Diffraction & Microwaves • Waves reinforce at some points and they cancel out at other points (bright and fainter points) • In microwaves: is a scaled up version of diffraction

  24. Intensity

  25. Main lobe energy • Circular central max •  Main lobe • 84% of energy • Sidelobes surround • No energy  minima

  26. Intensity 84% in main lobe

  27. Rectenna • Array of dipole antennas known as rectifying antenna or Rectenna • Diameter = Dr

  28. Rectenna

  29. Physical Limitations • The receiving diameter Dr increases with transmitter receiver separation distance S. • Dr increases if transmitter diameter Dt decreases

  30. Physical Limitations

  31. 2. Sample Calculations

  32. Calculations/Analysis • Frequency,f(Hz) • Intensity, I(watts per square meter) • Wave-Length, L(meters) • Received Main Beam Lope (“spot”) Diameter, Dr(meters or kilometers) • Transmitting Phased Array Diameter, Dt(meters or kilometers) • Example: how to estimate Intensity, I?

  33. Frequency Formula Dt * Dr • Frequency,f (Hz)= -------------- (2) (L * S) Dt: transmitting phased array diameter Dr: received main beam lobe (“spot”) diameter L: wavelength S: separation

  34. Frequency Analysis Dt * Dr If (Frequency,f(Hz)= ----------- ) 2.44 GHz (2) (L * S) Then at least, 84% of the energy of the beam will be captured Note: • This energy is not linear; 42% of the energy is not equivalent to 1.22 GHz. • Equation (2) represent a best case scenario. • Practical antenna sizes may have to be larger if most of the beam is to be captured. • The rectenna will have to be at least as large as Dt, even if (2) says Dr is smaller.

  35. Frequency Analysis • Such a wide beam can be focused, but only to a minimum size Dr. • For low Earth-orbit power-beaming demonstrations, it is easier to put the smaller antenna in space and the larger antenna on Earth. • Early demonstrations may capture only a small percentage of the total power, in order to keep antenna sizes small. • to light up a 60 watt bulb, thousands of watts may have to be transmitted. • Since costly to launch such a power generating apparatus, the most feasible demonstration project may be Earth-to-space transmission from a large transmitting antenna (such as the Arecibo dish) to a smaller rectenna in space.

  36. Intensity, IFormula • Intensity, I(watts per square meter) P Dt = ½ ( Pi * -----) * ( --------- ) (3) 4 L * S Pi: 3.14… P: total power transmitted Dt: transmitted phased array diameter L: wave length S: transmitter to receiver distance (separation)

  37. Wave-Length, LCalculations • Wave-Length, L(meters) c 300,000,000 meter/sec = ----- = ( -------------------------------- ) = 0.1224 (1) f 2,450,000,000/sec meter c: speed of light f: frequency

  38. Received Main Beam Lope Diameter, Dr Calculations • Received Main Beam Lope (“spot”) Diameter, Dr(meters or kilometers) f * L * S 2.44 * 0.12224m * 35,800,000m = -------------- = -------------------------------------------- Dt 1000m = 10,700 meter = 10.7 kilometers L: wave length S: separation Dt: transmitting phased array diameter

  39. Transmitting Phased Array Diameter, DtCalculations • Transmitting Phased Array Diameter, Dt(meters or kilometers) f * L * S 2.44 * 0.12224m * 35,800,000m = -------------- = ---------------------------------------------- Dr 10,700 meter = 1000m = 1 kilometers L: wave length S: separation Dr: received main beam lope (“spot”) diameter

  40. Example What is the Intensity, I = ? Given: f, Dr, and a typical solar power satellite transmitting 5 billion watts from geostationary orbit 35800 kilometers high. Solution: Use the following (1), (2), & (3) C f = -----  L(1) L Dt * Dr Frequency,f(Hz)= --------------  Dt(2) (L * S) P Dt Intensity, I(watts/m^²) = ½ ( Pi * -----) * ( --------- ) (3) 4 L * S

  41. Example Calculations • Intensity, I(watts per square meter) P Dt = ½ ( Pi * -----) * ( --------- ) (3) 4 L * S 2287485.869w 1000m = ½ ( Pi * ---------------------------) * ( ----------------------------------- ) 4m 0.1224m* 35800,000m = 205 watts/m^² or 20.5 milliwatts/cm^²

  42. Example Analysis • peak beam intensity, Ip = 20.5 milliwatts/cm^²  This is abouttwice US industrial standard for human exposure  This is converted (by rectenna) to electricity by 90% efficiency • Average intensity, Ia 1/3 * 20.5 milliwatts/cm^²

  43. Rectangular Transmitting antenna array Calculations • Mathematics slightly different, but the same general principles apply. • Central maximum of the beam contain 82% of the transmitted energy. • Rectangular in shape, but will spread out more along TX array’s short direction than its long direction. • Example: Canada’s Radar sat rectangular transmitting antenna: 1.5m × 15m “footprint” on the ground: 7,000m × 50,000m frequency: 5.3 GHz altitude: 800,000m output power: 5000 watts  The power is too spread out at the ground to use in a practical demonstration project.

  44. Two more points • Use certain transmitting methods • to reduce the level of the sidelobes • to put some of the sidelobe energy into the main lobe •  Price to pay: Larger Rectenna (because main lobe spreads out) • Principal of diffraction also limits the resolution of optical systems: • Lenses • Telescopes

  45. 3. Major Research Projects

  46. 1979 SPS Reference System concept (GEO)

  47. Accomplishments of Solar Power Satellites • 1980, 30 kW of microwave power was transmitted to a receiving antenna over one mile • 1993, Japan successfully transmitted a 800W microwave beam from a rocket to a free-flying satellite in space. • 1998, Microwave to DC conversion efficiency of 82% or higher by the rectenna.

  48. NASA’s 1995-1997 Fresh Look Study • MEO (Mid-Earth Orbit) Sun Tower: - 6 SPS yields near 24-hr power to sites - ± 30 degrees Latitude Coverage - Power services of 200-400 MW

More Related