Wireless non-radiative energy transfer
Described herein are embodiments of a source high-Q resonator, optionally coupled to an energy source, a second high-Q resonator, optionally coupled to an energy drain that may be located a distance from the source resonator. A third high-Q resonator, optionally coupled to an energy drain that may be located a distance from the source resonator. The source resonator and at least one of the second resonator and third resonator may be coupled to transfer electromagnetic energy from said source resonator to said at least one of the second resonator and third resonator.
1. A wireless power system comprising:
a source module comprising a source resonator and a power supply coupled to the source resonator to provide power to the source resonator, the source resonator having a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 1 =ω 1 /(2Γ 1 ), the source resonator comprising at least one loop of conductive material and further comprising a capacitance; and
a portable electronic device having a device module comprising a device resonator and a load coupled to the device resonator to receive power from the device resonator and provide power to the portable electronic device, the device resonator having a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 2 =ω 2 /(2Γ 2 ), the device resonator comprising at least one loop of conductive material and further comprising a capacitance,
wherein the device module is spaced from the source module and configured to move freely relative to the source module over a range of distances D between the source module and the device module,
wherein the source resonator and the device resonator are configured to resonantly and wirelessly couple electromagnetic power from the source resonator to the device resonator using non-radiative electromagnetic induction having an energy transfer rate κ, and wherein the intrinsic loss rates satisfy κ/√{square root over (Γ 1 Γ 2 )}>2 over the range of distances D, and
wherein f 1 =ω 1 /(2π) and f 2 =ω 2 /(2π), and f 1 and f 2 , are between about 5 MHz and 380 MHz, and each intrinsic loss rate comprises a resistive component and a radiative component.
2. The wireless power system of claim 1 , wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is configured to be dynamically set as a function of the energy transfer rate κ between the first and second resonators as the device module is moveable relative to the source module over the range of distances D.
3. The wireless power system of claim 2 , wherein the work drainage rate Γ w is configured to be dynamically set such that the ratio of useful-to-lost power is maximized as a function of the energy transfer rate κ over the range of distances D.
4. The wireless power system of claim 2 , wherein the work drainage rate Γ w is configured to be dynamically set such that Γ w =Γ 2 √{square root over (1+(κ 2 /Γ 1 ·Γ 2 ))} as a function of the energy transfer rate κ over the range of distances D.
5. The wireless power system of claim 1 , wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is configured to be set such that Γ w =Γ 2 √{square root over (1+(κ 2 /Γ 1 ·Γ 2 ))} for some value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.
6. The wireless power system of claim 1 , wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is configured to be set such that the ratio of useful-to-lost power is maximized for some value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.
7. The wireless power system of claim 1 , wherein the portable electronic device is a cell phone, a computer, or a robot.
8. The wireless power system of claim 1 , wherein Q 1 >100.
9. The wireless power system of claim 8 , wherein Q 2 >100.
10. The wireless power system of claim 1 , wherein the source resonator has a characteristic size L 1 and the device resonator has a different characteristic size L 2 .
11. The wireless power system of claim 10 , wherein the intrinsic quality factors satisfy √{square root over (Q 1 Q 2 )}>100.
12. The wireless power system of claim 1 , wherein the range of distances D includes D=6 cm.
13. The wireless power system of claim 1 , wherein the range of distances D includes D=8 cm.
14. The wireless power system of claim 1 , wherein the range of distances D includes D=10 cm.
15. The wireless power system of claim 1 , wherein the non-radiative electromagnetic induction means that the distances D are less than the wavelengths corresponding to the resonant frequencies ω 1 and ω 2 .
16. The wireless power system of claim 1 , further comprising a second portable electronic device having a second device module comprising a second device resonator and a second load coupled to the second device resonator to receive power from the second device resonator and provide power to the second portable electronic device, and
wherein the second device module is spaced from the source module and configured to move freely relative to the source module and wherein the source resonator and the second device resonator are configured to resonantly and wirelessly couple electromagnetic power from the source resonator to the second device resonator using non-radiative electromagnetic induction.
17. The wireless power system of claim 1 , further comprising a feedback mechanism coupled to at least one of the resonators to correct for detuning of the resonant frequencies.
18. A source module for a wireless power system including a portable electronic device having a device module having a device resonator and a load coupled to the device resonator to receive power from the device resonator and provide power to the portable electronic device, the device resonator having a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 2 =ω 2 /(2Γ 2 ),
the source module comprising:
a source resonator and a power supply coupled to the source resonator to provide power to the source resonator, the source resonator having a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 1 =ω 1 /(2Γ 1 )>100, the source resonator comprising at least one loop of conductive material and further comprising a capacitance,
wherein the source module is configured to be spaced from the device module and the device module can move freely relative to the source module over a range of distances D between the source module and the device module,
wherein the source resonator is configured to resonantly and wirelessly provide electromagnetic power to the device resonator using non-radiative electromagnetic induction having an energy transfer rate κ, and wherein the intrinsic loss rates satisfy κ/√{square root over (Γ 1 Γ 2 )}>2 over the range of distances D, and
wherein f 1 =ω 1 /(2π) and f 2 =ω 2 /(2π), and f 1 and f 2 , are between about 5 MHz and 380 MHz, and each intrinsic loss rate comprises a resistive component and a radiative component.
19. The source module of claim 18 , wherein Q 1 >200.
20. A device module for use in a wireless power system for providing power to a portable electronic device, the wireless power system including a source module having a source resonator and a power supply coupled to the source resonator to provide power to the source resonator, the source resonator having a resonant frequency φ 1 , an intrinsic loss rate Γ 1 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 1 =ω 1 /(2Γ 1 ),
the device module comprising:
a device module comprising a device resonator and a load coupled to the device resonator to receive power from the device resonator and provide power to the portable electronic device, the device resonator having a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 2 =ω 2 /(2Γ 2 ), the device resonator comprising at least one loop of conductive material and further comprising a capacitance,
wherein the device module is configured to be spaced from the source module and move freely relative to the source module over a range of distances D between the source module and the device module,
wherein the device resonator is configured to resonantly and wirelessly receive electromagnetic power from the source resonator using non-radiative electromagnetic induction having an energy transfer rate κ, wherein the intrinsic loss rates satisfy κ/√{square root over (Γ 1 Γ 2 )}>2 over the range of distances D, and wherein f 1 =ω 1 /(2π) and f 2 =ω 2 /(2π), and f 1 and f 2 , are between about 5 MHz and 380 MHz, and each intrinsic loss rate comprises a resistive component and a radiative component, and
wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is configured to be dynamically set as a function of the energy transfer rate κ between the first and second resonators as the device module is movable relative to the source module over the range of distances D.
21. A device module for use in a wireless power system for providing power to a portable electronic device, the wireless power system including a source module having a source resonator and a power supply coupled to the source resonator to provide power to the source resonator, the source resonator having a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 1 =ω 1 /(2Γ 1 ),
the device module comprising:
a device module comprising a device resonator and a load coupled to the device resonator to receive power from the device resonator and provide power to the portable electronic device, the device resonator having a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 2 =ω 2 /(2Γ 2 ), the device resonator comprising at least one loop of conductive material and further comprising a capacitance,
wherein the device module is configured to be spaced from the source module and move freely relative to the source module over a range of distances D between the source module and the device module,
wherein the device resonator is configured to resonantly and wirelessly receive electromagnetic power from the source resonator using non-radiative electromagnetic induction having an energy transfer rate κ, wherein the intrinsic loss rates satisfy κ/√{square root over (Γ 1 Γ 2 )}>2 over the range of distances D, and wherein f 1 =ω 1 /(2π) and f 2 =ω 2 /(2π), and f 1 and f 2 , are between about 5 MHz and 380 MHz, and each intrinsic loss rate comprises a resistive component and a radiative component, and
wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is configured to be set such that the ratio of useful-to-lost power is maximized for some value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.
22. The device module of claim 21 , wherein the work drainage rate Γ w is configured to be set such that Γ w =Γ 2 √{square root over (1+(κ 2 /Γ 1 ·Γ 2 ))} for said value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.
23. A method for providing power wirelessly to a portable electronic device, wherein the portable electronic device is configured for use with a source module having a source resonator and a power supply coupled to the source resonator to provide power to the source resonator, the source resonator having a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 1 =ω 1 /(2Γ 1 ), the method comprising:
providing the portable electronic device with a device resonator and a load coupled to the device resonator to receive power from the device resonator and provide power to the portable electronic device, the device resonator having a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and capable of storing electromagnetic energy with an intrinsic quality factor Q 2 =ω 2 /(2Γ 2 ), the device resonator comprising at least one loop of conductive material and further comprising a capacitance, wherein the device module is spaced from the source module and configured to move freely relative to the source module over a range of distances D between the source module and the device module; and
resonantly and wirelessly receiving electromagnetic power at the device resonator from the source resonator using non-radiative electromagnetic induction having an energy transfer rate κ, wherein the intrinsic loss rates satisfy κ/√{square root over (Γ 1 F 2 )}>1 over the range of distances D, wherein f 1 =ω 1 /(2π) and f 2 =ω 2 /(2π), and f 1 and f 2 , are between about 5 MHz and 380 MHz, and wherein each intrinsic loss rate comprises a resistive component and a radiative component.
24. The method of claim 23 , further comprising:
providing power to the load in the portable electronic device from the device resonator, wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is dynamically set as a function of the energy transfer rate κ between the first and second resonators as the device module moves relative to the source module over the range of distances D.
25. The method of claim 24 , wherein the work drainage rate Γ w is dynamically set such that the ratio of useful-to-lost power is maximized as a function of the energy transfer rate κ over the range of distances D.
26. The method of claim 24 , wherein the work drainage rate Γ w is dynamically set such that Γ w =Γ 2 /√{square root over (1+(κ 2 /Γ 1 ·Γ 2 ))} as a function of the energy transfer rate κ over the range of distances D.
27. The method of claim 23 , further comprising:
providing power to the load in the portable electronic device from the device resonator, wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is set such that Γ w =Γ 2 /√{square root over (1+(κ 2 /Γ 1 ·Γ 2 ))} for some value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.
28. The method of claim 23 , further comprising:
providing power to the load in the portable electronic device from the device resonator, wherein the power provided to the load from the device resonator defines a work drainage rate Γ w , and wherein the work drainage rate Γ w is set such that the ratio of useful-to-lost power is maximized for some value of the energy transfer rate κ in the range of distances D as the device module is moveable relative to the source module over the range of distances D.