Wireless non-radiative energy transfer
The electromagnetic energy transfer device includes a first resonator structure receiving energy from an external power supply. The first resonator structure has a first Q-factor. A second resonator structure is positioned distal from the first resonator structure, and supplies useful working power to an external load. The second resonator structure has a second Q-factor. The distance between the two resonators can be larger than the characteristic size of each resonator. Non-radiative energy transfer between the first resonator structure and the second resonator structure is mediated through coupling of their resonant-field evanescent tails.
1. A system, comprising:
a source resonator configured to be coupled to an energy source; and
a second resonator located a distance from the source resonator;
wherein the source resonator and the second resonator are coupled to provide resonant non-radiative wireless energy transfer between the source resonator and the second resonator and wherein at least one resonator is a tunable resonator,
wherein the source resonator has a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and a first Q-factor Q 1 =ω 1 /(2Γ 1 ), the second resonator has a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and a second Q-factor Q 2 =ω 2 /(2Γ 2 ), and at least one of Q 1 and Q 2 is greater than 100.
2. The system of claim 1 , wherein the tunable resonator is a capacitively-loaded conducting-wire loop.
3. The system of claim 1 , wherein the tunable resonator is tuned through changes in its geometry.
4. The system of claim 1 , wherein the resonators wirelessly transfer energy at a continuous-wave frequency of the normal mode for the resonators that has a larger radiation-Q.
5. The system of claim 1 , wherein the resonators are electromagnetic resonators.
6. The system of claim 5 , wherein (√{square root over (Q 1 Q 2 )})>100.
7. The system of claim 5 , wherein the rate of the wireless energy transfer rate is κ, the second resonator has a characteristic size L 1 , and the resonators satisfy κ/√{square root over (Γ 1 Γ 2 )}>1 for at least some distances D between the first and second resonators satisfying D/L 2 >1.
8. The system of claim 5 , wherein the second resonator has a characteristic size L 2 and the efficiency of the wireless energy transfer is at least 20% for at least some distances D between the source and second resonators satisfying D/L 2 >1.
9. The system of claim 5 , wherein the efficiency of the wireless energy transfer is at least 20% for at least some distances D between the source and second resonators including 10 cm.
10. The system of claim 5 , further comprising the energy source and a load coupled to the second resonator, and wherein during operation the energy source and the load are driven to increase the ratio of useful-to-lost power for the wireless energy transfer rate κ.
11. The system of claim 5 , wherein the source resonator and the second resonator are electromagnetic resonators comprising a capacitance and an inductance.
12. The system of claim 5 , wherein the resonant frequencies f 1 =ω 1 /2π and f 2 =ω 2 /2π are each at least 5 MHz.
13. The system of claim 5 , further comprising an additional resonator coupled to the source resonator to provide resonant non-radiative wireless energy transfer between the source resonator and the additional resonator.
14. A system, comprising:
a source resonator configured to be coupled to an energy source; and
a second resonator located a distance from the source resonator;
wherein the source resonator and the second resonator are coupled to provide resonant non-radiative wireless energy transfer between the source resonator and the second resonator,
wherein at least one resonator is a tunable resonator, and
wherein at least one resonator is a high-Q resonator.
15. The system of claim 14 , wherein the high-Q resonator has a resonant frequency ω, an intrinsic loss rate Γ, and a first Q-factor Q=ω/(2Γ)>100.
16. The system of claim 14 , wherein the source resonator has a resonant frequency ω 1 , an intrinsic loss rate Γ 1 , and a first Q-factor Q 1 =ω 1 /(2Γ 1 ), the second resonator has a resonant frequency ω 2 , an intrinsic loss rate Γ 2 , and a second Q-factor Q 2 =ω 2 /(2Γ 2 ), and wherein (√{square root over (Q 1 Q 2 )})>100.
17. The system of claim 14 , wherein the tunable resonator is tuned through changes in its geometry.
18. The system of claim 14 , wherein the resonators wirelessly transfer energy at a continuous-wave frequency of the normal mode for the resonators that has a larger radiation-Q.
19. The system of claim 14 , wherein the rate of the wireless energy transfer rate is κ, the second resonator has a characteristic size L 1 , and the resonators to satisfy κ/√{square root over (Γ 1 Γ 2 )}>1 for at least some distances D between the first and second resonators satisfying D/L 2 >1.
20. The system of claim 14 , wherein the second resonator has a characteristic size L 2 and the efficiency of the wireless energy transfer is at least 20% for at least some distances D between the source and second resonators satisfying D/L 2 >1.
21. The system of claim 14 , wherein the efficiency of the wireless energy transfer is at least 20% for at least some distances D between the source and second resonators including 10 cm.
22. The system of claim 14 , further comprising the energy source and a load coupled to the second resonator, and wherein during operation the energy source and the load are driven to increase the ratio of useful-to-lost power for the wireless energy transfer rate κ.
23. The system of claim 14 , wherein the source resonator and the second resonator are electromagnetic resonators comprising a capacitance and an inductance.
24. The system of claim 14 , wherein the resonant frequencies f 1 =ω 1 /2π and f 2 =ω 2 /2π are each at least 5 MHz.
25. The system of claim 14 , further comprising an additional resonator coupled to the source resonator to provide resonant non-radiative wireless energy transfer between the source resonator and the additional resonator.
26. The system of claim 1 , wherein the source resonator and the second resonator are movable relative to one another to a define a variable distance between them.
27. The system of claim 14 , wherein the source resonator and the second resonator are movable relative to one another to a define a variable distance between them.