ELECTROMAGNETIC DEVICE HAVING COMPACT FLUX PATHS FOR HARVESTING ENERGY FROM VIBRATIONS

• US 20100194117A1
• Filed: 02/05/2009
• Published: 08/05/2010
• Est. Priority Date: 02/05/2009
• Status: Abandoned Application

• Current Assignee: Massachusetts Institute of Technology, Schlumberger Technology Corporation (Schlumberger NV)
• Original Assignee: Schlumberger Technology Corporation (Schlumberger NV)
• Inventors: Ma, Hongshen, Trimble, Zachary, Sihler, Joachim, Pabon, Jahir A., Guerrero, Julio, Lang, Jeffrey H., Slocum, Alex
• Application Number:
  US12/366,119
• Publication Number:
  US 20100194117A1
• Time in Patent Office: Days
• US Class Current: 290/1.00R
• CPC Class Codes: H02K 35/02 with moving magnets and stationary coil systems

Abstract

Electrical energy is produced by harvesting mechanical energy in the form of vibrations which are generally present in tools during the process of drilling oil wells. Electrical energy production is based on the Faraday induction principle whereby changes, i.e., movement, in magnetic flux through a coil induce an electric current through the coil. The changes in magnetic flux are produced by relative motion between at least one set of magnets and at least one coil. In particular, as the flux lines change due to the movement of the magnets, they remain perpendicular to both the direction of motion of the magnets as well as a planar or cylindrical surface defined by the coils. As a result, output for a given size of device is enhanced. Further, flexibility in adapting device form factor to particular shapes is enhanced. For example, a relatively flat device may be implemented using flexural bearing support of the magnets and coils on a printed circuit. The flexural bearings may also function as spring members that define the resonant frequency of the device. Alternative embodiments may be characterized by cylindrical or annular form factors.

Claims

1. Apparatus for converting mechanical energy into electrical energy, comprising:

at least one coil defining a surface;

a plurality of magnets arranged with respect to the at least one coil such that magnetic flux from the magnets induces an electric current through the coil in response to relative motion between the magnets and at least one coil over a range of motion, wherein magnetic lines of flux from the magnets through the at least one coil are perpendicular to both the surface of the coils and direction of relative motion between the at least one coil and magnets over the range of motion.

2. The apparatus of claim 1 wherein the magnets are arranged so that adjacent magnets are characterized by opposite polarizations.

3. The apparatus of claim 1 further including at least one magnetically permeable plate adjacent to the at least one coil.

4. The apparatus of claim 1 further including at least one magnetically permeable plate adjacent to the magnets.

5. The apparatus of claim 1 wherein the at least one coil includes a plurality of coils disposed with respect to each other and the magnets so as to generate separate alternating currents of different phase in each coil.

6. The apparatus of claim 5 wherein the coils are fixed relative to one another, and offset by a distance proportional to dimensions of the magnets.

7. The apparatus of claim 1 further including at least one spring member that controls the range of relative motion and defines a resonant frequency of the apparatus.

8. The apparatus of claim 7 wherein the at least one coil is attached to a mass, and the spring member is attached to the mass.

9. The apparatus of claim 7 wherein the magnets are attached to a mass, and the spring member is attached to the mass.

10. The apparatus of claim 7 wherein the spring member includes a flexure.

11. The apparatus of claim 10 wherein the flexures supports the coil, the magnet, or both the coil and the magnet to prevent or appreciably reduce movement in directions other than the one used to induce current on the coils, and thus eliminating the need to use bearings or other guiding mechanisms.

12. The apparatus of claim 1 wherein the surface defined by the coils is planar.

13. The apparatus of claim 1 wherein the surface defined by the coils is cylindrical.

14. The apparatus of claim 1 wherein the surface defined by the coils is a portion of a cylinder.

15. The apparatus of claim 1 wherein the magnets are characterized by an annular shape.

16. The apparatus of claim 15 wherein the magnets are radially polarized.

17. The apparatus of claim 16 wherein radial polarization of adjacent magnets in the stack is alternated.

18. The apparatus of claim 17 wherein the at least one coil is wound in partial wraps around the magnets.

19. The apparatus of claim 7 wherein the spring member is characterized by a non-linear spring constant.

20. The apparatus of claim 1 further including at least first and second spring members, the first spring member controlling motion of the at least one coil and the second spring member controlling motion of the magnets.

21. The apparatus of claim 20 wherein motion of the coil is characterized by a different resonant frequency than motion of the magnets.

22. The apparatus of claim 1 including first and second sets of coils, wherein the magnets are disposed between the first and second sets of coils.

23. The apparatus of claim 22 further including a separate mass and magnetically permeable backing plate for each of the first and second sets of coils.

24. The apparatus of claim 22 wherein first and second spring members are associated with the first and second sets of coils, respectively.

25. The apparatus of claim 24 wherein the first and second sets of coils are characterized by different resonant frequencies.

26. The apparatus of claim 25 wherein a third spring member is associated with the magnets.

27. The apparatus of claim 26 wherein the magnets are characterized by a different resonant frequency which is either higher or lower than the resonant frequencies of both sets of coils.

28. A method for converting mechanical energy into electrical energy, comprising:

with at least one coil defining a surface and a plurality of magnets arranged with respect to the at least one coil such that magnetic flux from the magnets induces an electric current through the coil in response to relative motion between the magnets and at least one coil over a range of motion, controlling relative motion between the magnets and at least one coil such that magnetic lines of flux from the magnets through the at least one coil are perpendicular to both the surface of the coils and direction of relative motion between the at least one coil and magnets over the range of motion.

29. The method of claim 28 wherein the at least one coil includes a plurality of coils, and including generating a plurality of alternating currents of different phase in each coil.

30. The method of claim 28 including controlling relative motion between the magnets and at least one coil with at least one spring member that defines a resonant frequency.

31. The method of claim 28 including controlling relative motion between the magnets and at least one coil with at least one spring member and at least one mass that define a resonant frequency.

32. The method of claim 28 including confining relative motion between the magnets and at least one coil to a linear range of motion.

33. The method of claim 28 including confining relative motion between the magnets and at least one coil to an arcuate range of motion.

34. The method of claim 28 including controlling relative motion between the magnets and at least one coil with at least one spring member characterized by a non-linear spring constant.

35. The method of claim 28 including controlling relative motion between the magnets and at least one coil with at least first and second spring members, the first spring member controlling motion of the at least one coil and the second spring member controlling motion of the magnets.

36. The method of claim 35 including controlling motion of the coil and controlling motion of the magnets at a different resonant frequencies.

37. The method of claim 28 including first and second sets of coils, wherein the magnets are disposed between the first and second sets of coils, wherein first and second spring members are associated with the first and second sets of coils, respectively, and including controlling the first and second sets of coils at different resonant frequencies.

38. The method of claim 37 wherein a third spring member is associated with the magnets, and including controlling the magnets at a different resonant frequency than the first and second sets of coils.