Angle sensing using differential magnetic measurement and a back bias magnet

• US 9,869,566 B2
• Filed: 02/12/2016
• Issued: 01/16/2018
• Est. Priority Date: 02/12/2016
• Status: Active Grant

• Current Assignee: Allegro Microsystems Incorporated (Sanken Electric Company Limited)
• Original Assignee: Allegro Microsystems Incorporated (Sanken Electric Company Limited)
• Inventors: Tima, Simon, Vuillermet, Yannick, Friedrich, Andreas P., Kerdraon, Thomas
• Primary Examiner(s): LE, THANG XUAN
• Application Number:
  US15/042,469
• Publication Number:
  US 20170234702A1
• Time in Patent Office: 704 Days
• Field of Search: 324173-174, 324178-179, 324161, 324162, 3242072-20725, 324259
• CPC Class Codes: G01B 7/14 for measuring distance or clearance between spaced objects or spaced apertures G01B7/30 takes precedence
• CPC Class Codes: G01D 2205/773 Spiral profiles
• CPC Class Codes: G01D 5/147 influenced by the movement of a third element, the position of Hall device and the source of magnetic field being fixed in respect to each other
• CPC Class Codes: G01D 5/2013 by a movable ferromagnetic element, e.g. a core G01D5/2033 takes precedence
• CPC Class Codes: G01R 33/072 Constructional adaptation of the sensor to specific applications

Abstract

A magnetic field sensor includes a back bias magnet to generate a DC magnetic field. First and second magnetic field sensing elements of the magnetic field sensor are disposed proximate to at least one ferromagnetic surface of a ferromagnetic target object. The first and second magnetic field sensing elements generate first and second electronic signals, respectively, in response to first and second sensed magnetic fields corresponding to the DC magnetic field but influenced by the at least one ferromagnetic surface. The magnetic field sensor generates a difference signal that is a difference of amplitudes of the first and second electronic signals. The difference signal is indicative of a rotation measurement of an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about a rotation axis.

Claims

1. A magnetic field sensor, comprising:

a back bias magnet configured to generate a DC magnetic field;

first and second magnetic field sensing elements disposed along a sensing element line and disposed proximate to at least one ferromagnetic surface of a ferromagnetic target object, the first and second magnetic field sensing elements configured to generate first and second electronic signals, respectively, in response to first and second sensed magnetic fields corresponding to the DC magnetic field but influenced by the at least one ferromagnetic surface;

wherein the magnetic field sensor is operable to generate a difference signal that is a difference of amplitudes of the first and second electronic signals, and the difference signal is indicative of a rotation measurement of an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about a rotation axis, wherein the sensing element line is substantially parallel to the rotation axis, wherein the at least one ferromagnetic surface of the ferromagnetic target object comprises a helical groove disposed on the ferromagnetic target object, the helical groove configured to provide the difference signal with respect to the absolute relative rotation.

2. The magnetic field sensor of claim 1, wherein the difference signal is substantially linear with respect to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis.

3. The magnetic field sensor of claim 1, wherein the at least one ferromagnetic surface comprises a first groove surface and a second groove surface, the first and second groove surfaces intersecting at a vertex, thereby forming a V-shaped helical groove.

4. The magnetic field sensor of claim 3, wherein the first groove surface and the second groove surface are straight in one dimension.

5. The magnetic field sensor of claim 3, wherein the first groove surface and the second groove surface are curved in two dimensions.

6. The magnetic field sensor of claim 5, wherein curvatures of the first and second groove surfaces are selected to provide the difference signal as substantially linear with respect to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis.

7. The magnetic field sensor of claim 1, wherein the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis comprises a rotation of the ferromagnetic target object about the rotation axis and the magnetic field sensor is stationary.

8. The magnetic field sensor of claim 1, further comprising:

a differential amplifier coupled to receive the first and second electronic signals and configured to generate the difference signal.

9. The magnetic field sensor of claim 1, wherein the ferromagnetic target object comprises a rotating shaft, and the first and second magnetic field sensing elements are disposed in a side-shaft measurement arrangement with respect to the rotating shaft.

10. The magnetic field sensor of claim 1, wherein the helical groove comprises a helix structure having a first helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between zero degrees and a maximum rotation angle that is less than three hundred sixty degrees, and a second portion proximate to the helical groove that is flat.

11. The magnetic field sensor of claim 1, wherein the helical groove comprises a symmetrical helix structure having a first helix portion and a second helix portion, the first helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between zero degrees and one hundred eighty degrees, and the second helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between one hundred eighty degrees and three hundred sixty degrees, wherein the first and second helix portions are symmetrical with each other.

12. The magnetic field sensor of claim 11, wherein the magnetic field sensor is configured to detect a one hundred eighty degree symmetry of the helix structure in regard to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor, thereby determining an absolute relative rotation angle over a rotation greater than three hundred sixty degrees.

13. The magnetic field sensor of claim 12, wherein the absolute relative rotation angle, θ

_abs, of the ferromagnetic target object is determined by a relationship θ

_abs=θ

(Δ

B) in the first helix portion and by the relationship θ

_abs=360°

−

θ

(Δ

B) in the second helix portion, wherein θ

(Δ

B) is a differential of a magnetic field related to the difference signal, wherein an amplitude of the difference signal is related to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis.

14. A method of sensing an absolute relative rotation of a ferromagnetic target object and a magnetic field sensor about a rotation axis, the method comprising:

generating a DC magnetic field by a back bias magnet;

generating first and second electronic signals, respectively, by first and second magnetic field sensing elements disposed along a sensing element line and disposed proximate to at least one ferromagnetic surface of a ferromagnetic target object, the first and second electronic signals in response to first and second sensed magnetic fields corresponding to the DC magnetic field but influenced by the at least one ferromagnetic surface;

generating, by the magnetic field sensor, a difference signal that is a difference of amplitudes of the first and second electronic signals, and the difference signal is indicative of a rotation measurement of an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about a rotation axis, wherein the sensing element line is substantially parallel to the rotation axis, axis, wherein the at least one ferromagnetic surface of the ferromagnetic target object comprises a helical groove disposed on the ferromagnetic target object, the helical groove configured to provide the difference signal with respect to the absolute relative rotation.

15. The method of claim 14, wherein the difference signal is substantially linear with respect to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis.

16. The method of claim 14, wherein the at least one ferromagnetic surface comprises a first groove surface and a second groove surface, the first and second groove surfaces intersecting at a vertex, thereby forming a V-shaped helical groove.

17. The method of claim 16, wherein the first groove surface and the second groove surface are straight in one dimension.

18. The method of claim 16, wherein the first groove surface and the second groove surface are curved in two dimensions.

19. The method of claim 18, comprising:

providing the difference signal as substantially linear with respect to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis based upon curvatures of the first and second groove surfaces.

20. The method of claim 14, wherein the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis comprises a rotation of the ferromagnetic target object about the rotation axis and the magnetic field sensor is stationary.

21. The method of claim 14, further comprising:

receiving, by a differential amplifier, the first and second electronic signals and generating the difference signal.

22. The method of claim 14, wherein the ferromagnetic target object comprises a rotating shaft, and the first and second magnetic field sensing elements are disposed in a side-shaft measurement arrangement with respect to the rotating shaft.

23. The method of claim 14, wherein the helical groove comprises a ix structure having a first helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between zero degrees and a maximum rotation angle that is less than three hundred sixty degrees, and a second portion proximate to the helical groove that is flat.

24. The method of claim 14, wherein the helical groove comprises a symmetrical helix structure having a first helix portion and a second helix portion, the first helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between zero degrees and one hundred eighty degrees, and the second helix portion corresponding to an absolute relative rotation of the ferromagnetic target object and the magnetic field sensor between one hundred eighty degrees and three hundred sixty degrees, wherein the first and second helix portions are symmetrical with each other.

25. The method of claim 24, comprising:

detecting, by the magnetic field sensor, a one hundred eighty degree symmetry of the helix structure in regard to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor; and

determining an absolute relative rotation angle over a rotation greater than three hundred sixty degrees.

26. The method of claim 25, comprising:

determining the absolute relative rotation angle, θ

_abs, of the ferromagnetic target object by a relationship θ

_abs=θ

(Δ

B) in the first helix portion and by the relationship θ

_abs=360°

−

θ

(Δ

B) in the second helix portion, wherein θ

(Δ

B) is a differential of a magnetic field related to the difference signal, wherein an amplitude of the difference signal is related to the absolute relative rotation of the ferromagnetic target object and the magnetic field sensor about the rotation axis.