Magnetoelastic torque transducer

• US 4,896,544 A
• Filed: 11/17/1987
• Issued: 01/30/1990
• Est. Priority Date: 12/05/1986
• Status: Expired due to Term

• Current Assignee: Chicago Pneumatic Sales (Atlas Copco AB)
• Original Assignee: Mag Dev Inc.
• Inventors: Garshelis, Ivan J.
• Primary Examiner(s): Ruehl, Charles A.
• Application Number:
  US07/119,531
• Time in Patent Office: 805 Days
• Field of Search: 73/862.36
• US Class Current: 73/862.333
• CPC Class Codes: G01L 3/102 involving magnetostrictive means magnetostrictive sensors H10N35/101
• CPC Class Codes: G01L 3/103 Details about the magnetic material used
• CPC Class Codes: G01L 3/105 involving inductive means G01L3/102, G01L3/104 take precedence

Abstract

A magnetoelastic torque transducer for providing an electrical signal indicative of the torque applied to a member, the member including ferromagnetic, magnetostrictive means affixed to, associated with or forming a part of the surface of the torqued member for altering in magnetic permeability in response to the application of torque to the member. The ferromagnetic, magnetostrictive means is advantageously formed of a thermally hardened or iron-nickel martensite hardenable steel alloy characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of one or more elements selected from Ni, Cr, Co, Ti, Al, Mn, Mo, Cu and B to raise the alloy magnetostriction to at least 5 ppm absolute. Preferably, the ferromagnetic, magnetostrictive means is formed of nickel maraging steel. The transducer comprises a pair of axially spaced-apart annular bands defined within a region of the ferromagnetic, magnetostrictive means, the bands being endowed with residual stress created, respectively symmetrical right and left hand helically directed magnetic anisotropy of sufficiently large magnitude that the contribution to total magnetic anisotropy of any random anisotropy in the member is negligible. In one aspect of the invention, each said band has at least one circumferential region which is free of residually unstressed areas over at least 50% of its circumferential length. In another aspect of the invention, the alloy is thermally hardened before the bands are endowed with the residual stress-created magnetic anisotropy.

Claims

1. A magnetoelastic torque transducer for providing an electrical signal indicative of the torque applied to a member, said member having a ferromagnetic and magnetostrictive region formed of a thermally hardened steel alloy characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute, said transducer comprising:

a pair of axially spaced-apart annular bands defined within said region, said bands having respectively symmetrical right and left hand helically directed residual stress created magnetic anisotropy of sufficiently large magnitude compared with the random magnetic anisotropy in said member that the contribution to total magnetic anisotropy of any random anisotropy is negligible, each said band having at least one circumferential region which is free of residually unstressed areas over at least 50% of its circumferential length;

means for applying a cyclically time varying magnetic field to said bands;

means for sensing the change in permeability of said bands caused by said applied torque; and

,

means for converting said sensed change in permeability to an electrical signal indicative of the magnitude of the torque applied to said member.

2. A magnetoelastic torque transducer, as claimed in claim 1, wherein each said band has at least one circumferential region which is free of residually unstressed areas over at least 80% of its circumferential length.

3. A magnetoelastic torque transducer, as claimed in claim 1, wherein said band has at least one continuous circumferential region which is free of residually unstressed areas.

4. A magnetoelastic torque transducer, as claimed in claim 1, wherein said alloy further includes from zero up to a useful quantity for imparting desired properties to said alloy of an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vanadium, hafnium, columbium, tantalum, tin, and combinations thereof.

5. A magnetoelastic torque transducer, as claimed in claim 1, wherein said region is formed of a thermally hardened steel alloy consisting essentially of the elements and proportions indicated by the general formula:

space="preserve" listing-type="equation">FeC.sub.a M.sub.b Q.sub.c

wherein;

"M" is an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof;

"Q" is an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vandadium, hafnium, columbium, tantalum, tin and combinations thereof;

"a" indicates a carbon content of from 0.05 to 0.75 percent by weight;

"b" indicates a content of element "M" at least sufficient to raise the magnetostriction of said alloy to at least 5 ppm absolute; and

"c" indicates a content of element "Q" from zero to a useful quantity for imparting desired properties to said alloy.

6. A magnetoelastic torque transducer, as claimed in claim 1, wherein said region forms a part of the surface of said member.

7. A magnetoelastic torque transducer, as claimed in claim 1, wherein said region is rigidly affixed to the surface of said member.

8. A magnetoelastic torque transducer, as claimed in claim 1, wherein said region is formed of a steel alloy selected from the group consisting of through hardenable and case hardenable steel alloys.

9. A magnetoelastic torque transducer, as claimed in claim 1, wherein the magnetic easy axes in said bands are oriented, respectively, at angles of ±

20°

-60°

to the axis of said member.

10. A magnetoelastic torque transducer, as claimed in claim 1, wherein said region is formed of nickel maraging steel and said bands are defined and said residual stress-created magnetic anisotropy has been instilled within a mechanically soft portion of said region.

43. An internal combustion engine having a torque-carrying output member, said member including a magnetoelastic torque transducer as claimed in claims 1 or 13.

44. Power transmission means having a torque-carrying output member, said member including a magnetoelastic torque transducer as claimed in claims 1 or 13.

45. Fluid turbine means having a torque-carrying output member, said member including a magnetoelastic torque transducer as claimed in claims 1 or 13.

46. A weighing system including torque-carrying means, said means including a magnetoelastic torque transducer as claimed in claims 1 or 13.

47. A machine tool including means for causing relative rotation between a tool and a workpiece, said machine tool having a torque-carrying member, said member including a magnetoelastic torque transducer as claimed in claims 1 or 13.

48. A robotic device comprising mechanical means for performing work pursuant to pre-programmed or real time control instructions, said device having a torque-carrying member, said member including a magnetoelastic torque transducer as claimed in claims 1 or 13.

49. A vehicular steering system having torque-carrying shaft means, said means including a magnetoelastic torque transducer as claimed in claims 1 or 13.

50. A force measuring system including means for converting a sensed force to torque, a torque transducer connected for sensing said torque, said torque transducer comprising a magnetoelastic torque transducer as claimed in claims 1 or 13.

11. A magnetoelastic torque transducer for providing an electrical signal indicative of the torque applied to a member, said member having a ferromagnetic and magnetostrictive region, said transducer comprising:

a pair of axially spaced-apart annular bands defined within a thermally hardened portion of said region, said bands having respectively symmetrical right and left hand helically directed residual stress created magnetic anisotropy instilled therein subsequent to thermal hardening of sufficiently large magnitude compared with the random magnetic anisotropy in said member that the contribution to total magnetic anisotropy of any random anisotropy is negligible, each said band having at least one circumferential region which is free of residually unstressed areas over at least 50% of its circumferential length;

means for applying a cyclically time varying magnetic field to said bands;

means for sensing the change in permeability of said bands caused by said applied torque; and

means for converting said sensed change in permeability to an electrical signal indicative of the magnitude of the torque applied to said member.

12. A magnetoelastic torque transducer, as claimed in claim 11, wherein said region is formed of a steel alloy selected from the group consisting of iron-nickel martensite hardenable and thermally hardened steel alloys characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute.

13. In a magnetoelastic torque transducer for providing an electrical signal indicative of the torque applied to a member including ferromagnetic, magnetostrictive means associated with said member for altering in magnetic permeability in response to the application of torque to said member, means for applying a magnetic field to said ferromagnetic magnetostrictive means, means for sensing the change in permeability caused by said applied torque, and means for converting said sensed change in permeability to an electrical signal indicative of the magnitude of the torque applied to said member, the improvement comprising forming said ferromagnetic, magnetostrictive means from a thermally hardened steel alloy characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute.

14. A magnetoelastic torque transducer, as claimed in claim 13, wherein said alloy further includes from zero up to a useful quantity for imparting desired properties to said alloy of an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vanadium, hafnium, columbium, tantalum, tin, and combinations thereof.

15. A magnetoelastic torque transducer, as claimed in claim 13, wherein said means is formed of a thermally hardened steel alloy consisting essentially of the elements and proportions indicated by the general formula:

space="preserve" listing-type="equation">FeC.sub.a M.sub.b Q.sub.c FeC

wherein;

"M" is an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof;

"Q" is an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vandadium, hafnium, columbium, tantalum, tin and combinations thereof;

"a" indicates a carbon content of from 0.05 to 0.75 percent by weight;

"b" indicates a content of element "M" at least sufficient to raise the magnetostriction of said alloy to at least 5 ppm absolute; and

"c" indicates a content of element "Q" from zero to a useful quantity for imparting desired properties to said alloy.

16. A magnetoelastic torque transducer, as claimed in claim 13, wherein said ferromagnetic, magnetostrictive means forms a part of the surface of said member.

17. A magnetoelastic torque transducer, as claimed in claim 13, wherein said ferromagnetic, magnetostrictive means is rigidly affixed to the surface of said member.

18. A magnetoelastic torque transducer, as claimed in claims 13, 16, or 17, wherein said ferromagnetic, magnetostrictive means is formed of a steel alloy selected from the group consisting of through hardenable and case hardenable steel alloys.

19. A magnetoelastic torque transducer, as claimed in claims 13, 16, or 17, wherein at least a portion of said ferromagnetic, magnetostrictive means is endowed with helically directed residual stress created magnetic anisotropy, at least one circumferential region of said portion being free of residually unstressed areas over at least 50% of its circumferential length, said applying means applying said magnetic field to said endowed portion and to an area of said member not so endowed, said sensing means sensing the permeability difference between said portion and said area resulting from the application of torque to said member, said converting means converting said sensed permeability difference to an electrical signal indicative of the magnitude of the applied torque.

20. A magnetoelastic torque transducer, as claimed in claim 19, wherein said portion is a thermally hardened portion of said ferromagnetic, magnetostrictive means, said residual stress-created magnetic anisotropy having been instilled in said portion subsequent to thermal hardening.

21. A magnetoelastic torque transducer, as claimed in claim 19, wherein said circumferential region is free of residually unstressed areas over at least 80% of its circumferential length.

22. A magnetoelastic torque transducer, as claimed in claim 19, wherein said portion has at least one continuous circumferential region which is free of residually unstressed areas.

23. A magnetoelastic torque transducer, as claimed in claims 13, 16, or 17, wherein said ferromagnetic, magnetostrictive means includes a pair of axially spaced-apart annular bands defined therewithin, said bands having respectively symmetrical right and left hand helically directed residual stress created magnetic anisotropy, each said band having at least one circumferential region which is free of residually unstressed areas over at least 50% of its circumferential length, said applying means applying said magnetic field to said bands, said sensing means sensing the change in permeability of said bands caused by said applied torque.

24. A magnetoelastic torque transducer, as claimed in claim 23, wherein each said band has at least one circumferential region which is free of residually unstressed areas over at least 80% of its circumferential length.

25. A magnetoelastic torque transducer, as claimed in claim 23, wherein each said band has at least one continuous circumferential region which is free of residually unstressed areas.

26. A magnetoelastic torque transducer, as claimed in claim 23, wherein the magnetic easy axes in said bands are oriented, respectively, at angles of ±

20°

-60°

to the axis of said member.

27. A magnetoelastic torque transducer, as claimed in claim 23, wherein said bands are defined within a thermally hardened portion of said means, said residual stress-created magnetic anisotropy having been instilled in said bands subsequent to thermal hardening.

28. A magnetoelastic torque transducer, as claimed in claim 23, wherein said means is formed of a thermally hardened steel alloy consisting essentially of the elements and proportions indicated by the general formula:

space="preserve" listing-type="equation">FeC.sub.a M.sub.b Q.sub.c

wherein;

"M" is an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof;

"Q" is an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vandadium, hafnium, columbium, tantalum, tin and combinations thereof;

"a" indicates a carbon content of from 0.05 to 0.75 percent by weight;

"b" indicates a content of element "M" at least sufficient to raise the magnetostriction of said alloy to at least 5 ppm absolute; and

"c" indicates a content of element "Q" from zero to a useful quantity for imparting desired properties to said alloy.

29. In a method of sensing the torque applied to a member having ferromagnetic, magnetostrictive means associated therewith which includes the steps of applying a magnetic field to said ferromagnetic, magnetostrictive means, sensing the change in permeability caused by said applied torque and converting said sensed change in permeability to an electrical signal indicative of the magnitude of the applied torque, the improvement comprising forming said ferromagnetic, magnetostrictive means of a thermally hardened steel alloy characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute.

30. A method, as claimed in claim 29, wherein said alloy further includes from zero up to a useful quantity for imparting desired properties to said alloy of an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vanadium, hafnium, columbium, tantalum, tin, and combinations thereof.

31. A method, as claimed in claim 29, wherein said steel alloy is selected from the group consisting of through hardenable and case hardenable steel alloys.

32. A method, as claimed in claim 29, wherein said ferromagnetic, magnetostrictive means is endowed with a pair of axially spaced-apart annular bands having respectively symmetrical right and left hand helically directed residual stress-created magnetic anisotropy, the permeability difference between the bands is sensed, and said sensed permeability difference is converted to an electrical signal indicative of the magnitude of the applied torque.

33. A method, as claimed in claim 32, wherein said ferromagnetic, magnetostrictive means is thermally hardened, at least within the region thereof wherein said bands are located, for imparting desirable mechanical properties to the material from which said region is formed and endowing said thermally hardened means with said bands having said residual stress-created anisotropy.

34. In a method of sensing the torque applied to a member having a ferromagnetic and magnetostrictive region including the steps of endowing at least a portion of said region with helically directed residual stress-created magnetic anisotropy, applying a cyclically time varying magnetic field to said portion and to an area of said member not so endowed, and sensing the permeability difference between said portion and said area resulting from the application of torque to said member, the difference being indicative of the magnitude of the applied torque, the improvement comprising forming said region of a thermally hardened steel alloy characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute.

35. A method as claimed in claim 34, wherein said alloy further includes from zero up to a useful quantity for imparting desired properties to said alloy of an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vanadium, hafnium, columbium, tantalum, tin, and combinations thereof.

36. A method as claimed in claim 34, wherein said portion is thermally hardened, at least where said portion is endowed with said magnetic anisotropy, for imparting desirable mechanical properties to the material from which said region is formed, and endowing said thermally hardened portion with said magnetic anisotropy.

37. In a method of sensing the torque applied to a member having a ferromagnetic and magnetostrictive region, including the steps of endowing a pair of axially spaced-apart annular bands within said region with respectively symmetrical right and left hand helically directed magnetic anisotropy, applying a cyclically time varying magnetic field to said bands, and sensing the permeability difference between said bands resulting from the application of torque to said member, the difference being indicative of the magnitude of the applied torque, the improvement comprising:

thermally hardening said member, at least within said region, for imparting desirable mechanical properties to the material from which said region is formed;

defining said bands at the surface of said thermally hardened member; and

,

endowing said bands with magnetic anisotropy by instilling a residual stress distribution in each band which is sufficiently extensive that at least one circumferential region within each band is free of residually unstressed areas over at least 50% of its circumferential length.

38. A method, as claimed in claim 37, wherein said instilled residual stress distribution is sufficiently extensive that said region is free of residually unstressed areas over at least 80% of its circumferential length.

39. A method, as claimed in claim 37, wherein said instilled residual stress distribution is sufficiently extensive that each said band has at least one continuous circumferential region which is free of residually unstressed areas.

40. A method, as claimed in claims 37, 38 or 39, wherein said region is formed of a steel alloy selected from the group consisting of iron-nickel martensite hardenable and thermally hardened steel alloys characterized by a substantially isotropic magnetostriction having an absolute value of at least 5 ppm and including from 0.05 to 0.75 percent by weight carbon and sufficient of an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof to raise said alloy magnetostriction value to said at least 5 ppm absolute.

41. A method as claimed in claim 40, wherein said alloy further includes from zero up to a useful quantity for imparting desired properties to said alloy of an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vanadium, hafnium, columbium, tantalum, tin, and combinations thereof.

42. A method, as claimed in claims 37, 38 or 39, wherein said region is formed of a thermally hardened steel alloy consisting essentially of the elements and proportions indicated by the general formula:

space="preserve" listing-type="equation">FeC.sub.a M.sub.b Q.sub.c

wherein;

"M" is an element selected from the group consisting of nickel, chromium, cobalt, titanium, aluminum, manganese, molybdenum, copper, boron, and combinations thereof;

"Q" is an element selected from the group consisting of silicon, phosphorous, sulfur, nitrogen, selenium, tungsten, vandadium, hafnium, columbium, tantalum, tin and combinations thereof;

"a" indicates a carbon content of from 0.05 to 0.75 percent by weight;

"b" indicates a content of element "M" at least sufficient to raise the magnetostriction of said alloy to at least 5 ppm absolute; and

"c" indicates a content of element "Q" from zero to a useful quantity for imparting desired properties to said alloy.