Hall effect apparatus for determining the angular position of a rotating part

• US 4,086,533 A
• Filed: 11/08/1976
• Issued: 04/25/1978
• Est. Priority Date: 11/12/1975
• Status: Expired due to Term

• Current Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Ricouard, Jean-Pierre, Schorter, Bruno
• Primary Examiner(s): Corcoran, Robert J.
• Application Number:
  US05/740,004
• Time in Patent Office: 533 Days
• Field of Search: 324/34 D, 324/34 PS, 324/45, 324/46, 338/32 R, 338/32 H, 323/94 H, 310/68 B, 310/111, 310/168
• US Class Current: 324/207.2
• 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 5/20 by varying inductance, e.g. by a movable armature
• CPC Class Codes: Y10S 310/03 Hall effect generators and converters

Abstract

A device for determining the angular position of a rotating part includes first and second parallel arranged magnets forming a symmetric magnetic excitation circuit with a Hall-effect element disposed on the axis thereof. The rotating part has first and second elements made of a soft magnetic material which are angularly displaced so as to alternately pass by the first and second magnets, respectively, to produce first and second oppositely directed transverse magnetic field components, H, at the Hall-effect element which thereby generates a signal whose polarity reverses to indicate angular position of the rotating part.

Claims

1. A device for detecting the specific angular positions of a rotating part comprising, a Hall-effect crystal, a fixed magnetic circuit for exciting the Hall-effect crystal which circuit includes two identical permanent magnets which are disposed at a small distance from and substantially parallel to each other and having adjacent poles of like magnetic polarity situated in proximity to the Hall-effect crystal to apply a magnetic excitation field thereto, said fixed magnetic circuit having an axis of symmetry along which the crystal is disposed, said rotating part including first and second soft-magnetic elements respectively located on opposite sides of said axis of symmetry and each having a leading end and a trailing end defined by the direction of travel of the rotating part, said first and second soft magnetic elements being relatively displaced so that the trailing end of one soft magnetic element coincides with the leading end of the other soft magnetic element and movement of the rotating part causes said first and second soft magnetic elements to successively and alternately pass in the proximity of said adjacent poles, a first soft-magnetic element which passes one of the magnets near its said adjacent pole being immediately followed by a second soft-magnetic element which passes the other magnet near its said adjacent pole to cause a reversal in the direction of the active component of the magnetic excitation field whereby the Hall-effect cyrstal responds by reversing the polarity of an output signal generated therein.

2. A device as claimed in claim 1 further comprising an auxiliary part from which the soft magnetic elements project from the body of said auxiliary part.

3. A device as claimed in claim 1 further comprising a printed circuit board, a preamplifier coupled to the Hall-effect crystal, the Hall-effect crystal and the preamplifier forming a part of an integrated circuit mounted to the printed circuit board, the fixed magnetic circuit and the printed circuit board with crystal and preamplifier being encapsulated in a block of a synthetic resin to which aluminum oxide powder is added and which is tinted.

4. A device for detecting the position of a moving part comprising, a Hall-effect crystal for generating an output voltage dependent upon an active component of a magnetic field in which the crystal is located, a fixed magnetic circuit for exciting the Hall-effect crystal and comprising first and second magnetic members symmetrically disposed so as to define a gap between adjacent ends thereof and an axis of symmetry in said gap, said adjacent ends defining magnetic poles of like polarity with said Hall-effect crystal disposed in said gap and subject to a magnetic excitation field produced therein by said first and second magnetic members, said moving part including first and second soft magnetic elements respectively located on opposite sides of said axis of symmetry and each having a leading end and a trailing end defined by the moving part, said first and second soft magnetic elements being relatively displaced so that the trailing end of one soft magnetic element coincides with the leading end of the other soft magnetic element and movement of the moving part causes said first and second soft magnetic elements to successively and alternately pass in proximity to said first and second magnetic members, the alternate passage of said soft magnetic elements past said first and second magnetic members causing a reversal in the direction of the active component of the magnetic excitation field acting upon the Hall-effect crystal which responds by generating an output voltage with a zero crossing which provides an indication of the position of the moving part.

5. A device as claimed in claim 4 wherein said first and second magnetic members comprise first and second permanent magnets spaced apart and in parallel having adjacent pole ends of like polarity and with the Hall-effect crystal located along said axis of symmetry and in the vicinity of said adjacent pole ends.

6. A device as claimed in claim 4 wherein said moving part is rotatable about an axis that is parallel to the active component of the gap magnetic field in the vicinity of the Hall-effect crystal and said first and second soft magnetic elements are axially displaced relative to one another along the axis of rotation.

7. A device as claimed in claim 4 wherein said moving part comprises a rotatable member and said first and second soft magnetic elements each have a pair of circular peripheral edge portions of at most 90°

each and with the circular peripheral edge portions of the first and second soft magnetic elements circumferentially displaced.