Magnetization state control method and magnetization state control device
US-2018219504-A1 · Aug 2, 2018 · US
US11011965B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11011965-B2 |
| Application number | US-201515747879-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 31, 2015 |
| Priority date | Jul 31, 2015 |
| Publication date | May 18, 2021 |
| Grant date | May 18, 2021 |
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A permanent magnet synchronous motor includes a stator, a rotor rotatable relative to the stator, and a magnetic structure with a low coercive force magnet and a high coercive force magnet that are arranged magnetically in series with respect to each other to define a pole-pair of the permanent magnet synchronous motor. A magnetization level of the low coercive force magnet is changeable by a stator current pulse such that a stator magnetomotive force at a rated current is equal to or larger than a product of a magnetic field strength for fully magnetizing the low coercive force magnet and a thickness of the low coercive force magnet.
Opening claim text (preview).
What is claimed is: 1. A permanent magnet synchronous motor comprising: a stator; a rotor rotatable relative to the stator; and a magnetic structure with a low coercive force magnet and a high coercive force magnet that are arranged magnetically in series with respect to each other to define a pole-pair of the permanent magnet synchronous motor, a magnetization level of the low coercive force magnet being changeable by a stator current pulse, and a rated current of the permanent magnet synchronous motor being set such that a stator magnetomotive force at the rated current is equal to or larger than a product of a magnetic field strength for fully magnetizing the low coercive force magnet and a thickness of the low coercive force magnet. 2. The permanent magnet synchronous motor according to claim 1 , wherein the stator, the rotor and the magnetic structure are further configured to satisfy the following formula (1): M M F ≥ H M ax t Low - J High μ 0 μ rh t High + ( J Max μ 0 μ rl + H Max ) ( t High + t g ) ( 1 ) where MMF represents the stator magnetomotive force per pole at the rated current, H Max represents the magnetic field strength for fully magnetizing the low coercive force magnet, t Low represents a thickness of the low coercive force magnet, J High represents a magnetization of the high coercive force magnet, μ 0 μ rh represents a magnetic permeability of the high coercive force magnet, μ 0 μ rh represents a magnetic permeability of the low coercive force magnet, t High represents a thickness of the high coercive force magnet, J Max represents a magnetization of the low coercive force magnet fully magnetized, and t g represents an air gap length between the stator and the rotor. 3. The permanent magnet synchronous motor according to claim 1 , wherein the stator, the rotor and the magnetic structure are further configured to satisfy the following formula (2): M M F ≥ - H Min t Low + J High μ 0 μ rh t High - ( J Min μ 0 μ rl + H Min )
Magnets embedded in the magnetic core, e.g. interior permanent magnets [IPM] · CPC title
Magnets shaped to vary the mechanical air gap between the magnets and the stator · CPC title
using magnetic devices with controllable degree of saturation, e.g. transductors · CPC title
for demagnetising; for reducing effects of remanence · CPC title
Arrangements for controlling the speed or torque of a single motor (H02P6/10, H02P6/28 take precedence) · CPC title
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