T-type flux-switching permanent magnet linear motor and modules of T-type flux-switching permanent magnet linear motor
A technology of permanent magnet linear motor and magnetic flux switching, which is applied in the field of motor manufacturing and electrical engineering, and can solve the unbalanced parameters such as the complementarity of each phase winding and structure, the opposite potential and inductance, and the asymmetry of the positive and negative half cycles of the magnetic flux. And other problems, to achieve the effect of improving fault tolerance, stable motor operation, and improved sine degree
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Embodiment 1
[0036] see figure 1 , The modular complementary flux switching permanent magnet linear motor structure provided by the present invention includes a motor primary 5 and a motor secondary 6 with an air gap between them. Primary 5 and secondary 6 both adopt a salient pole structure. And both the permanent magnet 3 and the winding 2 are on the primary 5, and the secondary 6 is only made of magnetically permeable material, without winding and permanent magnet.
[0037] At this time, when the number of phases m=3, the relative displacement between two adjacent different phases on the same module is 1 / 6τ s , k=4, s=2, λ 1 =9 / 2τ s ,λ 2 =13 / 6τ s , τ m =τ s .
[0038] The motor primary 5 includes T-shaped units 7, a total of N*m, each i T-shaped units 7 form a module, N is the number of coils in each phase winding, and i is a positive integer. And the non-magnetic conductive block 4 is used to fill the space between two adjacent modules 1 . Each T-shaped unit 7 consists of two...
Embodiment 2
[0045] Such as figure 2 As shown, when m=3, the relative displacement between two adjacent out-of-phase on the same module is 1 / 3τ s , k=4, s=2, λ 1 =4τ s ,λ 2 =11 / 6τ s , τ m =1 / 2τ s . The difference between the modular complementary magnetic flux switching permanent magnet linear motor in this embodiment and that in Embodiment 1 is that the motor is composed of four T-shaped units to form a module, and there are 3 modules in total. The width of the non-magnetic block 4 between two adjacent modules 1 becomes half of the original, that is, τ m =1 / 2τ s , τ m is the width of the non-magnetic block, τ s is the secondary pole distance, and at this time, the relative displacement between two adjacent out-of-phase on a module is (1 / m)*τ s. The winding method is still in accordance with the "ABCABC..." three-phase sequential winding, but the winding direction of the second module is completely opposite to that of the other two modules, and the following two conditions mus...
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