2014
DOI: 10.1109/tmag.2014.2325405
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Energy Conversion in DC Excited Flux-Switching Machines

Abstract: This paper initiates a study on energy conversion in dc excited flux-switching machines (DCEFSMs) to reveal the torque production mechanism of this type of machines. The flux linkage components and self-and mutual inductances of a single-phase two-rotor-tooth DCEFSM are investigated. Based on the understanding of the relation between these variables and the rotor position, two different switching strategies are implemented to the armature current of this machine. Current-flux linkage loops are sketched for eac… Show more

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Cited by 24 publications
(6 citation statements)
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“…Higher torque and power density are the key features of three-phase FEFSM, having relatively simpler structure [9]. As in FEFSM, all the active parts are present on the stator, thus providing easy cooling mechanism, while at the same time, field excitation provides the controllable flux with the variable flux capabilities [10,11]. In summary, outer rotor has edge over inner rotor providing advantages to completely eliminate drive belts, mechanical transmission, and differential gears.…”
Section: Introductionmentioning
confidence: 99%
“…Higher torque and power density are the key features of three-phase FEFSM, having relatively simpler structure [9]. As in FEFSM, all the active parts are present on the stator, thus providing easy cooling mechanism, while at the same time, field excitation provides the controllable flux with the variable flux capabilities [10,11]. In summary, outer rotor has edge over inner rotor providing advantages to completely eliminate drive belts, mechanical transmission, and differential gears.…”
Section: Introductionmentioning
confidence: 99%
“…1 saturation, the contribution of these inductances to the eletromagnetic torque, T em,tot , is derived using the virtual work method, [7] T em,…”
Section: Torque Ripple Analysismentioning
confidence: 99%
“…Obtained from [38, 39], the torque can be preserved by producing the same magnetomotive force (MMF) with two machine phases in the case of a phase open‐circuit fault. Where the MMF produced by three‐phase currents with (4) is shown in (5)1em4ptIas=Icosfalse(ωt+ϕfalse),Ibs=Icosfalse(ωt+ϕ2π/3false),Ics=Icosfalse(ωt+ϕ+2π/3false),1em4ptMMF=NIas+aNIbs+a2NIcs=32NInormalejθ=32NI(cosθ+jsinθ),wherea=1120, N is the effective number of stator turns per phase and a is the space angle.…”
Section: Fault‐tolerant Drive System During Open Circuitmentioning
confidence: 99%