Matches in SemOpenAlex for { <https://semopenalex.org/work/W1497325486> ?p ?o ?g. }
Showing items 1 to 93 of
93
with 100 items per page.
- W1497325486 abstract "Traditional design/prototype/test cycles have improved the efficiencies of small induction motors to high levels. To achieve still higher efficiencies, motor performance must be studied in a more detailed and integrated manner. The authors present a nonlinear, time-dependent computer simulaton modeling the performance of a permanent-splitcapacitor induction motor. The effects of nonlinear permeability and time varying terminal voltages are included in the model. Two-dimensional finite element magnetic field equations are coupled with the electri~: circuit equations and solved using the Newton-Raphson and Crank-Nicholson methods. The simulation predicts main and aWJ;iliary winding cur· rents, induced rotor currents, hysteresis losses and motor torque as functions of time. Due to the detailed nature of the results a deeper understanding of motor perfonnance factors, normally difficult to determine, can be obtained. INTRODUCTION Induction motor design involves the prediction and evaluation of performance parameters such as torque, line current and losses at any given slip and tenninal conditions. These parameters can be accurately determined only with knowledge of the magnetic field distribution within the machine. Approximate analytical methods [I] have been used in the past with some success. Continued pressure to conserve energy dictates improved motor performance. This requires an even more detailed knowledge of the magnetic fields occurring within motors. Two-dimensional statioruu:y magnetic field problems have been investigated by many authors [2,3]. The nonlinear penneability or saturation characteristics of steel require iterative methods for the solution of these problems. Tandon, Armor and Chari [4] were first to combine the Newton· Rapbson technique with the CrankNicholson central difference scheme to solve transient field problems in electrical machines. The disadvantage of these methods is that they rely on apriori knowledge of the c~ts or current densities in the device. The problem is much more complicated when current densities are unknown and terminal conditions must be considered. Potter and Cambrell [S] combined a twe>dimensional finite element field solution and circuit equations to simulate an indu~:tion motor. In their work the stator field was rq>laced with a current sbeet at slip ftequency. Strangas and Theis [6] also combined the finite element field solution with circuit equations to model a shaded-pole motor. Their approach used a time-dependent grid for rotor movement. This paper expands the above techniques to model a pennanent-splitA capacitor induction motor. The two-dimensional magnetic field equations are combined with electric circuit equations describing end and elCtemal effects. The partial derivatives" @default.
- W1497325486 created "2016-06-24" @default.
- W1497325486 creator A5066586869 @default.
- W1497325486 creator A5085577101 @default.
- W1497325486 date "1992-01-01" @default.
- W1497325486 modified "2023-09-26" @default.
- W1497325486 title "Induction Motor Modeling Using Coupled Magnetic Field and Electric Circuit Equations" @default.
- W1497325486 cites W2001325695 @default.
- W1497325486 cites W2021883393 @default.
- W1497325486 cites W23775177 @default.
- W1497325486 hasPublicationYear "1992" @default.
- W1497325486 type Work @default.
- W1497325486 sameAs 1497325486 @default.
- W1497325486 citedByCount "2" @default.
- W1497325486 countsByYear W14973254862013 @default.
- W1497325486 crossrefType "journal-article" @default.
- W1497325486 hasAuthorship W1497325486A5066586869 @default.
- W1497325486 hasAuthorship W1497325486A5085577101 @default.
- W1497325486 hasConcept C115260700 @default.
- W1497325486 hasConcept C119599485 @default.
- W1497325486 hasConcept C121332964 @default.
- W1497325486 hasConcept C124162555 @default.
- W1497325486 hasConcept C127413603 @default.
- W1497325486 hasConcept C135628077 @default.
- W1497325486 hasConcept C144171764 @default.
- W1497325486 hasConcept C154945302 @default.
- W1497325486 hasConcept C158622935 @default.
- W1497325486 hasConcept C165801399 @default.
- W1497325486 hasConcept C17281054 @default.
- W1497325486 hasConcept C173161252 @default.
- W1497325486 hasConcept C176871988 @default.
- W1497325486 hasConcept C177500038 @default.
- W1497325486 hasConcept C2775924081 @default.
- W1497325486 hasConcept C41008148 @default.
- W1497325486 hasConcept C47446073 @default.
- W1497325486 hasConcept C57879066 @default.
- W1497325486 hasConcept C62520636 @default.
- W1497325486 hasConcept C66938386 @default.
- W1497325486 hasConcept C71376005 @default.
- W1497325486 hasConcept C78519656 @default.
- W1497325486 hasConcept C80962145 @default.
- W1497325486 hasConcept C97355855 @default.
- W1497325486 hasConceptScore W1497325486C115260700 @default.
- W1497325486 hasConceptScore W1497325486C119599485 @default.
- W1497325486 hasConceptScore W1497325486C121332964 @default.
- W1497325486 hasConceptScore W1497325486C124162555 @default.
- W1497325486 hasConceptScore W1497325486C127413603 @default.
- W1497325486 hasConceptScore W1497325486C135628077 @default.
- W1497325486 hasConceptScore W1497325486C144171764 @default.
- W1497325486 hasConceptScore W1497325486C154945302 @default.
- W1497325486 hasConceptScore W1497325486C158622935 @default.
- W1497325486 hasConceptScore W1497325486C165801399 @default.
- W1497325486 hasConceptScore W1497325486C17281054 @default.
- W1497325486 hasConceptScore W1497325486C173161252 @default.
- W1497325486 hasConceptScore W1497325486C176871988 @default.
- W1497325486 hasConceptScore W1497325486C177500038 @default.
- W1497325486 hasConceptScore W1497325486C2775924081 @default.
- W1497325486 hasConceptScore W1497325486C41008148 @default.
- W1497325486 hasConceptScore W1497325486C47446073 @default.
- W1497325486 hasConceptScore W1497325486C57879066 @default.
- W1497325486 hasConceptScore W1497325486C62520636 @default.
- W1497325486 hasConceptScore W1497325486C66938386 @default.
- W1497325486 hasConceptScore W1497325486C71376005 @default.
- W1497325486 hasConceptScore W1497325486C78519656 @default.
- W1497325486 hasConceptScore W1497325486C80962145 @default.
- W1497325486 hasConceptScore W1497325486C97355855 @default.
- W1497325486 hasLocation W14973254861 @default.
- W1497325486 hasOpenAccess W1497325486 @default.
- W1497325486 hasPrimaryLocation W14973254861 @default.
- W1497325486 hasRelatedWork W2025423331 @default.
- W1497325486 hasRelatedWork W2045406432 @default.
- W1497325486 hasRelatedWork W2102321867 @default.
- W1497325486 hasRelatedWork W2119998170 @default.
- W1497325486 hasRelatedWork W2293219398 @default.
- W1497325486 hasRelatedWork W2622805980 @default.
- W1497325486 hasRelatedWork W2765640001 @default.
- W1497325486 hasRelatedWork W2950756797 @default.
- W1497325486 hasRelatedWork W2962964071 @default.
- W1497325486 hasRelatedWork W2999472216 @default.
- W1497325486 hasRelatedWork W3007196832 @default.
- W1497325486 hasRelatedWork W3139039560 @default.
- W1497325486 hasRelatedWork W3141595479 @default.
- W1497325486 hasRelatedWork W3144905433 @default.
- W1497325486 hasRelatedWork W3149407062 @default.
- W1497325486 hasRelatedWork W3151403528 @default.
- W1497325486 hasRelatedWork W3151992398 @default.
- W1497325486 hasRelatedWork W3173846923 @default.
- W1497325486 hasRelatedWork W3209769409 @default.
- W1497325486 hasRelatedWork W59192453 @default.
- W1497325486 isParatext "false" @default.
- W1497325486 isRetracted "false" @default.
- W1497325486 magId "1497325486" @default.
- W1497325486 workType "article" @default.