2020
DOI: 10.48084/etasr.3678
|View full text |Cite
|
Sign up to set email alerts
|

Accurate Magnetic Shell Approximations with Magnetostatic Finite Element Formulations by a Subdomain Approach

Abstract: This paper presents a subproblem approach with h-conformal magnetostatic finite element formulations for treating the errors of magnetic shell approximation, by replacing volume thin regions by surfaces with interface conditions. These approximations seem to neglect the curvature effects in the vicinity of corners and edges. The process from the surface-to-volume correction problem is presented as a sequence of several subdomains, which can be composed to the full domain, including inductors and thin magnetic … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
3
0

Year Published

2021
2021
2022
2022

Publication Types

Select...
5

Relationship

3
2

Authors

Journals

citations
Cited by 7 publications
(3 citation statements)
references
References 15 publications
0
3
0
Order By: Relevance
“…IV. CONCLUSION The current paper has developed stator and rotor embrace/pitch influenced on the average torque and torque ripples via FEM [10,11]. For high speed of the SRM, the control method is single voltage or current pulse because the magnetic circuit is saturated.…”
Section: Dynamic Simulation and Experimental Resultsmentioning
confidence: 99%
“…IV. CONCLUSION The current paper has developed stator and rotor embrace/pitch influenced on the average torque and torque ripples via FEM [10,11]. For high speed of the SRM, the control method is single voltage or current pulse because the magnetic circuit is saturated.…”
Section: Dynamic Simulation and Experimental Resultsmentioning
confidence: 99%
“…Hence, the displacement current density is negligible. The problem is described by Maxwell's equations [11][12][13][14][15][16]:…”
Section: A Canonical Magnetodynamic Problemmentioning
confidence: 99%
“…Based on the Maxell's equations along with the constitutive relations in (22), the weak form of Ampere' law (22b) is written [5,11,13] as: In order to satisfy strongly the lower part of the Tonti's diagram [14], the constitutive laws (23 a-b) have to be introduced in (12), i.e. :…”
Section: B Magnetic Vector Potential Formulationsmentioning
confidence: 99%