Maxwell’s Equations in Magnetostatics and Solving with the Curl Operator

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SUMMARY

Maxwell’s equations in magnetostatics, specifically the equation \(\nabla \times \vec{B}=\mu_o \vec{J}_{total}+\mu_o \epsilon_o \dot{\vec{E}}\) with \(\dot{\vec{E}}=0\), are essential for solving magnetostatic problems. The discussion highlights the importance of the magnetic pole model equation \(\vec{B}=\mu_o \vec{H}+ \mu_o \vec{M}\) and addresses the lack of comprehensive resources on these topics. Two specific problems are analyzed: one involving an integral expression for \(\vec{H}\) and another deriving the magnetomotive force (MMF) equation, which is crucial for electrical engineers working with transformers.

PREREQUISITES
  • Understanding of Maxwell's Equations in differential form
  • Familiarity with the concepts of magnetostatic fields
  • Knowledge of vector calculus, particularly the curl operator
  • Basic principles of electromagnetism and magnetic materials
NEXT STEPS
  • Study the derivation and applications of the magnetomotive force (MMF) equation
  • Explore the integral expressions for magnetic fields in magnetostatics
  • Learn about the role of magnetic materials in electromagnetism
  • Investigate advanced vector calculus techniques used in electromagnetism
USEFUL FOR

Electrical engineers, physicists, and students studying electromagnetism who seek a deeper understanding of magnetostatics and its applications in transformer design and analysis.

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Introduction:
Maxwell’s equation in differential form ## \nabla \times \vec{B}=\mu_o \vec{J}_{total}+\mu_o \epsilon_o \dot{\vec{E}}  ##  with ## \dot{\vec{E}}=0 ## comes up quite frequently in magnetostatic problems.  In addition, the equation from the magnetic pole model ## \vec{B}=\mu_o \vec{H}+ \mu_o \vec{M}  ## comes up quite often as well.  It seems the textbooks are somewhat lacking in a thorough treatment of the use of these two equations,  and the mathematical operations that can be used to generate solutions.   In this Insights article,  we will attempt to fill that gap.
In this paper,  we will consider two rather different problems,  which both employ the vector ## \vec{H}  ##.  The first involves an integral expression for ## \vec{H} ##.  The second involves a derivation of the magnetomotive force (MMF) equation.  The EE’s often use this equation in working with transformers.  Here we will show that this MMF equation arises from an alternate form of Maxwell’s/Ampere’s...

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