Chapter 8: Magnetoquasistatic fields: superposition integral and boundary value points of view
recorded by: Massachusetts Institute of Technology, MIT
published: Oct. 10, 2008, recorded: September 2005, views: 5270
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Watch videos: (click on thumbnail to launch)
Part 1: 8.2.1: Field of a circular cylindrical solenoid 04:28
Part 2: 8.2.2: Field of square pair of coils 04:11
Part 3: 8.4.1: Surface used to define the flux linkage 04:16
Part 4: 8.5.1: Field and inductance of a spherical coil 04:45
Part 5: 8.6.1: Surface currents induced in ground plane by overhead conductor 05:12
Part 6: 8.6.2: Inductive attenuator 05:17
Description
8.0 Introduction
- Vector field uniquely specified
8.1 The vector potential and the vector Poisson equation
- Two-dimensional current and vector potential distributions
8.2 The Biot-Savart superposition integral
- Stick model for computing fields of electromagnet
8.3 The scalar magnetic potential
- The scalar potential of a current loop
8.4 Magnetoquasistatic fields in the presence of perfect conductors
- Boundary conditions and evaluation of induced surface current density
- Voltage at the terminals of a perfectly conducting coil
- Inductance
8.5 Piece-wise magnetic fields 8.6 Vector potential and the boundary value point of view
- Vector potential for two-dimensional fields
- Vector potential for axisymmetric fields in spherical coordinates
- Boundary value solution by "Inspection"
- Method of images
- Two-dimensional boundary value problems
8.7 Summary
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