Chapter 4: Electroquasistatic fields: the superposition integral point of view
recorded by: Massachusetts Institute of Technology, MIT
published: Oct. 10, 2008, recorded: September 2005, views: 4148
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Description
4.0 Introduction 4.1 Irrotational field represented by scalar potential: the gradient operator and the gradient integral theorem
- Visualization of two-dimensional irrotational fields
4.2 Poisson's equation 4.3 Superposition principle 4.4 Fields associated with charge singularities
- Dipole at the origin
- Pair of charges at infinity having equal magnitude and opposite sign
- Other charge singularities
4.5 Solution of Poisson's equation for specified charge distributions
- Superposition integral for surface charge density
- Superposition integral for line charge density
- Two-dimensional charge and field distributions
- Potential of uniform dipole layer.
4.6 Electroquasistatic fields in the presence of perfect conductors
- Capacitance
4.7 Method of images
4.8 Charge simulation approach to boundary value problems
4.9 Summary
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