Chapter 4: Electroquasistatic fields: the superposition integral point of view (PDF)
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
| DEMONSTRATION TOPICS |
VIDEOS - SHORT FORM |
VIDEOS - LONG FORM |
|---|---|---|
| 4.7.1: Charge induced in ground plane by overhead conductor | Chapter 4.7.1: Charge Induced in Ground Plane by Overhead Conductor (demo only) | Chapter 4.7.1: Charge Induced in Ground Plane by Overhead Conductor |
