Electromagnetic Theory: Unit II: (c) Poissons and Laplaces Equations
Introduction
Poissons and Laplaces Equations
To solve such problems, Poisson's and Laplace's equations must be known. This chapter derives the Poisson's and Laplace's equations and explains its use in few practical situations.
Introduction
•
In earlier chapters, the 
in the given region are obtained using
Coulomb's law and Gauss's law. Using these laws is easy, if the charge
distribution or potential throughout the region is known. Practically it is not
possible in many situations, to know the charge distribution or potential
variation throughout the region. Practically charge and potential may be known
at some boundaries of the region, only. From those values it is necessary to
obtain potential and 
throughout the region. Such electrostatic problems
are called boundary value problems. To solve such problems, Poisson's and
Laplace's equations must be known. This chapter derives the Poisson's and
Laplace's equations and explains its use in few practical situations.
Electromagnetic Theory: Unit II: (c) Poissons and Laplaces Equations : Tag: : Poissons and Laplaces Equations - Introduction
Electromagnetic Theory: Unit II: (c) Poissons and Laplaces Equations
Under Subject
Electromagnetic Theory
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