# Electromagnetic Theory Lecture Notes Pdf

As before, we consider two cases i. Electrostatics can be defined as the study of electric charges at rest.

Example of scalar field is the electric potential in a region while e lectric or magnetic fields at any point is the example of o f vector field. Calculate the energy and potential due to a system of charges.

Polarization of dielectric Here we briefly describe the behavior of dielectrics or insulators when placed in static electric field. The flux density vector is defined to be independent of the material media as we'll see that it relates to the charge that is producing it. In this chapter we will consider the time varying scenario. An infinitely long conductor carries a current I A is bent into an L shape and placed as shown in Fig. For a good dielectric medium is very small and the medium is a good conductor if.

Quarks were predicted to carry a fraction of electronic charge and the existence of Quarks have been exper imentally verified. In terms of these current distributions. Both these law have experimental basis.

The conductors may have arbitrary shapes. For example, the number of flux lines passing through a unit surface S normal to the vector measures the vector field strength. To evaluate the energy and potential due to a system of charges. Since the line charge is assumed to be infinitely long, the electric field will be of the form as shown in Fig. By symmetry, the equipotential surfaces are spherical surfaces and the equipotential lines are circles.

Electromagnetic waves can transport energy from one point to another point. We begin our discussion with Faraday's Law of electromagnetic induction and then present the Maxwell's equations which form the foundation for the electromagnetic theory. Vector analysis is a mathematical mathematical tool with w ith which electromagnetic concepts are more conveniently expressed a nd best comprehended. Portfolio Theory Lecture Notes Concise notes for lecture on portfolio theory to undergrad finance majors.

Almost all real electric fields vary to some extent with time. Dielectric constant may be a function of space coordinates.

The vector or cross product of two vectors and is denoted by. We may further note that charges require a finite time to redistribute in a conductor. In polar molecules the atoms do not arrange themselves to make the net dipole moment zero. This results in frictional damping mechanism causing power loss.

If function of the vector function depends on the direction of is called the scalar potential. In doing so we note that and it applies for other components as well. The integration of the Poynting vector over any closed surface gives the net power flowing out of the surface. About Welcome to EasyEngineering, One of the trusted educational blog. No work is done in moving a charge from one point to the other along an equipotential line or surface.

The intersection of an equipotential surface with an plane surface results into a path called an equipotential line. It is an idealised model of a particle having an electric charge. The current continues to increase till the flux in the core and the induced emfs are restored to the no load values. For some other cases spatial distribution is nearly same as for the static case even though the actual field may vary with time. Further, if called uniaxial. Boundary conditions can be derived by applying the Maxwell's equations in the integral form to small regions at the interface of the two media. Our partners will collect data and use cookies for ad personalization and measurement. Polarised Dielectric Medium n being the number of molecules per unit volume i.

## Electromagnetic Theory Pdf Notes - EMT Pdf Notes

Thus if of a given current distribution, We have introduced the vector function can be found from and related its curl to through a curl operation. Therefore we may replace a polarized dielectric by an equivalent polarization surface charge density and a polarization volume charge density.  