EMT 2383 Electromagnetic Theory Shamsul Amir bin Abdul

EMT 238/3 Electromagnetic Theory Shamsul Amir bin Abdul Rais 12 September 2011

Basic Info • This is course is implemented 100% through lecture. • The assessment will be as follows: - 70% final exam - 10% mid-term exam, scheduled on 1/11/2011 -20% assignment (lab test, PBL) • You will be broken into several groups for PBL

Basic Preparation • To go through this lecture, you would be needing basic math skills such as calculus, vector, coordinate systems, SI units, dimensions and linear and algebra(matrix, dot & cross product) • The main reference for this subject is “Electromagnetics with Application” Kraus/Fleisch, Mc. Graw-Hill • All lecture notes, teaching plan and other things will be available at portal.

Examples of EM Applications

Dimensions and Units

Fundamental Forces of Nature

Charge: Electrical property of particles Units: coulomb One coulomb: amount of charge accumulated in one second by a current of one ampere. 1 coulomb represents the charge on ~ 6. 241 x 1018 electrons The coulomb is named for a French physicist, Charles-Augustin de Coulomb (1736 -1806), who was the first to measure accurately the forces exerted between electric charges. Charge of an electron e = 1. 602 x 10 -19 C Charge conservation Cannot create or destroy charge, only transfer

Electrical Force exerted on charge 2 by charge 1

Electric Field In Free Space Permittivity of free space

Coulomb’s Law Electric field at point P due to single charge Electric force on a test charge placed at P Electric flux density D

Electric Field Due to 2 Charges

Electric Field due to Multiple Charges

Maxwell’s Equations God said: And there was light!

Current Density For a surface with any orientation: J is called the current density

Convection vs. Conduction

Electric Field Due to Charge Distributions Field due to:

Gauss’s Law Application of the divergence theorem gives:

Applying Gauss’s Law Construct an imaginary Gaussian cylinder of radius r and height h:

Electric Scalar Potential Minimum force needed to move charge against E field:

Electric Scalar Potential

Electric Potential Due to Charges For a point charge, V at range R is: In electric circuits, we usually select a convenient node that we call ground assign it zero reference voltage. In free space and material media, we choose infinity as reference with V = 0. Hence, at a point P For continuous charge distributions:

Relating E to V

Cont.

(cont. )

Poisson’s & Laplace’s Equations In the absence of charges:

Conduction Current Conduction current density: Note how wide the range is, over 24 orders of magnitude

Conductivity ve = volume charge density of electrons he = volume charge density of holes e = electron mobility h = hole mobility Ne = number of electrons per unit volume Nh = number of holes per unit volume

Resistance Longitudinal Resistor For any conductor:

G’=0 if the insulating material is air or a perfect dielectric with zero conductivity.

Joule’s Law The power dissipated in a volume containing electric field E and current density J is: For a resistor, Joule’s law reduces to: For a coaxial cable:

Polarization Field P = electric flux density induced by E

Electric Breakdown

Boundary Conditions

Summary of Boundary Conditions Remember E = 0 in a good conduct

Conductors Net electric field inside a conductor is zero

Field Lines at Conductor Boundary At conductor boundary, E field direction is always perpendicular to conductor surface

Capacitance

Capacitance For any two-conductor configuration: For any resistor:

Application of Gauss’s law gives: Q is total charge on inside of outer cylinder, and –Q is on outside surface of inner cylinder

Electrostatic Potential Energy Electrostatic potential energy density (Joules/volume) Energy stored in a capacitor Total electrostatic energy stored in a volume

Image Method Image method simplifies calculation for E and V due to charges near conducting planes. 1. For each charge Q, add an image charge –Q 2. Remove conducting plane 3. Calculate field due to all charges