Maxwell Equations Dr. Anurag Srivastava

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1 Maxwell Equations Dr. Anurag Srivastava Web address: Visit me: Room-110, Block-E, IIITM Campus

2 Syllabus Electrodynamics: Maxwell s equations: differential and integral forms, significance of Maxwell s equations, displacement current and correction in Ampere s law, electromagnetic wave propagation, transverse nature of EM waves, wave propagation in bounded system, applications. Quantum Physics: Dual nature of matter, de-broglie Hypothesis, Heisenberg uncertainty principle and its applications, postulates of quantum mechanics, wave function & its physical significance, probability density, Schrodinger s wave equation, Eigen values & Eigen functions, Applications of Schrodinger equation. 2

3 Prerequisite E & M

4 The History of Electromagnetics The history of electromagnetics shows that it is a series of discoveries of many people instead of by just one person.

5 Early Electromagnetics Amber The ancient Greeks realized that it attracts chaff and feather particles. Loadstone A naturally magnetized mineral; magnetite. Chinese used it properties to invent the compass.

6 Charles Coulomb He was a civil engineer in the French army, but had to quit due to illness. He discovered that electric forces obey the same inverse square law Newton discovered.

7 Alessandro Volta Learned that body tissue could conduct electricity from his friend Galvini. Discovered that all metals could conduct electricity. Created the voltaic pile as the first continuous electric power source.

8 André-Marie Ampère Early in life his father was beheaded during the French Revolution. After Orsted discovered in 1820 that electricity induced magnetism he wrote a mathematical paper to describe the behavior in one week.

9 Michael Faraday, early life Grew up in a poor family in England. He received very little formal education. Read many books as an apprentice bookbinder and did experiments in the shop. After attending a lecture by Humphrey Davy he was hired as a lab assistant.

10 Michael Faraday, later life While Faraday made discoveries Davy became jealous and tried to take credit. Knew that electricity could produce magnetism, but could magnetism produce Electricity?

11 James Clerk Maxwell (Dafty) Born into a wealthy family in Edinburgh. Was well educated and inquisitive. Went to Cambridge college, but moved to Trinity for competitive reasons. Was a professor at Trinity, Aberdeen, and London. Put Faraday s Law in mathematical form. Discovered the famous 4 equations that govern electromagnetics. Devout Christian.

12 Quantities In mathematics there are two types of quantities: Vector: Direction + Magnitude Scalar: Only Magnitude Gradient: An operator in vector calculus.

13 Two key concepts in vector calculus are divergence and curl, the latter of which is sometimes called circulation. Basically, divergence has to do with how a vector field changes its magnitude in the neighborhood of a point, and curl has to do with how its direction changes.

14

15 Materials Comprises of many atoms. Atoms have neutron, proton and electrons. Protons are positively charged. Electrons are negatively charged. Interactions among the particles through long range as well as short range forces. Electrons

16 Current Flow of electrons per unit time is called current. Two types: Direct current- electrons flow in same direction Alternating current- electrons flow in different direction

17 Circuit Path for the flow of electrons Three types Series: Parallel: Hybrid

18 Voltage Voltage is defined as the electromotive force or the electric potential energy difference between two points (often within the context of an electrical circuit) per unit of charge. Expressed in volts (V).

19 Coulomb's law Force on a test charge Q1 due to a single point charge Q2, is given by

20 Electric Field Intensity

21 Charge distribution Total charge due to these distributions are given by:

22 Electric flux

23 Flux For a Closed Area Then flux is given by:

24 Permittivity Measure of a material's ability to resist an electric field. Denoted by the symbol.

25

26 Gauss law of electric fields The total of the electric flux out of a closed surface is equal to the charge enclosed divided by the permittivity.

27 Magnetism Is a physical phenomenon produced by the motion of electric charge, which results in attractive and repulsive forces between objects. Magnetic Field Is a region around a magnetic material or a moving electric charge within which the force of magnetism acts. Magnet produces magnetic force and have magnetic field lines.

28 Magnets Magnets have two poles. North pole South pole Opposite pole attract each other Similar pole repel each other.

29 Permeability Is the degree of magnetization that a material obtains in response to an applied magnetic field Tells, how easily an external magnetic field can induce an internal field in the material Where, B = induced magnetic field H = externally applied magnetic field

30 Gauss law of Magnetism The net magnetic flux out of any closed surface is zero. For any closed surface,the magnetic flux directed inward toward the south pole will equal the flux outward from the north pole.

31 Electromagnetism Moving charge create a magnetic field in the direction perpendicular to the current. Direction of magnetic field is given by right hand rule. Thumb- direction of current Fingers direction of magnetic field.

32 Faraday s Law Any change in the magnetic field of a coil of wire will cause an EMF to be induced in the coil. This EMF induced is called induced EMF and if the conductor circuit is closed, the current will also circulate through the circuit and this current is called induced current. dl =

33 Ampere Law Magnetic field created by an electric current is proportional to the current with constant of proportionality equal to the permeability of free space. d l

34 Maxwell Equations Differential form of Maxwell s equations Integral form of Maxwell s equations

35 Physical Significance Of Maxwell Equations Gauss law of electric fields: It tells us that electric field origins from electric charge. Gauss law of magnetic fields: tells us that magnetic monopoles do not exist. Faradays law: Any change in magnetic flux across some closed path generates e.m.f. Ampere s law: Electric current generates magnetic field

36 Integral form of Maxwell Equation

37 Integral form of Maxwell Equation

38 Integral form of Maxwell Equation

39 Integral form of Maxwell Equation

40 Integral form of Maxwell Equation

41 Integral form of Maxwell Equation

42 Differential form of Maxwell Equation Fundamentals of Electrical EnginPHYring 42

43 Difference between differential and integral form of Maxwell Equation Fundamentals of Electrical EnginPHYring 43

44 Difference between differential and integral form of Maxwell Equation The equations are entirely equivalent, as can be proven using Gauss' and Stokes' theorems. The integral forms are most useful when dealing with macroscopic problems with high degrees of symmetry (e.g. spherical or axial symmetry; or, following on from comments below, a line/surface integrals where the field is either parallel or perpendicular to the line/surface element). The differential forms are strictly local - they deal with charge and current densities and fields at a point in space and time. The differential forms are far easier to manipulate when dealing with electromagnetic waves; they make it far easier to show that Maxwell's equations can be written in a covariant form, compatible with special relativity; and far easier to put into a computer to do numerical electromagnetism calculations. Fundamentals of Electrical EnginPHYring 44

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