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[NOTES/EM-12002]-Electromagnetic Field Tensor and Maxwell's equationsNode id: 5759page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
The field tensor for the electromagnetic fields is defined in terms of the vector potential. It components are expressed in terms of the electric and magnetic fields. The Maxwell's equations are written down in relativistic notation.
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23-03-03 21:03:14 |
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[NOTES/EM-12001]-Lorentz transformations Node id: 5757page
The basic equations of Maxwell's theory are written down in relativistic notation. Using Lorentz transformations of the potentials, the expressions of the scalar and vector potentials of a point charge moving with a uniform velocity are obtained.
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23-03-03 21:03:55 |
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[NOTES/EM-11004]-Wave Equation for FieldsNode id: 5756page
The Maxwell's equations in vacuum, in absence of charges and currents are written and are shown to imply wave equation for the electric and magnetic fields. The plane wave solutions, the electromagnetic waves, are shown to travel with a velocity equal to \(1/\sqrt{\mu_0\epsilon_0}\). The numerical value of this expression equals the velocity of light. This leads to the identification of light as electromagnetic waves.
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23-03-03 21:03:01 |
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[NOTES/EM-11003]-Electromagnetic waves in vacuumNode id: 5755page
The plane wave solution of wave equation for free fields in vacuum is obtained. It is proved that the electric and magnetic fields are mutually perpendicular and both ar perpendicular to the direction of propagation. It shown that the amplitudes of the electric and magnetic fields obey the relation \(|\vec{E}_0|=c|\vec{B}_0|\).
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23-03-03 21:03:44 |
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[NOTES/EM-11002]-Energy Density of Free Electromagnetic WavesNode id: 5754page
The Poynting theorem gives an expression for energy density and rate of flow of energy across a surface. Using these expressions, the energy density and other quantities are computed for plane wave solutions.
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23-03-03 21:03:31 |
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[NOTES/EM-11001]-Electromagnetic Potentials in ElectrodynamicsNode id: 5753page
The vector and scalar potentials are defined in terms of the fields. Using the Maxwell's equations the wave equation for the potentials are derived in the Lorentz gauge.
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23-03-03 21:03:15 |
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[NOTES/EM-10005]-Maxwell's Fourth Equation, Displacement CurrentNode id: 5738page $\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
Two problems with,Ampere's law and charge conservation, Maxwell's equations for time varying field are discussed. Maxwell modified the fourth equation by adding a displacement current.
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23-03-03 21:03:36 |
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[NOTES/EM-10006]-Maxwell's Fourth Equation, Displacement CurrentNode id: 5739page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
We discuss how Maxwell's addition of a displacement current in the fourth equation.
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23-03-03 21:03:00 |
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[NOTES/EM-10010]-Wave Equation in Free SpaceNode id: 5745page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
In absence of any medium and in free space, \(\rho=0, \vec{j}=0\), it is proved that the electric and magnetic fields satisfy wave equation.
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23-03-03 20:03:13 |
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[NOTES/EM-10007]-Time Varying Fields ,Ampere's LawNode id: 5740page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
We explain how Maxwell's addition of a displacement current in the fourth equation.
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23-03-03 20:03:30 |
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[NOTES/EM-10008]-Maxwell's Equations for Time Varying Fields and Ampere's LawNode id: 5743page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
Several concepts and results valid for static fields need revision when one is considering the situation of time varying fields. Some of these are discussed here
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23-03-03 20:03:05 |
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[NOTES/EM-10009]-A Summary Maxwell's EquationsNode id: 5744page$\newcommand{\DD}[2][]{\frac{d^2 #1}{d^2 #2}}$ $\newcommand{\matrixelement}[3]{\langle#1|#2|#3\rangle}$ $\newcommand{\PP}[2][]{\frac{\partial^2 #1}{\partial #2^2}}$ $\newcommand{\dd}[2][]{\frac{d#1}{d#2}}$ $\newcommand{\pp}[2][]{\frac{\partial #1}{\partial #2}}$ $\newcommand{\average}[2]{\langle#1|#2|#1\rangle}$
An overview of how Maxwell's equations for static and time varying field is given. The changes needed from static to time varying case are emphasized.
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23-03-03 20:03:38 |
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[NOTES/EM-07010]-Magnetic Field of a Current Distribution at a Large DistancesNode id: 5715page
For a volume distribution of current an expression for magnetization density,{\it i.e.} the magnetic moment per unit volume, is obtained. An expression for the magnetic field at large distances, in terms of magnetization density, is derived.
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23-03-03 20:03:07 |
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[NOTES/EM-07007]-Cross product ruleNode id: 5712page
in this section the rule about the direction of cross product the cross product of two vectors is explained.
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23-03-03 20:03:55 |
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[NOTES/EM-07012]-Biot Savart LawNode id: 5717page
The Biot Savart law for current carrying wire is explained.
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23-03-03 20:03:04 |
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[NOTES/EM-07011]-Direction convention for Ampere’s LawNode id: 5716page
Direction convention for Ampere's law is explained
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23-03-03 20:03:34 |
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[NOTES/EM-07009]-Magnetic Field of a Current Loop at Large DistancesNode id: 5714page
In this section we compute the leading term in the magnetic field of a current loop at large distances and obtain an expression for the magnetic moment of the loop.
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23-03-03 20:03:32 |
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[NOTES/EM-07008]-Magnetic Vector PotentialNode id: 5713page
The vector potential is introduced using the Maxwell's equation \(\nabla \times \vec{B}=0\) and the equation \( \nabla \times \vec{B} = \mu_0 \vec{j}\) is derived. The expression for the magnetic field is obtained as volume integral, the Biot Savart law, is derived. The expressions for the magnetic field for the surface current and the line current are given.
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23-03-03 20:03:21 |
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\(\S5.1\) Reducion of Two Body Problem to One Body Node id: 1272page |
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23-03-01 11:03:17 |
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[TESTING ] Open Systems.Node id: 5855page An open system can exchange energy and particles with the environment. The energy of the system and the number of particles does not remain constant. The composite system consisting of the system of interest and environment will be called universe. The universe is an isolated system and the results from micro-canonical ensemble are applied to obtain the conditions that the system and the environment may be in equilibrium. These conditions are temperatures, the pressures, and the chemical potentials of the environment and the system be equal. |
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23-03-01 06:03:15 |
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