Part IB | Electromagnetism Theorems Based on lectures by D. Tong Notes taken by Dexter Chua Lent 2015 These notes are not endorsed by the lecturers, and I have modified them (often significantly) after lectures. They are nowhere near accurate representations of what was actually lectured, and in particular, all errors are almost surely mine. Electromagnetism and Relativity Review of Special Relativity; tensors and index notation. Lorentz force law. Electro- magnetic tensor. Lorentz transformations of electric and magnetic fields. Currents and the conservation of charge. Maxwell equations in relativistic and non-relativistic forms. [5] Electrostatics Gauss's law. Application to spherically symmetric and cylindrically symmetric charge distributions. Point, line and surface charges. Electrostatic potentials; general charge distributions, dipoles. Electrostatic energy. Conductors. [3] Magnetostatics Magnetic fields due to steady currents. Ampre's law. Simple examples. Vector potentials and the Biot-Savart law for general current distributions. Magnetic dipoles. Lorentz force on current distributions and force between current-carrying wires. Ohm's law. [3] Electrodynamics Faraday's law of induction for fixed and moving circuits. Electromagnetic energy and Poynting vector. 4-vector potential, gauge transformations. Plane electromagnetic waves in vacuum, polarization. [5] 1 Contents IB Electromagnetism (Theorems) Contents 0 Introduction 3 1 Preliminaries 4 1.1 Charge and Current . .4 1.2 Forces and Fields . .4 2 Electrostatics 5 2.1 Gauss' Law . .5 2.2 Electrostatic potential . .5 2.2.1 Point charge . .5 2.2.2 Dipole . .5 2.2.3 General charge distribution . .5 2.2.4 Field lines and equipotentials . .5 2.3 Electrostatic energy . .5 2.4 Conductors . .5 3 Magnetostatics 6 3.1 Ampere's Law . .6 3.2 Vector potential . .6 3.3 Magnetic dipoles . .6 3.4 Magnetic forces . .6 4 Electrodynamics 7 4.1 Induction . .7 4.2 Magnetostatic energy . .7 4.3 Resistance . .7 4.4 Displacement currents . .7 4.5 Electromagnetic waves . .7 4.6 Poynting vector . .7 5 Electromagnetism and relativity 8 5.1 A review of special relativity . .8 5.1.1 A geometric interlude on (co)vectors . .8 5.1.2 Transformation rules . .8 5.1.3 Vectors and covectors in SR . .8 5.2 Conserved currents . .8 5.3 Gauge potentials and electromagnetic fields . .8 5.4 Maxwell Equations . .8 5.5 The Lorentz force law . .8 2 0 Introduction IB Electromagnetism (Theorems) 0 Introduction 3 1 Preliminaries IB Electromagnetism (Theorems) 1 Preliminaries 1.1 Charge and Current Law (Continuity equation). @ρ + r · J = 0: @t 1.2 Forces and Fields Law (Lorentz force law). F = q(E + v × B) Law (Maxwell's Equations). ρ r · E = "0 r · B = 0 @B r × E + = 0 @t @E r × B − µ " = µ J; 0 0 @t 0 where we have two constants of nature: −12 −3 −1 2 2 { "0 = 8:85 × 10 m kg s C is the electric constant; −6 −2 { µ0 = 4π × 10 m kg C is the magnetic constant. Some prefer to call these constants the \permittivity of free space" and \per- meability of free space" instead. But why bother with these complicated and easily-confused names when we can just call them \electric constant" and \mag- netic constant"? 4 2 Electrostatics IB Electromagnetism (Theorems) 2 Electrostatics 2.1 Gauss' Law Law (Gauss' law). Z Q E · dS = ; S "0 where Q is the total charge inside V . 2.2 Electrostatic potential 2.2.1 Point charge 2.2.2 Dipole 2.2.3 General charge distribution 2.2.4 Field lines and equipotentials 2.3 Electrostatic energy Proposition. " Z U = 0 E · E d3r: 2 2.4 Conductors 5 3 Magnetostatics IB Electromagnetism (Theorems) 3 Magnetostatics 3.1 Ampere's Law Law (Ampere's law). I B · dr = µ0I; C where I is the current through the surface. 3.2 Vector potential Proposition. We can always pick χ such that r · A0 = 0. Law (Biot-Savart law). The magnetic field is µ Z r − r0 B(r) = r × A = 0 J(r0) × dV 0: 4π jr − r0j3 If the current is localized on a curve, this becomes I 0 µ0I 0 r − r B = dr × 0 3 ; 4π C jr − r j since J(r0) is non-zero only on the curve. 3.3 Magnetic dipoles 3.4 Magnetic forces 6 4 Electrodynamics IB Electromagnetism (Theorems) 4 Electrodynamics 4.1 Induction Law (Faraday's law of induction). dΦ E = − : dt 4.2 Magnetostatic energy Proposition. The energy stored in a magnetic field is 1 Z U = B · B dV: 2µ0 4.3 Resistance Law (Ohm's law). E = IR; Law (Ohm's law). J = σE: 4.4 Displacement currents 4.5 Electromagnetic waves 4.6 Poynting vector Theorem (Poynting theorem). dU Z 1 Z + J · E dV = − (E × B) · dS : dt V µ0 S | {z } | {z } Total change of energy in V (fields + particles) Energy that escapes through the surface S 7 5 Electromagnetism and relativity IB Electromagnetism (Theorems) 5 Electromagnetism and relativity 5.1 A review of special relativity 5.1.1 A geometric interlude on (co)vectors 5.1.2 Transformation rules 5.1.3 Vectors and covectors in SR 5.2 Conserved currents 5.3 Gauge potentials and electromagnetic fields 5.4 Maxwell Equations 5.5 The Lorentz force law 8.