13- Electro-Magnetism
This lecture introduces the static electric and magnetic fields, the associated Lagrangian and the Lorentz force. The vector potential, it’s gauge field and gauge invariance are also introduced.
Topics
Magnetic and electric fields
The concept of field
The “del” or “nabla” symbol
Vector calculus: Gradient, Divergence and Curl
The Levi-Civita symbol
Algebra: div curl and curl grad vanish
The vector potential and why it’s needed
Gauge field: “Gauge” is a misnomer
Lorentz force. Lorentz force compared with the Coriolis force
Lagrangian for charged particles in a electro-static and magneto-static fields
Gauge invariance of the equations of motions associated to the electro-magneto-static Lagrangian
References
This final lecture is a general review of all the concepts learned so far applied to a particle in electric and magnetic static fields
Topics
Review of the vector potential, concept of gauge and gauge invariance
Lorentz force law
Example of different vector potentials for a constant magnetic field and the gauge transformation that relate them
Importance of gauge invariance and choice of gauge
Lagrangian of a particle in a static magnetic field. Review of the related action gauge invariance
Distinction between mechanical and canonical momentum: only the canonical momentum is related to symmetries and invariance
Derivation of the Euler-Lagrange equation of motion from the magneto-static Lagrangian and rediscovery of the Lorentz force
Justification of the vector potential as an essential tool for the least action principle
Derivation of the magneto-static Hamiltonian
Smart choice of gauge and derivation of the Lorentz force from symmetry arguments only, “cyclic coordinates”
Circular motion of a charged particle in a static magnetic field
Monopoles discussion as part of the questions session
Brief Quaternions discussion as part of the questions session
References