Fundamental physics, year 1
(Teknisk fysik, årskurs 4)
Advanced classical physics — Lecture notes
by Christian von Schultz
Lecturer: Per Salomonson
The course home page can be found at
http://fy.chalmers.se/~tfeps/acp.dir/.
- Tuesday 2008-09-02
- Repetition of the Newtonian mechanics. Position, force,
momentum. Particle systems. The weak form of the third law and the
strong form of the third law. Conservation of momentum and angular
momentum. Energy of a particle. Three equivalent criteria for
conservative forces. Potential for particle systems. Centre of mass
coordinates. The angular momentum of a particle system equals the
angular momentum of the mass centre, plus the angular momentum due
to motion relative to the centre of mass. The kinetic energy of a
particle system equals the kinetic energy of the mass centre, plus
the kinetic energy due to motion relative to the centre of
mass. Rigid bodies, and the inertia tensor Ia
b.
- Friday 2008-09-05
- Generalised coordinates, generalised force, generalised
momentum. Lagrange's equations without a potential. Lagrange's
equation for a conservative force, with a potential. Examples:
planetary motion in polar coordinates (r, θ); plane
pendulum. Holonomic constraints. Constraint forces and d'Alembert's
principle.
- Monday 2008-09-08
- Holonomic constraints. Constraint forces and d'Alembert's
principle. Elimination of the constraints from the set of
equations (example: spherical pendulum). Lagrange multiplier
method. Lagrangian for Lorentz force.
- Tuesday 2008-09-09
- No lecture notes today, sorry.
- Friday 2008-09-12
- Variational calculus. Soap bubble surface (minimisation of
area). The analogy between variational calculus and ordinary
differential calculus. Hamilton's principle. The action. Variational
calculus with Lagrange parameters. Boundary terms and boundary
conditions.
- Monday 2008-09-15
- For each conserved quantity there corresponds a continuous
symmetry. The summation convention. Energy conservation — time
translation. Momentum conservation — spatial
translation. Conservation of angular momentum —
rotation. Cyclic variables (ignorable variables). Elimination of
cyclic coordinates from the Lagrangian. Jacobi's principle.
- Tuesday 2008-09-16
- Hamilton's equations. Going from a Lagrangian to the
corresponding Hamiltonian. The action in the Hamiltonian
formulation. Cyclic variables in the Hamiltonian
formulation. Configuration space versus phase space. Flow in phase
space. Liouville's theorem: “The phase fluid is incompressible.”
Extended phase space.
- Friday 2008-09-19
- Canonical transformations. Point transformations. The generating
function of a canonical transformation. Legendre
transformation. Infinitesimal canonical transformations. Dynamical
variables — infinitesimal canonical transformations. Poisson
brackets. The Hamiltonian is the generator of infinitesimal time
translation. Momentum as a generator of translation. Angular
momentum as a generator of rotations. Symmetry transformation if the
Hamiltonian is invariant. The Jacobi identity. The connection to
quantum mechanics.
- Monday 2008-09-22
- Relativistic mechanics. Lorentz transformation. The
metric η. Making theory relativistic = choosing equations
covariant. The action from scalar pieces. The action for a free
particle. The action for electromagnetism. Examples of a scalar
field, a vector field and a tensor field. Curved spacetime. The
Hamiltonian formulation in relativistic mechanics. Gauge
transformations, gauge symmetry, gauge invariance, gauge
theories.
- Tuesday 2008-09-23
- Exercise class.
- Friday 2008-09-26
- Mechanics of fields. The correspondence between particle theory
and field theory. Equations of motion. Boundary conditions. Scalar
field in relativistic theory [the Klein-Gordon
Lagrangian]. Interpretation as a quantum field theory. The
Hamiltonian formulation of field mechanics. The Poisson
bracket. Current conservation and conservation of charge. Space
translation and energy-momentum conservation.
- Monday 2008-09-29
- Integrable systems. Solving a system of linear differential
equations with constant coefficients. System of free scalar fields.
Lagrangian with O(n) symmetry. The action for the
electromagnetic field.
- Tuesday 2008-09-30
- The Hamiltonian for the electromagnetic field. Gauge
transformation of the electromagnetic
potential Aμ. Field degrees of freedom. Second
class constraints, first class constraints.
- Friday 2008-10-03
- The procedure of gauging. Gauging the O(n) symmetry
(making the O(n) symmetry local). Covariant derivative. Gauge
field potential. Gauge field strength. An O(n) Yang-Mills
theory. The mathematical definition of a group.
- Monday 2008-10-06
- Symmetry groups. U(n) and O(n). SU(n) and
SO(n). U(1) = SO(2). How the Lagrangian of the standard model
is built. Goldstone's theorem and the Higgs mechanism.
- Tuesday 2008-10-07
- Solitions. O(1) model with spontaneous symmetry breaking
[Wikipedia calls
this a φ4
theory].
- Friday 2008-10-10
- No lecture notes today, sorry. I was holding a lecture myself,
teaching the first years
about ISO 31 and
related matters.
- Monday 2008-10-13
- Tensors (continued). Addition. Outer
multiplication. Contraction. Symmetrisation. Quotient rule
(important for showing that a given object is a tensor). The
Kronecker symbol — an invariant tensor. Metric
manifold. Differentiation of a (p, q) field
object. Tensor densities. Group theory: Subgroup. Invariant
subgroup. Conjugacy. Equivalence relations: transitivity, symmetry,
reflexivity. Equivalence classes (conjugacy classes). Albelian
groups. Lie groups.
- Friday 2008-10-17
- Lie group. Lie algebra. Lie bracket. Adjoint
representation. Ideal. Simple Lie algebra. Albelian
ideal. Semisimple Lie algebra.
A word of thanks goes to Christer Samuelsson, who reported
in some typos.
Christian von Schultz <forelant@vonschultz.se>