| spring | time | place | lectures | thursday 11:00 - 13:00 | MIN 0.11 |
ECTS : 7.5 credit points
Hamiltonian systems naturally occur in frictionless mechanics, but are also used to answer questions that arise in optics or when studying certain partial differential equations. After a short introduction we present the necessary theory motivated by examples like the N-body problem or the geodesic flow.
A central result is the existence of so-called action angle variables of an integrable Hamiltonian system; the action variables are conserved quantities in involution. Expressing a given system in action angle variables not only simplifies the study of the dynamical properties of the system itself, but also makes perturbations of the system accessible to both quantitative and qualitative investigations.
Ordinary Differential Equations
Manifolds (a bit: `tangent space')
Introductory Dynamical Systems
A combination of worked out home work exercises and a final exam.
Thursday 5 february. Introduction, N-body problem, tangent bundle.
Thursday 12 february. Co-tangent bundle, symmetry group, Lie bracket.
Thursday 19 february. Rigid body, exterior algebra, differential forms.
Thursday 26 february. Stokes theorem, symplectic forms and manifolds.
Thursday 5 april. Regular symmetry reduction, reduced system, momentum mapping.
Thursday 12 april. Geodesic flow, free rigid body.
Thursday 19 april. Dynamics of the free rigid body.
Thursday 2 may. Integrable systems, generalized action angle variables.
Thursday 9 may. Andoyer variables, invariant tori.
Thursday 16 may. Elliptic equilibria.
Thursday 23 may. Normal forms for equilibria, normal form algorithm.
Thursday 30 may. Normal forms for periodic orbits and invariant tori, perturbation analysis.
Thursday 7 june. Lunar problem.
Thursday 21 june. Spatial Kepler system.
Thursday 4 july. 3-body problem, normalization, symmetry reduction.
Thursday 11 july. Reduction of the discrete symmetry, singular points and their isotropy groups.
Thursday 15 july. Bifurcation analysis in one degree of freedom.
Thursday 25 july. Invariant tori in the 3-body problem.
Thursday 26 july. Open problems.