manifolds serve as the phase space in classical mechanics; four dimensional pseudo-Riemannian manifolds are used to model spacetime in general relativity. What follows is a clean mathematical treatment of manifolds. |
manifolds serve as the phase space in classical mechanics; four dimensional pseudo-Riemannian manifolds are used to model spacetime in general relativity. What follows is a clean mathematical treatment of manifolds. |
Manifolds are important because they provide the proper generalization of surfaces. In classical mechanics, the state space of systems with constraints are often modelled as manifolds. The theory of general relativity postulates that all of spacetime is a 4-manifold; in fact it is a [pseudo-Riemannian manifold]? which allows one to define angles, lengths and curvature. If a manifold also carries an infinitely differentiable group structure, it is called a Lie group. These are the proper objects for describing symmetries of analytical structures. |
If a C∞ manifold also carries an infinitely often differentiable group structure, it is called a Lie group. These are the proper objects for describing symmetries of analytical structures. |
/Talk? |
/Talk? |