Drakkith said:
When we talk about space-time curvature or the curvature of space, how many different "types" of curvature are there according to GR?
For example, the rounded surface of a cylinder is curved in only 1 dimension, while the other is flat. For a sphere, both dimensions of the surface are curved. Since space-time is 4 dimensional, I assume the curvature extends to all 4 dimensions?
Also, I've read about intrinsic and extrinsic curvature. Which one does GR predominately deal with?
Your example of a cylinder having two curvatures is the extrinsic curvature. GR is concerned mainly with the intrinsic curvature of the cylinder. For any two dimensional surface, there are two principal extrinsic curvatures. The intrinsic curvature is equal to the product of the two principal extrinsic curvatures, which is a single number. This number is 0 in the case of the cylinder because the Gaussian curvature is proportional to the product of the principal curvatures, and one of the principal curvatures is zero for the cylinder.
See for instance
http://en.wikipedia.org/w/index.php?title=Gaussian_curvature&oldid=598900344
In GR, the curvature is generally taken to be described completely by the Riemann curvature tensor. This is a tensor with 4 indices. In two dimensions, each index can take one of two values, in four dimensions, each index can take one of 4 values.
Thus in 2 dimensions, the Riemann has 2 x 2 x 2 x 2 = 8 components. However, there is a great deal of symmetry in the Riemann (formally described by the Bianchi identities), and there is only one degree of freedom in the tensor.
The only non-zero components in the 2d case would be ##R_{0101} = R_{1010} = -R_{0110} = -R_{1001}, ## so there is only one degree of freedom in the GR case, thus specifying the Gaussian curvature, a single number, specifies the whole tensor.
In four dimensions, the Riemann has 4 x 4 x 4 x 4 = 256 components, but there are 20 degrees of freedom
http://mathworld.wolfram.com/RiemannTensor.html. So one needs to specify 20 unique and independent numbers at a point in a general space-time to fully describe its curvature.
Using the Bel decomposition,
http://en.wikipedia.org/w/index.php?title=Bel_decomposition&oldid=597299599, given a space-time split, we can refine the 20 components of the Riemann into smaller tensors which provide more physical insight. There are:
6 components for the electrogravitic tensor, a 3 x 3 tensor which is basically equivalent to the Newtonian idea of the tidal force tensor. It's typically given the symbol E to represent it's similarity to the electric field in electromagnetism. The six degrees of freedom represent three degrees of freedom for the rotation of the tensor, and 3 values which represent the magnitude of the tidal force along each principal axis of the tensor.
8 components for the magnetetogravitc tensor, which describes frame dragging effects. If you have a static spacetime, this tensor is zero. This tensor is typically given the symbol B to represent its similarity to the magnetic field in electromagnetism.
6 components for the topogravitic tensor, which describes the purely spatial part of the space-time curature. As I recall the topogravitic tensor is equal to the electrogravitic tensor if you have a vacuum space-time. Its usually given the symbol L, and it doesn't have any electromagnetic equivalent as electromagnetism doesn't warp space.
Thus for a typical static Schwarzschild metric, B=0 and L=E, so all you need to specify is E, and that can be specified by the orientation of the three principal axes of the tensor (which takes three numbers to specify) and the magnitude of the tidal forces along said axes (which also takes three numbers to specify).
A completely general space-time would need 20 numbers to specify, however.