I think matematikuvol refers to precisely the degrees of freedom you have specified, i.e., the microscopic degrees of freedom. In the most simple case you may consider the classical model of a monatomic gas, where a gas is described by a system of very many (noninteracting or at a higher degree of sophtification weakly interacting) point particles.
To specify the micro state of this system uniquely you need to give a point in a 6N-dimensional space. The most elegant way is to use the Hamiltonian formulation of mechanics, and then these 6N degrees of freedom are the 3N components of positions and 3N components of momenta for the particles.
Of course, nobody can ever write down all these phase-space coordinates, let alone calculate their time evolution since [itex]N = \mathcal{O}(10^{24})[/itex]. Thus one uses averaged "macroscopic" variables like various densities (particle number, energy density etc.) to describe the most important observables of the system as a whole. This very roughly is the fundamental idea behind statistical physics.