β Scribed by George E. Uhlenbeck; Erich Beth
No coin nor oath required. For personal study only.
π SIMILAR VOLUMES
The considerations on the second virial coefficient B (T) given in the first part of this paper (see Ref. 1) have been extended by taking into account the influence of Bose or Fermi statistics (w 2) and of discrete quantum states (existence of polarization molecules, w 3). The expression (I, Eq. 21)
From the assumption that the collective Hamiltonian be invariant under the orthogonal group O(A -1, iR) it is concluded that classical collective dynamics can be formulated on a symplectic manifold. This manifold is shown to be a coset space of the symplectic group Y/2(6, [R) of dimension 12, 16 or
The Onsager linear relations between macroscopic ows and thermodynamics forces are derived from the point of view of large deviation theory. For a given set of macroscopic variables, we consider the short-time evolution of near-equilibrium uctuations, represented as the limit of ΓΏnite-size condition