The Hamiltonian description of hydrodynamic type systems for applicati
on to plasmas, hydrodynamics, and magnetohydrodynamics is reviewed wit
h emphasis on the problem of introducing canonical variables. The rela
tion to other Hamiltonian approaches, in particular natural-variable P
oisson's brackets, is pointed out. It is shown that the degeneracy of
noncanonical Poisson's brackets relates to the special type of symmetr
y, the relabeling transformations of fluid-particle Lagrangian markers
, from which all known vorticity conservation theorems, such as Ertel'
s, Cauchy's, Kelvin's, as well as the vorticity frozenness and the top
ological Hopf invariant, derive. The application of canonical variable
s to collisionless plasma kinetics is described. The Hamiltonian struc
ture of Benney's equations and of the Rossby wave equation is discusse
d. Davey-Stuartson's equation is given the Hamiltonian form. A general
method for treating weakly nonlinear waves is presented based on clas
sical perturbation theory and the Hamiltonian reduction technique.