For small Hamiltonian perturbation of a Hamiltonian system of arbitrary num
ber of degrees of freedom with a normally non-degenerate submanifold of per
iodic orbits we construct a nearby submanifold and an `effective Hamiltonia
n' on it such that the difference between the two Hamiltonian vector fields
is small. The effective Hamiltonian is independent of one coordinate, the
`overall phase', and hence the corresponding action is preserved. Unlike st
andard averaging approaches, critical points of our effective Hamiltonian s
ubject to given action correspond to exact periodic solutions. We prove the
re has to be at least a certain number of these critical points given by gl
obal topological principles. The linearisation of the effective Hamiltonian
about critical points is proved to give the linearised dynamics for the fu
ll system to leading order in the perturbation. Hence in the case of distin
ct eigenvalues which move at non-zero speed with epsilon, the linear stabil
ity type of the periodic orbit can be read off from the effective Hamiltoni
an. Our principal application is to networks of oscillators or rotors where
many such submanifolds of periodic orbits occur at the uncoupled limit - s
imply excite a number N greater than or equal to 2 of the units in rational
frequency ratio and put the others on equilibria, subject to a non-resonan
ce condition. The resulting exact periodic solutions for weak coupling are
known as multibreathers. We call the approximate solutions given by the eff
ective Hamiltonian dynamics, 'generalised multibreathers'. They correspond
to solutions which look periodic on a short time scale but the relative pha
ses of the excited units may evolve slowly. Extensions are sketched to trav
elling breathers and energy exchange between degrees of freedom.