In the present work, we study the dynamical properties of fluids confi
ned at molecular scales. First, we show that, for a fluid confined bet
ween two parallel solid walls, the phenomenological hydrodynamic descr
iption of bulk fluids holds down to nanoscopic scales, once appropriat
e boundary conditions at the solid walls are applied. Then, we investi
gate the influence of confinement on the self-diffusion coefficient (i
n the direction parallel to the walls) in a fluid slab. We have comput
ed the effect of confinement on the mode-coupling contribution to the
diffusion coefficient. These finite-size corrections are shown to redu
ce the diffusion constant by an amount -(sigma/h) log(h/sigma), where
h is the thickness of the fluid slab and a the atomic size. This behav
iour can be interpreted in terms of the suppression of long-wavelength
modes in the backflow effect, due to confinement.