Density fluctuations of fluids with negative pressure exhibit decreasing ti
me behaviour in the long-wavelength limit, but are strongly unstable in the
small-wavelength limit when a hydrodynamical approach is used. On the othe
r hand, the corresponding gravitational waves are well behaved. We verify t
hat the instabilities present in density fluctuations are due essentially t
o the hydrodynamical representation: if we turn to a field representation t
hat leads to the same background behaviour, the instabilities are no longer
present. In the long-wavelength limit, both approaches give the same resul
ts. We also show that this inequivalence between background and perturbativ
e level is a feature of a negative pressure fluid. When the fluid has posit
ive pressure, the hydrodynamical representation leads to the same behaviour
as the field representation both at the background and perturbative levels
.