Pattern formation and transition to chaos in a macroscopic dissipative syst
em is discussed. It is supposed that the system has a continuous family of
spatially uniform states, which can be transformed into each other by a cer
tain symmetry transformation. If such a system undergoes instability agains
t spatially periodic perturbations with a finite wavenumber, interplay of s
hort-wavelength modes associated with the instability and long-wavelengths
modes generated by the symmetry transformation affects the dynamics of the
system dramatically. In particular, it may result in direct transition from
a spatially uniform state to spatiotemporal chaos, analogous to second ord
er phase transition in equilibrium systems. The obtained results may be app
lied to kinetic of polymerization, to reaction-diffusion problems, to flame
propagation, to some hydrodynamic problems, etc.