The large-scale dynamics of the Kolmogorov flow near its threshold of
instability is studied in the presence of the beta-effect (Rossby wave
s). The governing equation, obtained by a multiscale technique, fails
the Painleve test of integrability when beta not equal 0. This ''beta-
Cahn-Hilliard'' equation with cubic nonlinearity is simulated numerica
lly in various regimes, The dispersive action of the waves modifies th
e inverse cascade associated with the Kolmogorov flow (She, Phys, Lett
, A 124 (1987) 161). For small values of beta the inverse cascade is i
nterrupted at a wavenumber which increases with beta, For large values
of beta only resonant wave interactions (RWI) survive, An original ap
proach to RWI is developed, based on a reduction to normal form, of th
e sort used in celestial mechanics. Otherwise, wavenumber discreteness
effects, which are dramatic in the present case, are not captured. (T
he method is extendable to arbitrary RWI problems.) The only four-wave
resonances present involve two pairs of opposite wavenumbers. This al
lows leading-order decoupling of moduli and phases of the various Four
ier modes, so that an exact kinetic equation is obtained for the energ
ies of the modes. It has a Lyapunov (gradient Bow) functional formulat
ion and multiple attracting steady-states, each with a single mode exc
ited.