A simple expression is introduced as an approximation for the rate of chang
e of the spectral energy density of surface gravity waves due to nonlinear
wave-wave interaction. It has the Form of a second-order nonlinear diffusio
n operator, and conserves wave energy, momentum and wave action. It is inde
pendent of the details of the dispersion relation, so it can possibly be us
ed for both deep and shallow water, although its application to shallow wat
er is not explicitly considered. The directional dependence of the Formula
is essential in permitting the wave momentum to be conserved, in addition t
o the wave energy and action. The formula may be useful in discussing the q
ualitative behavior of wave spectrum evolution without making elaborate cal
culations. It is consistent with the observed and modelled result that nonl
inear effects tend to cause the wave energy to be transferred to lower wave
frequencies. However, when applied to a JONSWAP wave spectrum it behaves r
ather diffusively, tending to directly reduce the amplitude of the spectral
peak. In the absence of other wave energy source terms, the formula Leads
to various time-independent wave spectra, whose dependence on scalar wave n
umber is linked to the angular wave energy distribution. In general the dir
ectional spreading of the spectrum tends to increase as the scalar wavenumb
er increases. The limiting directionally-isotropic spectrum has the Kitaigo
rodskii equilibrium-range behavior, where the wave energy (variance) spectr
um is proportional to the inverse Fourth power of the frequency.