Sediment-wave parameters, notably the parameter Omega = H-b/WsT (where
H-b is wave breaker height, W-s sediment fall velocity, and T wave pe
riod), have been used in the literature to identify thresholds between
various beach morphodynamic states ranging from reflective, through i
ntermediate, to dissipative. Such parameters may be useful as elementa
ry descriptors of beaches, especially in microtidal swell wave setting
s with mature sediment suites, and when used in conjunction with conce
ptual beach state models elaborated in recent years. Although the prob
lems of temporal wave height variability and large tide ranges have be
en addressed in the parametric characterization of various beach types
, these factors, together with sediment variability, may result in bea
ch morphodynamic systems that cannot be meaningfully characterized by
sediment wave parameters. Morphodynamic parameters such as the Iribarr
en Number xi(b)(xi(b)=tan(b)/(HbL0)(0.5), where tan(b) represents beac
h slope, H-b is wave breaker height, and L-o deepwater wavelength), an
d the surf-scaling parameter epsilon (epsilon = a(b)w(2)/(gtan(2)b), w
here a(b) is runup amplitude on the beach. w wave radian frequency, an
d g the gravitational constant), are based on beach slope, and avoid t
he problem of the choice of representative beach sediment parameters.
The intertidal beach slope is also a better index of characterization
of spatial and temporal changes in the reflective-to-dissipative beach
morphodynamic continuum, especially in settings with large tide range
s.