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Fig. 11.1 Types of tidal
channels: ( a ) a dendritic or
fractal network in the Dutch
Wadden Sea, stream orders
are numbered (Cleveringa
and Oost 1999 ) ; ( b ) braided/
interconnected channeling in
the Western Scheldt Estuary,
Netherlands; and ( c ) a sketch
of ebb and fl ood channels in a
braided network (van Veen
( 1950 ) ; adapted from Hibma
et al. ( 2004a ) )
gradients; and (4) width to depth ratios greater than 5
(Steers 1969 ; D'Alpaos et al. 2005 ) . In general, the
channels tend to narrow inland; seen from above,
coastal waterways often appear funnel-shaped. This
relates to a reduction in tidal prism upstream (the rate
of this reduction is sometimes explained by tidal reso-
nance; for further discussion see Wright et al. ( 1973 )
and Van der Wegen et al. ( 2008 ) ). This strong spatial
gradient of channel width, which occurs in shallow
tidal channels of all orders, is arguably one of the key
characteristics that distinguishes tidal from fl uvial sys-
tems, along with the notably higher width of tidal
channels with respect to the inter-channel region that
they 'drain' (Fagherazzi et al. 1999 ) . This difference in
channel width to drainage area means that tidal chan-
nels would seem more closely spaced when compared
to rivers of a similar width.
Tidal channels are ubiquitous, occurring across
macro-, meso- and microtidal environments. They
often form dendritic networks (i.e. branching and blind
ended; Ashley and Zeff 1988 ) , commonly of low-
order. The smallest creeks at the edge of a network are
the lowest order, these meet to form a channel of the
next order (Fig. 11.1a , Horton 1945 ) . Tidal channel
networks have been described by some studies as
fractal (Perillo et al. 1996 ; Fagherazzi et al. 1999 ;
Schwimmer 2008 ) . Pestrong ( 1965 ) observed that the
dendritic tidal networks in San Francisco Bay resem-
bled fl uvial systems. However, despite their apparent
similarity, he determined that the tidal channels did not
follow Hortonian laws of drainage networks. Tidal net-
works, unlike their fl uvial counterparts, are not true
scaling structures (Fagherazzi et al. 1999 ) . Marani
et al. ( 2002 ) concluded that “in any real case of fl uvial
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