in which Hsis offshore significant wave height, Tis the mean wave period,
is the approach angle, dis the depth at the toe of the wall, Ris freeboard
of the wall from SWL and sis the beach slope.
Overtopping of non-porous vertical walls due to regular waves may
be determined from the model tests reported in Shore Protection Manual,
(US Army, 1984) (see also Thomas and Hall, 1992).
For simple slopes, the test results of Owen (1980) with random waves
are applied for the prediction of discharge due to overtopping. The results
are expressed in terms of a relationship between two non-dimensional
quantitiesQ* and R*.
QAexp (^) (15.31)
in which Q and R*. Q is the mean discharge in
m^3 s^1 per m run of the wall overtopping the crest of the sea wall, Tis the
mean wave period, Ris the freeboard of the wall from the still water level
to the crest and ris the roughness factor as given in Table 15.1. The results
are valid for the range of slopes from 1:1 to 1:4 and wave steepness from
0.035 to 0.055.
Typical values of AandBare given in Table 15.2
For values of the coefficients AandBof equation (15.31) to estimate
the mean overtopping discharge to include bermed sea wall and the effects
of angle of wave attack, refer to Owen (1980).
Tolerable overtopping discharges
For vehicles Besley et al.(1998) suggest mean values of overtopping dis-
charge0.001 l/s/m as safe at all speeds, between 0.001 and 0.02 l/s/m as
unsafe at high speed and 0.021 l/s/m as unsafe at any speed. For pedestri-
R
T g H (^) s
Q
TgHs
BR*
r
Table 15.2 Values of coefficients AandBfor simple sea walls
Seawall slope A B
1:1 7.9 103 20.12
1:1.5 1.02 102 20.12
1:2 1.25 102 22.06
1:2.5 1.45 102 26.1
1:3 1.63 102 31.9
1:3.5 1.78 102 38.9
1:4 1.92 102 46.96
1:4.5 2.15 102 55.7
1:5 2.50 102 65.2