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(a)
2
1
0
0
2
4
6
8
10
12
14
(b)
1
0
1
−
0
4
6
8
2
10
12
14
Time (days)
Figure 9.7
(a) Bottom-surface density difference over a neap-spring transition in Liverpool
Bay. (b) Depth-averaged tidal currents in Liverpool Bay. Data were collected by the vertical
array of current meters shown in Fig. 1.7. The position of the mooring is marked in
Fig. 9.6
.
Adapted from Sharples and Simpson,
1993
, with permission from the Estuarine Research
Federation.
mixing fronts, which indicates a balance between heating and stirring influences, adjusts
over the spring-neap cycle as the tidal currents change. The condition for maintaining
freshwater-driven stratification (
Equation 9.22
) allows for a similar adjustment of the
balance as the springs-neaps tidal cycle imposes a regular cycle of change in the stirring.
Figure 9.7
shows how this modulation of stirring is frequently observed in a fortnightly
cycle of stratification and mixing. During the period around neap tides (day 1-2),
reduced stirring has allowed the development of pronounced stratification with sur-
face-bottom density difference
1-2kgm
3
. As the tides increase towards
spring tides (day 9-10), greater stirring results in a complete breakdown of stratification
D
D
r
0kgm
3
. This pattern can be complicated bymonthlymodulation of the tides due
to the N
2
tidal constituent which results in one springs-neaps cycle in each month being
stirring decreases is rapid, resulting in the propagation of a front westward through the
bay to about 4
W until a geostrophic balance is established.
r
Box 9.1 Density currents versus stirring in a tank experiment
The interaction between horizontal buoyancy spreading and vertical mixing has been
on a modified version of the classical lock-exchange experiment. In the original
experiment, a rectangular tank is equipped with a central 'lock gate' which separates
two miscible fluids of different density (usually brine and freshwater with different
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