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The evolution of Jumpinpin Inlet - OzCoasts

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<strong>The</strong> <strong>evolution</strong> <strong>of</strong> <strong>Jumpinpin</strong> <strong>Inlet</strong><br />

4.1.6 <strong>Inlet</strong> stability and closure<br />

Some inlets are comparatively permanent features being maintained by tidal<br />

exchange supplemented by storm generated currents, whereas other inlets tend to<br />

close. <strong>The</strong> tendency toward closure is related to the ratio between littoral drift and<br />

tidal flow bypassing <strong>of</strong> sand past the inlet (Stanley & Swift, 1974). When, as the result<br />

<strong>of</strong> a storm the cross-sectional area <strong>of</strong> an inlet is reduced below a certain value, the<br />

tidal currents could become too small to flush the sediment coming into the inlet by<br />

the longshore current. Longshore processes will dominate over tidal flow and the inlet<br />

will close. <strong>The</strong> importance <strong>of</strong> inlet width has been explored by Van De Kreeke (1985;<br />

1990a,b) and is described in terms <strong>of</strong> stability analysis and closure curves.<br />

Stability <strong>of</strong> single inlets deals with the equilibrium between gorge cross-sectional area<br />

and inlet hydrodynamics. From Van De Kreeke (1990a), the parameters <strong>of</strong> stability<br />

are actual tidal maximum <strong>of</strong> the bottom shear stress and the equilibrium shear stress.<br />

<strong>The</strong> equilibrium shear stress is defined as the bottom stress induced by tidal currents<br />

that is required to flush sediments carried into the inlet by longshore currents.<br />

When actual shear stress equals the equilibrium shear stress, the inlet is in<br />

equilibrium with the hydraulic environment. If the actual shear stress becomes larger,<br />

the inlet goes into scouring mode. If equilibrium shear stress is larger the inlet is in<br />

shoaling mode. <strong>The</strong> equilibrium is considered stable if, after changes such as storms,<br />

the inlet cross-sectional area unconditionally returns to its equilibrium value.<br />

For two-inlet bay systems Van De Kreeke (1990a) provides a possible configuration<br />

for equilibrium flow curves (see Figure 4.2). <strong>The</strong> open and closed circles imply four<br />

sets <strong>of</strong> values for which both inlets have cross-sectional areas that are in equilibrium<br />

with the hydraulic environment. Results <strong>of</strong> a stability analysis on a two-inlet bay<br />

system conducted by Van De Kreeke (1985) showed that at best two sets <strong>of</strong><br />

equilibrium flow area can exist. Based on these results, a set <strong>of</strong> stable cross-sectional<br />

areas cannot exist and ultimately one or both the inlets will close.<br />

14

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