Chapter 3 : Reservoir models - KU Leuven
Chapter 3 : Reservoir models - KU Leuven
Chapter 3 : Reservoir models - KU Leuven
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1.2<br />
throughflow (m 3 /s)<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0<br />
hydrodynamic model<br />
dynamic reservoir model<br />
0 1000 2000 3000 4000 5000 6000 7000<br />
storage (m 3 )<br />
Figure 3.16 : Storage/throughflow-relationship for the sewer system<br />
of Dessel when the dynamic storage is included<br />
for a composite storm that will just lead to an overflow event.<br />
3.2.3.4 Extra storage during the overflow event<br />
During the overflow event the water will rise above the crest level. In some cases this<br />
increasing water level can lead to significant extra backwater effects, which results in<br />
increased storage in the system. This storage above the crest level can be defined as<br />
dynamic storage as is shown in figure 3.14, but it is difficult to link this dynamic<br />
storage unambiguously to the inflow as proposed in paragraph 3.2.3.2. Therefore, it<br />
is better to define an extra storage above the crest level as the storage between a<br />
horizontal plane at the crest level and a horizontal plane at the maximum water<br />
level above the crest of the overflow (figure 3.17). In that definition the dynamic<br />
storage is only the part above the horizontal plane at the maximum water level<br />
above the crest of the overflow. Again, this is an artificial division, but these three<br />
components can be recognised in the system behaviour.<br />
This extra (static) storage above the weir can be assumed to be a function of the<br />
overflow discharge. For a free overflow the relationship between discharge Q and<br />
water level h above the crest is a non-linear function [Berlamont, 1996] :<br />
(3.1)<br />
This relationship may be the case for a storage basin (figure 3.18).<br />
<strong>Chapter</strong> 3 : <strong>Reservoir</strong> <strong>models</strong> 3.17