Model of frictional two-layer exchange flow
An unsteady model is developed for two-layer exchange through a channel with friction on the bottom, sidewalls, surface and interface. Steady or time-varying barotropic forcing can be specified. The unsteady model is first used to solve for the steady solution with zero barotropic forcing startin...
Main Author: | |
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Format: | Others |
Language: | English |
Published: |
2009
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Online Access: | http://hdl.handle.net/2429/11479 |
Summary: | An unsteady model is developed for two-layer exchange through a channel with friction
on the bottom, sidewalls, surface and interface. Steady or time-varying barotropic forcing
can be specified. The unsteady model is first used to solve for the steady solution with
zero barotropic forcing starting from initial conditions of the lock exchange problem. The
effects of friction on steady exchange are investigated for four channel configurations: a
contraction with constant depth and with an offset sill, and a constant-width channel with
constant depth and with a sill near one end. Exchange flow decreases substantially with
increasing friction. The interface position and locations of internal hydraulic control are
affected by varying friction. Solutions are asymmetrical when surface friction is absent.
Internal hydraulic jumps form when friction is increased. Flow becomes hydraulically
uncontrolled for high friction in all channel geometries considered. The model predictions
are compared to experiments in a constant-width channel with constant depth and with
a sill.
The model is also applied to the Burlington Ship Canal which connects Hamilton
Harbour to Lake Ontario. The exchange in the Burlington Ship Canal is modeled with
zero and net steady barotropic components. Field observations from boat-mounted instruments
show barotropic components and unsteadiness in flows. The magnitude of the
observed barotropic variations is not great enough to influence exchange so that friction
is the dominant factor governing exchange in the Burlington Ship Canal.
The unsteady model is finally used with a periodic barotropic forcing in the contraction
geometry. Exchange increases with forcing period and magnitude for the frictionless
case. The model results are inconclusive for the effect of increasing friction with the
periodic barotropic forcing. The numerical methods of the model do not' allow it to be
generally applied to other channel geometries with time-varying barotropic forcing. === Applied Science, Faculty of === Civil Engineering, Department of === Graduate |
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