Channel infilling under waves parallel to steady currents: Difference between revisions

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== '''Setup''' ==
== '''Setup''' ==
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A laboratory experiment on the evolution of channel morphology under cross-channel flow with waves parallel to the channel axis was carried out in a wave-current flume by van Rijn (1986). The channel was approximately 4 m wide and 0.22 m deep, and had 1:10 side slopes (see Figure 1). The current speed at the inflow boundary was 0.245 m/s. Incident irregular waves (JONSWAP form) were parallel to the channel axis (90º with respect to the flow) and had a significant wave height of 0.105 m and peak wave period of 2.2 s. The initial bathymetric profile is shown in Figure 1. Manning’s coefficient n is calibrated as approximately 0.02 with the measured velocity profile. The bed slope coefficient is set to 2.0. The sediment median diameter is 0.1 mm. The transport grain size is set to, so that no hiding and exposure is considered. The sediment concentration at the inflow boundary is specified as the equilibrium concentration based on the Lund-CIRP transport equations. The total-load adaptation length calibrated as 0.75 m by comparing the calculated and measured morphology changes.


A laboratory experiment on the evolution of channel morphology under cross-channel flow with waves parallel to the channel axis was carried out in a wave-current flume by  van Rijn (1986). The channel was approximately 4 m wide and 0.22 m deep, and had 1:10 side slopes (see Figure 1). The current speed at the inflow boundary was 0.245 m/s. Incident irregular waves (JONSWAP form) were parallel to the channel axis (90º with respect to the flow) and had a significant wave height of 0.105 m and peak wave period of 2.2 s. The initial bathymetric profile is shown in Figure 1. Manning’s coefficient n is calibrated as approximately 0.02 with the measured velocity profile. The bed slope coefficient is set to 2.0. The sediment median diameter                                    is 0.1 mm. The transport grain size is set to      , so that no hiding and exposure is considered. The sediment concentration at the inflow boundary is specified as the equilibrium concentration based on the Lund-CIRP transport equations. The total-load adaptation length calibrated as 0.75 m by comparing the calculated and measured morphology changes.
[[Image:vanRijn_1986_Exp_Setup.png|thumb|left|600px| Figure 1. Experimental setup. (from van Rijn 1986)]]
[[Image:Thuc_Exp_Setup.png|thumb|left|400px| Figure 1. Experimental setup for Thuc (1991) experiment. ]]
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== '''Results''' ==
== '''Results''' ==
  Normal  0      false  false  false                    MicrosoftInternetExplorer4      The computed morphology changes agree well with the measured, as shown in Figure 1. The root-mean-squared error (RMSE) between measured and computed water depths is 0.01 m, which is less than 5% of the upstream flow depth. The relative-mean-absolute error (RMAE) is 2%. The model reproduces well the general trend of the morphology change including the upstream bank migration and downstream bank erosion. The small oscillations (on the order of 1 m in length) in the measured bathymetry are more likely to be large bed forms that cannot be simulated in the present model.
Figure 1. The root-mean-squared error (RMSE) between measured and computed water depths is 0.01 m, which is less than 5% of the upstream flow depth. The relative-mean-absolute error (RMAE) is 2%. The model reproduces well the general trend of the morphology change including the upstream bank migration and downstream bank erosion. The small oscillations (on the order of 1 m in length) in the measured bathymetry are more likely to be large bed forms that cannot be simulated in the present model.


[[Image:Thuc_Depth4hrs.png|thumb|left|600px| Figure 2. Computed bed elevations and current velocities at t=4 hrs.]]
[[Image:vanRijn_1986_Bed_Elevation.PNG|thumb|left|600px| Figure 2. Computed bed elevations and current velocities at t=10 hrs.]]
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[[Image:Thuc_Bed_Elevation.png|thumb|left|600px| Figure 3. Computed and measured bed elevations at t=1,4 hrs.]]
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== '''References''' ==
== '''References''' ==
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van Rijn, L. C. (1986) “Sedimentation of dredged channels by currents and waves”, Journal of Waterway, Port, Coastal and Ocean Engineering, 112(5), 541-559.


van Rijn, L. C. (1986) “Sedimentation of dredged channels by currents and waves”, Journal of Waterway, Port, Coastal and Ocean Engineering, 112(5), 541-559.
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[[Test_Cases]]
[[Test_Cases]]

Latest revision as of 19:38, 26 August 2010

Setup

A laboratory experiment on the evolution of channel morphology under cross-channel flow with waves parallel to the channel axis was carried out in a wave-current flume by van Rijn (1986). The channel was approximately 4 m wide and 0.22 m deep, and had 1:10 side slopes (see Figure 1). The current speed at the inflow boundary was 0.245 m/s. Incident irregular waves (JONSWAP form) were parallel to the channel axis (90º with respect to the flow) and had a significant wave height of 0.105 m and peak wave period of 2.2 s. The initial bathymetric profile is shown in Figure 1. Manning’s coefficient n is calibrated as approximately 0.02 with the measured velocity profile. The bed slope coefficient is set to 2.0. The sediment median diameter is 0.1 mm. The transport grain size is set to, so that no hiding and exposure is considered. The sediment concentration at the inflow boundary is specified as the equilibrium concentration based on the Lund-CIRP transport equations. The total-load adaptation length calibrated as 0.75 m by comparing the calculated and measured morphology changes.

Figure 1. Experimental setup. (from van Rijn 1986)


Results

Figure 1. The root-mean-squared error (RMSE) between measured and computed water depths is 0.01 m, which is less than 5% of the upstream flow depth. The relative-mean-absolute error (RMAE) is 2%. The model reproduces well the general trend of the morphology change including the upstream bank migration and downstream bank erosion. The small oscillations (on the order of 1 m in length) in the measured bathymetry are more likely to be large bed forms that cannot be simulated in the present model.

Figure 2. Computed bed elevations and current velocities at t=10 hrs.


References

van Rijn, L. C. (1986) “Sedimentation of dredged channels by currents and waves”, Journal of Waterway, Port, Coastal and Ocean Engineering, 112(5), 541-559.


Test_Cases