CMS-Flow:Transport Formula: Difference between revisions
(Created page with "__NOTOC__ ==Lund-CIRP== Camenen and Larson (2005, 2007, and 2008) developed a general sediment transport formula for bed and suspended load under combined waves and currents. ...") |
(Created page with __NOTOC__ ==Lund-CIRP== Camenen and Larson (2005, 2007, and 2008) developed a general sediment transport formula for bed and suspended load under combined waves and currents. ...) |
||
Line 5: | Line 5: | ||
=== Bed load=== | === Bed load=== | ||
The current-related bed load transport with wave stirring is given by | The current-related bed load transport with wave stirring is given by | ||
{{Equation| | {{Equation|math \frac{q_{b}}{\sqrt{(s-1)gd^3}} = a_c \sqrt{\theta_c} \theta_{cw}\exp{ \biggl ( -b_c \frac{\theta_{cr}}{\theta_{cw}}} \biggr ) /math|2=1}} | ||
=== Suspended load === | === Suspended load === | ||
The current-related suspended load transport with wave stirring is given by | The current-related suspended load transport with wave stirring is given by | ||
{{Equation| | {{Equation|math \frac{q_s}{\sqrt{ (s-1) g d^3 }} = U c_R \frac{\epsilon}{w_s} \biggl[ 1 - \exp{ \biggl( - \frac{w_s d}{\epsilon}} \biggr) \biggr] /math|2=2}} | ||
The reference sediment concentration is obtained from | The reference sediment concentration is obtained from | ||
{{Equation| | {{Equation|math c_R = A_{cR} \exp{ \biggl( - 4.5 \frac{\theta_{cr}}{\theta_{cw}}} \biggr) /math|2=3}} | ||
where the coefficient | where the coefficient mathA_{cR}/math is given by | ||
{{Equation| | {{Equation|math A_{cR} = 3.5x10^3 \exp{ \bigl( - 0.3 d_{*} } \bigr) /math|2=4}} | ||
with | with math d_{*} = d \sqrt{(s-1) g \nu^{-2}} /math being the dimensionless grain size and math \nu /math the kinematic viscosity of water. | ||
The sediment mixing coefficient is calculated as | The sediment mixing coefficient is calculated as | ||
{{Equation| | {{Equation|math \epsilon = h \biggl( \frac{k_b^3 D_b + k_c^3 D_c + k_w^3 D_w}{\rho} \biggr)^{1/3} /math|2=5}} | ||
== van Rijn == | == van Rijn == | ||
Line 27: | Line 27: | ||
== Watanabe == | == Watanabe == | ||
The equilibrium total load sediment transport rate of Watanabe (1987) is given by | The equilibrium total load sediment transport rate of Watanabe (1987) is given by | ||
{{Equation| | {{Equation|math q_{t*} = A \biggl[ \frac{(\tau_{b,max} - \tau_{cr}) U_c }{\rho g } \biggr] /math|2=6}} | ||
where | where math \tau_{b,max} /math is the maximum shear stress, math \tau_{cr} /math is the critical shear stress of incipient motion, and math A /math is an empirical coefficient typically ranging from 0.1 to 2. | ||
The critical shear stress is determined using | The critical shear stress is determined using | ||
{{Equation| | {{Equation|math \tau_{cr} = (\rho_s - \rho) g d \phi_{cr} /math|2=6}} | ||
In the case of currents only the bed shear stress is determined as | In the case of currents only the bed shear stress is determined as math \tau_{c} = \frac{1}{8}\rho g f_c U_c^2 /math where math f_c /math is the current friction factor. The friction factor is calculated as math f_c = 0.24log^{-2}(12h/k_{sd}) /math where math k_{sd} /math is the Nikuradse equivalent sand roughness obtained from math k_{sd} = 2.5d_{50} /math. | ||
If waves are present, the maximum bed shear stress | If waves are present, the maximum bed shear stress math\tau_{b,max} /math is calculated based on Soulsby (1997) | ||
{{Equation| | {{Equation|math \tau_{max} = \sqrt{(\tau_m + \tau_w \cos{\phi})^2 + (\tau_w \sin{\phi})^2 } /math|2=6}} | ||
where | where math \tau_m /math is the mean shear stress by waves and current over a wave cycle, math \tau_w /math is the mean wave bed shear stress, and math \phi /math is the angle between the waves and the current. The mean wave and current bed shear stress is | ||
{{Equation| | {{Equation|math \tau_{m} = \tau_c \biggl[ 1 + 1.2 \biggl( \frac{\tau_w}{\tau_c + \tau_c} \biggr)^{3.2} \biggr] /math|2=6}} | ||
The wave bed shear stress is given by | The wave bed shear stress is given by math \tau_{w} = \frac{1}{2}\rho g f_w U_w^2 /math where math f_w /math is the wave friction factor, and math U_w /math is the wave orbital velocity amplitude based on the significant wave height. | ||
The wave friction factor is calculated as (Nielsen 1992) | The wave friction factor is calculated as (Nielsen 1992) mathf_w = \exp{5.5R^{-0.2}-6.3}/math where | ||
where | where math R /math is the relative roughness defined as math R = A_w/k_{sd} /math and math A_w /math is semi-orbital excursion math A_w = U_w T / (2 \pi) /math. | ||
== Soulsby-van Rijn == | == Soulsby-van Rijn == | ||
The equilibrium sediment concentration is calculated as (Soulsby 1997) | The equilibrium sediment concentration is calculated as (Soulsby 1997) | ||
{{Equation| | {{Equation|math C_{*} = \frac{A_{sb}+A_{ss}}{h} \biggl[ \biggl( U_c^2 + 0.018 \frac{U_{rms}^2}{C_d} \biggr)^{0.5} - u_{cr} \biggr]^{2.4} /math|2=7}} | ||
---- | ---- | ||
{| border= | {| border=1 | ||
! Symbol !! Description !! Units | ! Symbol !! Description !! Units | ||
|- | |- | ||
| | |math q_{bc} /math || Bed load transport rate || msup3/sup/s | ||
|- | |- | ||
| | |math s /math || Relative density || - | ||
|- | |- | ||
| | |math \theta_{c} /math || Shields parameter due to currents || - | ||
|- | |- | ||
| | |math \theta_{cw} /math || Shields parameter due to waves and currents || - | ||
|- | |- | ||
| | |math \theta_{cw}/math || Critical shields parameter || - | ||
|- | |- | ||
| | |math a_c /math || Empirical coefficient || - | ||
|- | |- | ||
| | |math b_c /math || Empirical coefficient || - | ||
|- | |- | ||
| | |math U_c /math || Current magnitude || m/s | ||
|} | |} | ||
== References == | == References == | ||
* Camenen, B., and Larson, M. (2005). | * Camenen, B., and Larson, M. (2005). A bed load sediment transport formula for the nearshore, Estuarine, Coastal and Shelf Science, 63, 249-260. | ||
* Camenen, B., and Larson, M. (2007). | * Camenen, B., and Larson, M. (2007). A unified sediment transport formulation for coastal inlet applications, ERDC/CHL-TR-06-7, US Army Engineer Research and Development Center, Coastal and Hydraulics Laboratory, Vicksburg, MS. | ||
* Camenen, B., and Larson, M., (2008). | * Camenen, B., and Larson, M., (2008). A General Formula for Non-Cohesive Suspended Sediment Transport, Journal of Coastal Research, 24(3), 615-627. | ||
* Soulsby, D.H. (1997). | * Soulsby, D.H. (1997). Dynamics of marine sands. A manual for practical applications, Thomas Telford Publications, London, England, 249 p. | ||
* Watanabe, A. (1987). | * Watanabe, A. (1987). 3-dimensional numerical model of beach evolution, Proceedings Coastal Sediments '87, ASCE, 802-817. |
Revision as of 01:16, 17 January 2011
Lund-CIRP
Camenen and Larson (2005, 2007, and 2008) developed a general sediment transport formula for bed and suspended load under combined waves and currents.
Bed load
The current-related bed load transport with wave stirring is given by
math \frac{q_{b | ({{{2}}}) |
{\sqrt{(s-1)gd^3}} = a_c \sqrt{\theta_c} \theta_{cw}\exp{ \biggl ( -b_c \frac{\theta_{cr}}{\theta_{cw}}} \biggr ) /math|2=1}}
Suspended load
The current-related suspended load transport with wave stirring is given by
math \frac{q_s}{\sqrt{ (s-1) g d^3 | ({{{2}}}) |
= U c_R \frac{\epsilon}{w_s} \biggl[ 1 - \exp{ \biggl( - \frac{w_s d}{\epsilon}} \biggr) \biggr] /math|2=2}}
The reference sediment concentration is obtained from
{{{1}}} | ({{{2}}}) |
{\theta_{cw}}} \biggr) /math|2=3}}
where the coefficient mathA_{cR}/math is given by
{{{1}}} | (4) |
with math d_{*} = d \sqrt{(s-1) g \nu^{-2}} /math being the dimensionless grain size and math \nu /math the kinematic viscosity of water.
The sediment mixing coefficient is calculated as
{{{1}}} | (5) |
van Rijn
Watanabe
The equilibrium total load sediment transport rate of Watanabe (1987) is given by
{{{1}}} | (6) |
where math \tau_{b,max} /math is the maximum shear stress, math \tau_{cr} /math is the critical shear stress of incipient motion, and math A /math is an empirical coefficient typically ranging from 0.1 to 2.
The critical shear stress is determined using
{{{1}}} | (6) |
In the case of currents only the bed shear stress is determined as math \tau_{c} = \frac{1}{8}\rho g f_c U_c^2 /math where math f_c /math is the current friction factor. The friction factor is calculated as math f_c = 0.24log^{-2}(12h/k_{sd}) /math where math k_{sd} /math is the Nikuradse equivalent sand roughness obtained from math k_{sd} = 2.5d_{50} /math.
If waves are present, the maximum bed shear stress math\tau_{b,max} /math is calculated based on Soulsby (1997)
{{{1}}} | (6) |
where math \tau_m /math is the mean shear stress by waves and current over a wave cycle, math \tau_w /math is the mean wave bed shear stress, and math \phi /math is the angle between the waves and the current. The mean wave and current bed shear stress is
{{{1}}} | (6) |
The wave bed shear stress is given by math \tau_{w} = \frac{1}{2}\rho g f_w U_w^2 /math where math f_w /math is the wave friction factor, and math U_w /math is the wave orbital velocity amplitude based on the significant wave height.
The wave friction factor is calculated as (Nielsen 1992) mathf_w = \exp{5.5R^{-0.2}-6.3}/math where
where math R /math is the relative roughness defined as math R = A_w/k_{sd} /math and math A_w /math is semi-orbital excursion math A_w = U_w T / (2 \pi) /math.
Soulsby-van Rijn
The equilibrium sediment concentration is calculated as (Soulsby 1997)
{{{1}}} | ({{{2}}}) |
{h} \biggl[ \biggl( U_c^2 + 0.018 \frac{U_{rms}^2}{C_d} \biggr)^{0.5} - u_{cr} \biggr]^{2.4} /math|2=7}}
Symbol | Description | Units |
---|---|---|
math q_{bc} /math | Bed load transport rate | msup3/sup/s |
math s /math | Relative density | - |
math \theta_{c} /math | Shields parameter due to currents | - |
math \theta_{cw} /math | Shields parameter due to waves and currents | - |
math \theta_{cw}/math | Critical shields parameter | - |
math a_c /math | Empirical coefficient | - |
math b_c /math | Empirical coefficient | - |
math U_c /math | Current magnitude | m/s |
References
- Camenen, B., and Larson, M. (2005). A bed load sediment transport formula for the nearshore, Estuarine, Coastal and Shelf Science, 63, 249-260.
- Camenen, B., and Larson, M. (2007). A unified sediment transport formulation for coastal inlet applications, ERDC/CHL-TR-06-7, US Army Engineer Research and Development Center, Coastal and Hydraulics Laboratory, Vicksburg, MS.
- Camenen, B., and Larson, M., (2008). A General Formula for Non-Cohesive Suspended Sediment Transport, Journal of Coastal Research, 24(3), 615-627.
- Soulsby, D.H. (1997). Dynamics of marine sands. A manual for practical applications, Thomas Telford Publications, London, England, 249 p.
- Watanabe, A. (1987). 3-dimensional numerical model of beach evolution, Proceedings Coastal Sediments '87, ASCE, 802-817.