CMS-Flow:Transport Formula: Difference between revisions

From CIRPwiki
Jump to navigation Jump to search
(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. ...)
No edit summary
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|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}}
{{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|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}}
{{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|math c_R = A_{cR}  \exp{ \biggl( - 4.5 \frac{\theta_{cr}}{\theta_{cw}}}  \biggr)  /math|2=3}}
{{Equation|<math> c_R = A_{cR}  \exp{ \biggl( - 4.5 \frac{\theta_{cr}}{\theta_{cw}}}  \biggr)  </math>|2=3}}


where the coefficient mathA_{cR}/math is given by
where the coefficient <math>A_{cR}</math> is given by
{{Equation|math A_{cR} = 3.5x10^3 \exp{ \bigl( - 0.3 d_{*} } \bigr)  /math|2=4}}
{{Equation|<math> A_{cR} = 3.5x10^3 \exp{ \bigl( - 0.3 d_{*} } \bigr)  </math>|2=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.  
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|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}}
{{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|math q_{t*} = A \biggl[ \frac{(\tau_{b,max} - \tau_{cr}) U_c }{\rho g } \biggr]  /math|2=6}}
{{Equation|<math> q_{t*} = A \biggl[ \frac{(\tau_{b,max} - \tau_{cr}) U_c }{\rho g } \biggr]  </math>|2=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.
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|math \tau_{cr} = (\rho_s - \rho) g d \phi_{cr} /math|2=6}}
{{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  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.
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)
If waves are present, the maximum bed shear stress <math>\tau_{b,max} </math> is calculated based on Soulsby (1997)
{{Equation|math \tau_{max} = \sqrt{(\tau_m + \tau_w \cos{\phi})^2  + (\tau_w \sin{\phi})^2 } /math|2=6}}
{{Equation|<math> \tau_{max} = \sqrt{(\tau_m + \tau_w \cos{\phi})^2  + (\tau_w \sin{\phi})^2 } </math>|2=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  
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|math \tau_{m} = \tau_c \biggl[ 1 +  1.2 \biggl( \frac{\tau_w}{\tau_c + \tau_c} \biggr)^{3.2} \biggr]  /math|2=6}}
{{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 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 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
The wave friction factor is calculated as (Nielsen 1992) <math>f_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.
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|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}}
{{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=1
{| border="1"
! Symbol !! Description !! Units
! Symbol !! Description !! Units
|-
|-
|math q_{bc} /math || Bed load transport rate || msup3/sup/s
|<math> q_{bc} </math> || Bed load transport rate || m<sup>3</sup>/s
|-
|-
|math s /math ||  Relative density || -
|<math> s </math> ||  Relative density || -
|-
|-
|math \theta_{c}  /math || Shields parameter due to currents || -
|<math> \theta_{c}  </math> || Shields parameter due to currents || -
|-
|-
|math \theta_{cw} /math ||  Shields parameter due to waves and currents || -
|<math> \theta_{cw} </math> ||  Shields parameter due to waves and currents || -
|-
|-
|math \theta_{cw}/math ||  Critical shields parameter  || -
|<math> \theta_{cw}</math> ||  Critical shields parameter  || -
|-
|-
|math a_c /math || Empirical coefficient || -
|<math> a_c </math> || Empirical coefficient || -
|-
|-
|math b_c /math || Empirical coefficient || -
|<math> b_c </math> || Empirical coefficient || -
|-
|-
|math U_c /math || Current magnitude || m/s
|<math> U_c </math> || Current magnitude || m/s
|}
|}


== References ==
== 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. (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. (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.  
* 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.  
* 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.
* Watanabe, A. (1987). "3-dimensional numerical model of beach evolution," Proceedings Coastal Sediments '87, ASCE, 802-817.
 
----
[[CMS#Documentation Portal | Documentation Portal ]]

Revision as of 01:17, 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

  (1)

Suspended load

The current-related suspended load transport with wave stirring is given by

  (2)

The reference sediment concentration is obtained from

  (3)

where the coefficient is given by

  (4)

with being the dimensionless grain size and the kinematic viscosity of water.

The sediment mixing coefficient is calculated as

  (5)

van Rijn

Watanabe

The equilibrium total load sediment transport rate of Watanabe (1987) is given by

  (6)

where is the maximum shear stress, is the critical shear stress of incipient motion, and is an empirical coefficient typically ranging from 0.1 to 2.

The critical shear stress is determined using

  (6)

In the case of currents only the bed shear stress is determined as where is the current friction factor. The friction factor is calculated as where is the Nikuradse equivalent sand roughness obtained from .

If waves are present, the maximum bed shear stress is calculated based on Soulsby (1997)

  (6)

where 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 is the angle between the waves and the current. The mean wave and current bed shear stress is

  (6)

The wave bed shear stress is given by where is the wave friction factor, and is the wave orbital velocity amplitude based on the significant wave height.

The wave friction factor is calculated as (Nielsen 1992) where

where is the relative roughness defined as and is semi-orbital excursion .

Soulsby-van Rijn

The equilibrium sediment concentration is calculated as (Soulsby 1997)

  (7)

Symbol Description Units
Bed load transport rate m3/s
Relative density -
Shields parameter due to currents -
Shields parameter due to waves and currents -
Critical shields parameter -
Empirical coefficient -
Empirical coefficient -
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.

Documentation Portal