Title: Lecture 7a Finish SubTidal Salt Flux Calculations
 1 Lecture 7a  Finish Sub-Tidal Salt Flux 
Calculations Lecture 7b  Introduction to 
Estuarine Boundary Layers
- Outline 
- Review Hansen  Rattray classification 
- Scaling for Length of Salt Intrusion 
- Introduction to unstratified boundary layers 
- Log-layer scaling 
- Eddy-viscosity for a log-layer 
- Drag Coefficients
2Cross-sectional and tidal averaged salt balance
Rate of change in mass of salt landward of 
cross-section
Down-estuary salt flux due to river discharge.
Up-estuary salt flux (all mechanisms)
Tidal pumping  gravitational circulation  
oscillatory shear dispersion
Ratio of tidal pumping to total salt flux 
 3Hudson River Qriver 150 m3/s  ltugt  0.01 m/s
Residual Velocity
Residual Salinity
Usurf  0.3 m/s
?S  5
width (km)
width (km)
Chesapeake Bay Qriver 2000 m3/s  ltugt  0.01 m/s
Residual Velocity
Residual Salinity
?S  6
Usurf  0.15 m/s
width (km)
width (km) 
 4Hansen and Rattray Estuarine Classification
Hudson River
Chesapeake Bay
Gravitational circulation
0.99
Tidal Pumping 
 5For Chesapeake Bay and Hudson River it is 
probably reasonable to assume gravitational 
circulation dominates up-estuary salt flux. 
 6Data from San Francisco Bay Monismith et al. JPO 
(2002)
LQ-1/7
LQ-1/3 
 7Estuarine Boundary Layers
For steady, fully developed turbulent flow (with 
no rotation) 
 8For fully developed, stead flow, depth integrated 
P.G. is balanced by bed stress.
tb
Viscous sublayer thickness 
 9From dimensional analysis, the velocity shear 
(du/dz) must depend on a velocity scale and a 
length scale
The only relevant velocity scale is the shear 
velocity (u)
Assumed constant with z, so often referred to as 
a constant stress layer
The only relevant length scale is the distance 
from the boundary
von Karmans constant  0.41 derived from 
numerous empirical experiments.
Integrate in z, to get velocity distribution
Boundary Condition U  0, _at_ z  zo
Law of the wall
hrough
Roughness height 
 10Mixing Length Model
Momentum flux (stress)  eddy viscosity  
velocity shear
Eddy coefficient is represented as a turbulent 
length scale  turbulent velocity scale
So, for constant stress layer
Alternatively, if you assume velocity scale is 
set by local value of stress
u
L
hbbl
Eddy Viscosity
stress 
 11Scaling for oscillatory turbulent boundary layer
For unstratified flow Az  0.01 m2/s
For tidal boundary layer T  12.42 hours ?  
10-4 s-1
Hbbl  8 m
But what is appropriate value for Az ?
Log-layer scaling
Bed Stress can be represented using a quadratic 
drag law
So if
Zo  0.5mm
From log-scaling
CD  0.003 
 12Homework Problem
Assuming the following
- What is the tidally averaged value of the eddy 
 viscosity?
- Plot it as a function of z. 
- If dS/dx  410-4 m-1 , what is the predicted 
 strength of the residual estuarine circulation
 (Usurf) and stratification (?S) based on your
 estimate of Az.
- How does this compare with the data shown on 
 slide 3?
- What value of Az best matches these values in the 
 Hudson.
- Using this value, calculate the estimated length 
 of the Hudson River salt intrusion if the river
 discharge is 150 m3/s.