Outline of Presentation : Richardson number control of saturated suspension
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Transcript of Outline of Presentation : Richardson number control of saturated suspension
Outline of Presentation:
• Richardson number control of saturated suspension• Under-saturated (weakly stratified) sediment suspensions• Critically saturated (Ricr-controlled) sediment suspensions• Hindered settling, over-saturation, and collapse of turbulence
Interactions of Turbulence and Suspended Sediment
Carl FriedrichsVirginia Institute of Marine Science
Presented at Warnemünde Turbulence DaysVilm, Germany, 5 September 2011
g = accel. of gravitys = (s - )/ c = sediment mass conc.s = sediment density
Stratification
Shear=c < 0.3 g/l c > 0.3 g/l
Amazon Shelf (Trowbridge & Kineke, 1994)
Ri ≈ Ricr ≈ O(1/4)
For c > ~ 300 mg/liter Sedi
men
t gra
dien
t Ric
hard
son
num
ber
Sediment concentration (grams/liter)
0.25
When strong currents are present, mud remains turbulent and in suspension at a concentration that gives Ri ≈ Ricr ≈ 1/4:
Gradient RichardsonNumber (Ri) = density stratification
velocity shearShear instabilities occur for Ri < Ricr
“ “ suppressed for Ri > Ricr
Ri
-
(a) If excess sediment enters bottom boundary layer or bottom stress decreases, Ri beyond Ric, critically damping turbulence. Sediment settles out of boundary layer. Stratification is reduced and Ri returns to Ric.
(b) If excess sediment settles out of boundary layer or bottom stress increases, Ri below Ric and turbulence intensifies. Sediment re-enters base of boundary layer. Stratification is increased in lower boundary layer and Ri returns to Ric.
Sediment concentration
Hei
ght a
bove
bed
Sediment concentrationH
eigh
t abo
ve b
ed
Ri = Ric Ri < Ric
Ri > Ric
Ri = Ric
Large supply of easily suspended sediment creates negative feedback:
Gradient RichardsonNumber (Ri) = density stratification
velocity shearShear instabilities occur for Ri < Ricr
“ “ suppressed for Ri > Ricr
(a) (b)
Are there simple, physically-based relations to predict c and du/dz related to Ri?
Sediment concentration
Heig
ht a
bove
bed
Ri = Ricr
Ri > Ricr
Ri < Ricr
Consider Three Basic Types of Suspensions
3) Over-saturated -- Settling limited
1) Under-saturated-- Supply limited
2) Critically saturated load
Outline of Presentation:
• Richardson number control of saturated suspension• Under-saturated (weakly stratified) sediment suspensions• Critically saturated (Ricr-controlled) sediment suspensions• Hindered settling, over-saturation, and collapse of turbulence
Interactions of Turbulence and Suspended Sediment
Carl FriedrichsVirginia Institute of Marine Science
Presented at Warnemünde Turbulence DaysVilm, Germany, 5 September 2011
(Dyer, 1986)
Const. = 1/k
Dimensionless analysis of bottom boundary layer in the absence of stratification:
h = thickness of boundary layer or water depth, n = kinematic viscosity, u* = (tb/)1/2 = shear velocity
i.e.,
Outer Layer
Overlap Layer: z/h << 1 & n/(zu*) << 1
n/(zu*) << 1
Variables du/dz, z, h, n, u*
z/h << 1
(a.k.a. “log-layer”)
Boundary layer - current log layer
(Wright, 1995)
zo = hydraulic roughness
“Overlap” layer
n/(zu*) << 1
z/h << 1
Bottom boundary layer often plotted on log(z) axis:
Dimensionless analysis of overlap layer with (sediment-induced) stratification:
Dimensionless ratio
= “stability parameter”
Additional variableb = Turbulent buoyancy flux
Heig
ht a
bove
the
bed,
z
u(z)
s = (s – )/ ≈ 1.6c = sediment mass conc.
w = vertical fluid vel.
Rewrite f(z) as Taylor expansion around z = 0:
= 1 = a≈ 0 ≈ 0
From atmospheric studies, a ≈ 4 - 5
If there is stratification (z > 0) then u(z) increases faster with z than homogeneous case.
Deriving impact of z on structure of overlap (a.k.a. “log” or “wall”) layer
Current Speed
Log
elev
atio
n of
hei
ght a
bove
bed
z as z
well-mixedstratified
(i)
(iii)
(ii)
z is constant in z
well-mixed stratified
well-mixed stratified
z as z
-- Case (i): No stratification near the bed (z = 0 at z = z0). Stratification and z increase with increased z.-- Eq. (1) gives u increasing faster and faster with z relative to classic well-mixed log-layer.(e.g., halocline being mixed away from below)
-- Case (ii): Stratified near the bed (z > 0 at z = z0). Stratification and z decreases with increased z.-- Eq. (1) gives u initially increasing faster than u, but then matching du/dz from neutral log-layer.(e.g., fluid mud being entrained by wind-driven flow)
z0
z0
z0
Eq. (1)
-- Case (iii): uniform z with z. Eq (1) integrates to
-- u remains logarithmic, but shear is increased buy a factor of (1+az)
(Friedrichs et al, 2000)
Overlap layer scaling modified by buoyancy flux
Definition of eddy viscosity
Eliminate du/dz and get
-- As stratification increases (larger z), Az decreases
-- If z = const. in z, Az increases like u*z , and the result is still a log-profile.
Effect of stratification (via z) on eddy viscosity (Az)
Connect stability parameter, z, to shape of concentration profile, c(z):
Definition of z: Rouse balance (Reynolds flux
= settling):
Combine to eliminate <c’w’> :z = const. in z if
(Assuming ws is const. in z)
If suspended sediment concentration, C ~ z-A
Then A <,>,= 1 determines shape of u profile(Friedrichs et al, 2000)
If A < 1, c decreases more slowly than z-1
z increases with z, stability increases upward, u is more concave-down than log(z)
If A > 1, c increases more quickly than z-1
z decreases with z, stability becomes less pronounced upward,u is more concave-up than log(z)
If A = 1, c ~ z-1
z is constant with elevationstability is uniform in z,u follows log(z) profile
z = const. in z if
Fit a general power-law to c(z) of the form
Then
Current Speed
Log
elev
atio
n of
hei
ght a
bove
bed
z as z
well-mixedstratified
(i)
(iii)
(ii)
z is constant in z
well-mixed stratified
well-mixed stratified
z0
z0
z0
z as z
A < 1
A = 1
A > 1
STATAFORM mid-shelf site, Northern California, USA
Inner shelf, Louisiana
USA
Eckernförde Bay,Baltic Coast,
Germany
If suspended sediment concentration, C ~ z-A
A < 1 predicts u more concave-down than log(z)A > 1 predicts u more concave-up than log(z)A = 1 predicts u will follow log(z)
Testing this relationship using observations from bottom boundary layers:
(Friedrichs & Wright, 1997;Friedrichs et al, 2000)
STATAFORM mid-shelf site, Northern California, USA,
1995, 1996
Inner shelf, Louisiana, USA,1993
-- Smallest values of A < 1 are associated with concave-downward velocities on log-plot.-- Largest value of A > 1 is associated with concave-upward velocities on log-plot.-- Intermediate values of A ≈ 1 are associated with straightest velocities on log-plot.
A ≈ 0.11
A ≈ 3.1
A ≈ 0.35
A ≈ 0.73
A ≈ 1.0
If suspended sediment concentration, C ~ z-A
A < 1 predicts u more convex-up than log(z)A > 1 predicts u more concave-up than log(z)A = 1 predicts u will follow log(z)
Eckernförde Bay, Baltic Coast, Germany, spring 1993
-- Salinity stratification that increases upwards cannot be directly represented by c ~ z-A. Friedrichs et al. (2000) argued that this case is dynamically analogous to A ≈ -1.
(Friedrichs & Wright, 1997)
Observations showing effect of concentration exponent A on shape of velocity profile
Normalized burst-averaged current speed
Nor
mal
ized
log
of s
enso
r hei
ght a
bove
bed
Observations also show: A < 1, concave-down velocityA > 1, concave-up velocity
A ~ 1, straight velocity profile(Friedrichs et al, 2000)
Outline of Presentation:
• Richardson number control of saturated suspension• Under-saturated (weakly stratified) sediment suspensions• Critically saturated (Ricr-controlled) sediment suspensions• Hindered settling, over-saturation, and collapse of turbulence
Interactions of Turbulence and Suspended Sediment
Carl FriedrichsVirginia Institute of Marine Science
Presented at Warnemünde Turbulence DaysVilm, Germany, 5 September 2011
Relate stability parameter, z, to Richardson number:
Definition of gradient Richardson number associated with suspended sediment:
Original definition and application of z:
Assume momentum and mass are mixed similarly:
So a constant z with height also leads to a constant Ri with height.
Also, if z increases (or decreases) with height Ri correspondingly increases (or decreases).
Relation found for eddy viscosity:
Definition of eddy diffusivity:
Combine all these and you get:
(Friedrichs et al, 2000) Current Speed
Log
elev
atio
n of
hei
ght a
bove
bed
z and Ri as z
well-mixedstratified
(i)
(iii)
(ii)
z and Ri are constant in z
well-mixed stratified
well-mixed stratified
z0
z0
z0
A < 1
A = 1
A > 1z and Ri as z
If suspended sediment concentration, C ~ z-A
then A <,>,= 1 determines shape of u profileand also the vertical trend in z and Ri
z and Ri const. in z if
thenDefine
If A < 1, c decreases more slowly than z-1
z and Ri increase with z, stability increases upward, u is more concave-down than log(z)
If A > 1, c decreases more quickly than z-1
z and Ri decrease with z, stability becomes less pronounced upward,u is more concave-up than log(z)
If A = 1, c ~ z-1
z and Ri are constant with elevationstability is uniform in z,u follows log(z) profile
Sediment concentration
Heig
ht a
bove
bed
Ri = Ricr
Ri > Ricr
Ri < Ricr
Now focus on the case where Ri = Ricr (so Ri is constant in z over “log” layer)
3) Over-saturated -- Settling limited
1) Under-saturated-- Supply limited
2) Critically saturated load
Eliminate Kz and integrate in z to get
Connection between structure of sediment settling velocity to structure of “log-layer” when Ri = Ricr in z (and therefore z is constant in z too).
Rouse Balance:
Earlier relation for eddy viscosity:
But we already know when Ri = const.
So and when Ri = Ricr
when Ri = Ricr . This also means that when Ri = Ricr :
STATAFORM mid-shelf site, Northern California, USA
Mid-shelf site off Waiapu River, New Zealand
(Wright, Friedrichs et al., 1999;Maa, Friedrichs, et al., 2010)
(a) Eel shelf, 60 m depth, winter 1995-96(Wright, Friedrichs, et al. 1999)
Velocity shear du/dz (1/sec)
10 - 40 cm40 - 70 cm
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.410-2
10-1
100
101
Ricr = 1/4Se
dim
ent g
radi
ent R
icha
rdso
n nu
mbe
r
(b) Waiapu shelf, NZ, 40 m depth, winter 2004(Ma, Friedrichs, et al. in 2008)
Ricr = 1/4
18 - 40 cm
Application of Ricr log-layer equations fo Eel shelf, 60 m depth, winter 1995-96
(Souza & Friedrichs, 2005)
Outline of Presentation:
• Richardson number control of saturated suspension• Under-saturated (weakly stratified) sediment suspensions• Critically saturated (Ricr-controlled) sediment suspensions• Hindered settling, over-saturation, and collapse of turbulence
Interactions of Turbulence and Suspended Sediment
Carl FriedrichsVirginia Institute of Marine Science
Presented at Warnemünde Turbulence DaysVilm, Germany, 5 September 2011
Sediment concentration
Heig
ht a
bove
bed
Ri = Ricr
Ri > Ricr
Ri < Ricr
Now also consider over-saturated cases:
3) Over-saturated -- Settling limited
1) Under-saturated-- Supply limited
2) Critically saturated load
More Settling(Mehta & McAnally,
2008)
Starting at around 5 - 8 grams/liter, the return flow of water around settling flocs creates so much drag on neighboring flocs that ws starts to decrease with additional increases in concentration.
At ~ 10 g/l, ws decreases so much with increased C that the rate of settling flux decreases with further increases in C. This is “hindered settling” and can cause a strong lutecline to form.
Hindered settling below a lutecline defines “fluid mud”. Fluid mud has concentrations from about 10 g/l to 250 g/l. The upper limit on fluid mud depends on shear. It is when “gelling” occurs such that the mud can support a vertical load without flowing sideways.
(Van Maren, Winterwerp, et al., 2009)
(g/li
ter)
ws
Saturated flow
(Winterwerp, 2011)
-- 1-DV k-e model based on components of Delft 3D-- Sediment in density formulation-- Flocculation model-- Hindered settling model
(Ozedemir, Hsu & Balachandar, in press)
U ~ 60 cm/sC ~ 10 g/liter
LES modelFixed sediment supply
ws = 0.45 mm/s
ws = 0.75 mm/s
(Ozedemir, Hsu & Balachandar, in press)
U ~ 60 cm/sC ~ 10 g/liter
LES model
ws = 0.45 mm/s ws = 0.75 mm/s
Profiles of flux Richardson number at time of max free stream U
Outline of Presentation:
• Richardson number control of saturated suspension• Under-saturated (weakly stratified) sediment suspensions• Critically saturated (Ricr-controlled) sediment suspensions• Hindered settling, over-saturation, and collapse of turbulence
Interactions of Turbulence and Suspended Sediment
Carl FriedrichsVirginia Institute of Marine Science
Presented at Warnemünde Turbulence DaysVilm, Germany, 5 September 2011