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Research group River and delta morphodynamics
Hydraulic Geometry How large is a river?
GEO3-4305, 2014
Dr. Maarten Kleinhans
[email protected]
www.geo.uu.nl/fg/mkleinhans
flow
sediment
transport
morphology
This course: the morphodynamic system
• Introduction
• River flooding
• Hydraulic roughness and
• Bedforms
• Sediment transport
• Mixture effects
• Channel dimensions
• Bars, bends, islands
• Overbank sedimentation
• Channel patterns
Introduction 1. Work done by floods – which floods?
2. Hydraulic geometry – prediction of width
• Parker E-book chapter 3, 2007 WRR paper
3. Partial explanations and future work
• bank stability
BIG QUESTIONS
1. How is channel geometry related to discharge and
how to incorporate meander geometry and floods?
2. Why do channels exist?
What processes explain the dimensions?
Definition of a channel during floods
Bankfull discharge:
width of natural channel, not artificial levees
■difficult! spatial variation in levee height, new banks
Q = uhW (continuity equation ~ mass
conservation)
floodplain width (artificial)
channel
width
channel depth
natural levee
(oeverwal) artificial levees
(winterdijk
of zomerdijk)
The Waal (Ochten) anno 1830: Low flow situation
Example: the River Allier, France • low flow situation
• flood: low-sloping
point bars submerged
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Example: a river in Alaska, USA
Courtesy Addink
Example: the Amazon leveed
turbidity current channel on the shelf
Pirmez et al
Example: the
River
Waimakariri,
New Zealand
What discharge does most work?
Low flow
(Source: Rijkswaterstaat)
Large discharge
(Source:
Rijkswaterstaat Directie Oost-Nederland
/ Slagboom en Peeters Luchtfotografie,
20 March 2001 (7000m3/s)
Rhine, 1st bifurcation
Discharge peaks and work
Key point:
river channel dimensions
do not co-vary with discharge
during a flood
rather, channel dimensions depend on
an effective discharge
that summarises its variation
Flood probability
Herhalingstijden jaarlijkse afvoermaxima Rijn - Lobith
extrapolatie met kansverdeling
0
2000
4000
6000
8000
10000
12000
14000
16000
18000
1 10 100 1000
herhalingstijd (jr)
afv
oer
(m3/s
)
1926 1995
1993
Recurrence time (yr)
dis
char
ge
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Long-term average flood
Maximum and minimum annual discharge
of the Rhine at Lobith
0
2000
4000
6000
8000
10000
12000
14000
1900 1920 1940 1960 1980 2000
year
Bo
ven
rijn
dis
ch
arg
e (
m3/s
)
Channel-forming discharge definitions
Bankfull discharge
observed, depends on morphology
Discharge peak frequency
common: flood of once per 1-2.33 year
mean annual flood
Sediment-transport based
most efficient discharge frequency
discharge that transports annual sediment load
Transport efficiency of floods
Multiply sed tr rate with discharge probability
Q
Qs
Qs=u3 to 5
Q
probability
of Q
Qs
Two options:
1. peak of distribution
2. integral discharge that
transports annual sediment load
probability
of Qs
2 1
So, what discharge?
choice specified for relations in literature!
usually: bankfull discharge (+uncertainty)
long-term morphodynamic modelling of
channel:
discharge that transports annual sediment load
long-term morphodynamic modelling
of channel and floodplain??
2. Hydraulic geometry
Historically: regime equations for stable
(irrigation) canal design ■e.g. Lacey (1929) (Punjab)
At-a-station hydraulic geometry
empirical (many streams) ■ e.g. Leopold & Maddock 1953
computer class!
Downstream hydraulic geometry
increasing W,h with increasing catchment A
changes along the river (from highland to lowland)
Why channels exist...
upstream water and sediment feed
water carries sediment more effectively in
flows deeper than thin sheets
will carve a channel
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At-a-station hydraulic geometry
Lacey type:
perimeter P = aQ1/2 a~4.84
hyd radius R = bQ1/3D1/6 b~0.41
velocity u = cQ1/6D1/6 c~0.50
Leopold-Maddock type (Hey & Thorne 1986):
width w = aQp a~3.67 p~0.45
depth h = bQq b~0.33 q~0.35
velocity u = cQr c~0.83 r~0.20
what are relations between a,b,c and p,q,r ?
Effect of vegetation
1. grassy banks w = 4.33Q0.5
2. 1-5% tree/shrub cover w = 3.33Q0.5
3. 5-50% tree/shrub cover w = 2.73Q0.5
4. >50% tree/shrub cover w = 2.34Q0.5 (Hey & Thorne 1986)
Many other equations
sand/gravel, meandering/braided
Why does vegetation matter?
Consistent predictors for gravel beds
nondimensional width, depth:
relations:
a=4.63, p=0.0667
b=0.382, q=-0.0004
d=0.101, s=0.344
u = Q/(Wh) Parker et al. 2007, J. Geophys. Res., 112, F04005,
doi:10.1029/2006JF000549
5/2
5/1
5/2
5/1
2
~,
~,
~
bf
bf
bf
bfbf
Q
hgh
Q
WgW
DgD
QQ
sqp QdSQbhQaW~
,~~
,~~
Example calculations
Do Lacey, Hey-Thorne and Parker et al.
calculate W,h,u
two rivers:
Q = 2500 m3/s
D = 0.3 or 3 mm
Downstream geometry (1): slope
Concave long-profiles
slope decreases downstream
logarithmic or exponential approximation
Why?
mountains do not have straight slopes
discharge increases downstream (tributaries)
sediment transport capacity increases
downstream fining?
S = aQb Dc
a ~ 0.05, b ~ -0.4, c ~ 0.7
Knighton fig 5.26
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Downstream geometry (2)
imagine a river:
with increasing downstream discharge
decreasing downstream grain size
and increasing downstream silt-clay deposition
S = 0.05 Q-0.4 D0.7
w = 5.54 Q0.58 M-0.37 M=%mud
h = 0.12 Q0.42 M0.35
Schumm (1971, eq. 5.23-24 in Knighton p. 175)
Downstream implications?
Downstream implications
decreasing slope
higher water levels, longer backwaters
flow deceleration despite Q increase!
mud deposition!!
slowing increase of width
mud deposition increases strength of banks
faster increase of depth
width-depth ratio smaller
change from braided to meandering
pattern possible
Threshold channel concept
Imagine river in sand without mud / vegetation
θc,banks < θc,bed (slope of bank!)
initially: θ >> θc
so, erosion of bank toe and collapse of bank!
eroded sediment deposited on bed
shallowing
continue until θ = θc in bankfull conditions
‘threshold channel’
Example: the
River
Waimakariri,
New Zealand
Effect on bankfull Shields number
threshold channels: θbf ~ 1.2θc ~ 0.02-0.06
channels with cohesive banks: higher
Parker hypothesis E-book chapter 3, 24
next class: channel patterns
effect of width on bar pattern
effect of bank strength on channel pattern
Bank strength! Now add vegetation (roots) or mud to bank
equilibrium channel will be narrower
bank strength:
bank height and gradient
soil cohesion
root strength
Coulomb friction (remember Mohr circles?)
hydraulic head
■water inflow before flood and outflow after flood
banks weaker after flood peak
NB capacity to remove eroded bank material
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Example: the River Allier, France • low flow situation
• flood: low-sloping
point bars submerged
Bank erosion is not simple
An
dre
w S
imo
n e
t a
l (U
SG
S)
Slingebeek
Brahmaputra
Bank stability and toe erosion model
Andrew Simon et al (USGS)
Mohr-Coulomb equation:
where
τf = shear stress at failure (Pa)
σ = normal stress (Pa)
μw = pore-water pressure (Pa)
φ’ = effective angle of internal friction
c' =effective cohesion (Pa)
■ chemical bonding, plant roots!
'tan' wfailure c
http://www.ars.usda.gov/Research/docs.htm?docid=5044
Geometry of meanders
Empirical relations
discharge
wavelength
→ e.g. λ=10W
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Bend migration
Sharper bend, faster erosion
why the optimum?
Empirical curves
bend in theerosion M
tcoefficien and radius bend critical with
:/for and
: caseIn
2
2
kc
cW
rk
W
McWr
r
cWk
W
Mcr/W
Allier Big questions
How is channel geometry related to
discharge and how to incorporate meander
geometry and floods?
Why do channels exist? What processes
explain the dimensions?