sediment transport part 1: initial motion
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Sediment transport Part 1: initial motion. GEOL/CE/EEB 8601 Intro to Stream Restoration. Why does it matter?. A common requirement in channel design is that the bed be stable under some specified discharge, i.e. the sediment will not move - PowerPoint PPT PresentationTRANSCRIPT
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Sediment transportPart 1: initial motion
GEOL/CE/EEB 8601 Intro to Stream Restoration
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Why does it matter?
1. A common requirement in channel design is that the bed be stable under some specified discharge, i.e. the sediment will not move
2. Total transport of bed-material sediment plays a major though incompletely understood role in setting channel width
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Why does it matter?
3. Changes in the transport capacity of the reach may cause erosion or deposition
4. In-stream organisms are often sensitive to bed texture, especially fines content of gravel bed streams
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Steps in analyzing sediment mobility
1. Determination of bed sediment characteristics: grain size distribution and texture
2. Will it move? Apply the Shields criterion (Shields diagram)
3. Estimate bed-material transport rate if desired – note that existing formulas are highly imprecise/inaccurate
4. Consider the watershed, boundary conditions and natural history:
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Watershed and historya) What is being supplied from upstream? Does
it/will it/could it include material not represented in the bed (e.g. fines from upland land management)?
b) Is there morphologic evidence (e.g. air photos) for changes in stream type related to sediment supply (e.g. braided vs meandering)?
c) What is the long-term trend (depositing, degrading, bypass)? Why?
d) Are there downstream changes (e.g. reduction in base level) that could lead to aggradation or degradation?
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Step 1. Sediment characterization
• Gravel beds: usually bimodal– Gravel mode: Wolman
count+gravelometer, image-based measurement
– Distinguish surface vs subsurface
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Step 1. Sediment characterization
• Gravel beds: usually bimodal– Greater intrinsic mobility of
sand often leads to higher gravel fraction in surface layer: “armor” or “pavement”
– You can measure GSD of either depending on your purpose. Usually do surface Note higher sand content
– subsurface GSD is usually closer to the GSD of material in transport
Frey & Church Science 2009
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Step 1. Sediment characterization
• Sand beds: usually unimodal– sieve– automated size counter
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Either way you end up with something like this:
Unimodal sand
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or this:Bimodal gravel-sand
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Summary: grain-size distributions
• Logarithmic size scales: ln2 [], -ln2 [], or log10
• Standard form: percentages in size range; cumulative
• Common percentiles: 90, 84, 65, 50, 16
• Unimodel or bimodal (e.g. gravel-sand)
• No standard form at present for single modes (e.g. log-normal)
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Summary: size and mineralogy
• Gravel, cobble, etc: > 2 mm; all common rock lithologies
• Sand: 62 m – 2 mm; quartz, feldspar, other
• Silt: 4 m – 62 m; quartz, feldspar, other• Clay: < 4 m; clay minerals• Cohesive effects important for D <~ 10 m
and/or clay minerals and/or biological effects
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Settling velocity, ws
• Two regimes, distinguished by Reynolds number: Stokes (laminar, R<~1) vs impact (turbulent, R>~100)
• General formula, Ferguson & Church 2004
5.0321
2
)75.0( RgDCC
RgDws
C1 = 18
C2 = 0.4 1
R = s/f – 1
= kinematic viscosity
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Settling velocity
• Rule of thumb, qtz density in water:
for D < 100 m, ws in diam/s D in m
for 100 < D < 1000, ws in diam/s 100 diam/s
D > 1000, ws increases as D1/2
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5.0321 )75.0( RgDCC
RgDws
R < 1
R > 104
C2 1
C2 0.4
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2. Will it move? Shields initial motion
From Buffington (1999)
Duu
Dsg
u
Re
)1(0
2
Shields stress:
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2. Will it move? Shields initial motion
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2. Will it move? Shields initial motion
DgDs-
p)( 1
Re
)7.7(6.06.0
1006.022.0 p
pcRe
Re
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Initial motion: standard conditions
stolen from Peter Wilcock, JHU
Motion
No motion
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What not to use Less objectionable if this is interpreted as initial motion, but still better to use shear stress
Hjulstrom diagram
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What to do about size mixtures?
When grain sizes are clearly segregated into patches like this, you have to apply Shields to each patch separately.
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Within a mixture, all sizes tend to move together up to very large clasts
0.1
1
10
0.1 1 10x
x
50c
ci
Di / D50
Parker; Wilcock; Proffitt & Sutherland
mixture effects diminish for extremely large grain sizes
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Modifying Shields for slope effects
ccoc
tan1cos
tan slope streamwise xS
2/1
2
2tan1cos
ccoc
tan slope lateral yS7.0c
Streamwise slope
Lateral slope
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Transport ofBiota
Hondzo & Wang 02
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Initial motion -- summary• Brownlie formula for Shields curve:
• Correction for streamwise slope:
• Correction for side slope:
• Correction for mixtures:
)7.7(6.06.0
1006.022.0 p
pcRe
Re
NB Parker et al. (2003) have suggested reducing this by a factor of 2
ccoc
tan1cos tan slope streamwise xS
2/1
2
2tan1cos
ccoc
tan slope lateral yS
DgD
p
RRe
5050 D
Dic
ci 85.0
7.0c