3 Erosion and Sediment Transport - 3.4 Sediment transport processes Flashcards

1
Q

Total Sediment Load

  1. Bed load (3-20%)
A

grains that slide, roll or hop (saltate) over the bed, with saltation being the most important mechanism.

Bed load differentiate to Contact load and Saltation load

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2
Q

Total Sediment Load

  1. Suspended Load and Wash load (75-95%)
A
  • Suspended load (e): solid material, which are hold in suspension by the equilibrium of vertical forces. Material moves without interacting with the channel bed. Density is higher than that of water.
  • Wash load: as suspended load, but from catchment.
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3
Q

Total Sediment Load

  1. Floating material and Dissolved material (2-5%)
A
  • Floating material: Solid material, which swims on the water (natural material and waste: trees, limbs, leaves, bottles etc.). Density is lower than that of water.
  • Dissolved material: some authors count dissolved material as part of the sediment load. Due to its nature, hydraulic equations for water but not sediment apply.
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4
Q

Definitions: Transport

See pict on slide 39

A

 How much sediment can the channel transport with the available water?

 Is this transport rate greater or smaller than the rate at which sediment is being supplied to a reach?

BED LOAD = rolling, sliding, saltation, saltation (longitudinal/transversal)

SUSPENDED LOAD = suspension

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5
Q

Definitions: Sedimentation

A

 Sedimentation is a process of deposition of a solid material from a state of suspension (particles) or solution (molecules) in a fluid (usually air or water). Sediment is accumulating on the bottom of a creek, river, lake, or wetland.

 Armouring (surface pebbles): generation of a stable covering of the river bed caused by optimal granulometric composition and particle shape of the underlying material.

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6
Q

Remark: Fluvial Hydraulics (berhubung dgn sungai)

A

 This lecture does not deal with fluvial hydraulics!

 You may need basic knowledge in hydraulics to understand sediment transport in depth.

 In particular, we do not calculate flow velocity here!

 Basic equations in fluvial hydraulics:
– Bernoulli equation: one-dimensional stationary flow (no viscosity, no compressibility)
– Saint-Venant equations: calculation of transient flow and water levels
– Navier-Stokes equations: describe the motion of viscous fluid substances including momentum, continuity and energy equations
– Gauckler-Manning-Strickler formula: empirical equation, uses roughness parameters, widely used in practise

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7
Q

Grain Sizes

A

See table on slide 42

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8
Q

Bed load: Characterization via Grain Size Distribution

A

 Collect sediment samples from river bed

 grain size distribution can be obtained by sieving (d > 0.06 mm) or hydrometer analysis with an areometer (0.001 mm < d < 0.125 mm)

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9
Q

Characteristic Grain Diameter

A

 In various equations for bed load simulation, a characteristic grain diameter dm is used.

 In case of very steep grain distribution: dm ≈ d50

 Otherwise, the expectation value of the grain distribution is used for dm:

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10
Q

Models of Sediment Transport

A

 Transport of suspended load and bed load are off different physical nature. That’s why different equations are used.

 Models for bed load use the concept of shear stress. The start of motion depends on stream velocity and bed material.

 Worlds for suspended load can be seen as an extension of bed
load. Here, we want to know when particles lift off the sole and move into suspension state, and when particles sink to the ground.

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11
Q

Forces at the River Bed

See equation and pict on slide 46

A

 Flowing water in a water body exerts a shear force F on the river bed

 F equals the component of weight, which is parallel to the river bed

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12
Q

Angle of Repose (istirahat)

See graph on slide 48

A

Angle of repose for non-cohesive material depending on grain size at 25 % fraction of mass (d25) and depending on the shape of the grains

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13
Q

Shear stress distribution over the cross-section

See pict on slide 49

A

Shear stress distribution over the crosssection

of a trapezoidal profile (approximated)

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14
Q

Critical Shear Stress Values: Cohesive Bed Material

See graph on slide 50

A

Not dependent on diameter, but on void ratio

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15
Q

Critical Shear Stress Values: Non-Cohesive Bed Material

A

See graph on slide 51

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16
Q

Dimensionless Parameters in Sedimentology

A

 The particle Reynolds number Re* allows to describe the flow and sinking behavior via the relationship between inertia and viscosity. With large values of Re*, inertial forces are more important, so flow is more turbulent. In practice, flow is mostly turbulent.

 Particle Reynolds Number Re* [-]

 The particle Froude number FR* expresses the relationship between inertia and gravity.

 Particle Froude No. Fr

 Sedimentological diameter [-]

17
Q

Initiation of Movement

See graph on slide 54

A

Empirical model by Shields (1936): relationship between acting forces and resistance of particles against movement: dimensionless ratio of Reynolds and Froude numbers.

18
Q

Mid Channel Bars

See pict on slide 55

A

 After the beginning of bed load motion, rhythmic bumps form at the sole of the river. These are called mid channel bars.

 Three main forms of transport are differentiated:

a) Riffel: minor irregular bumps at the sole;
b) Dunes: bottom waves with flowing runoff;
c) Anti-dunes: Sole waves with a running drain.

19
Q

Transport equations

A

 There are several empirical transport equations for bridled transport, which are based on the foundations presented before.

 Examples
– Meyer-Peter und Müller (1948)
– Einstein (1950)
– Bagnold-Formel (1966)

20
Q

Types of Transport

A

See graph on slide 57

21
Q

Total Annual Sediment Transport Budget

A

See graph on slide 58

22
Q

General sediment load equations

A

 For long-term analysis on large scale, people often do not use hydraulic models but empirical relationships between catchment properties and sediment load.

 The following types of models are available:
– Empirical erosion models with sediment delivery rate
– Correlation analysis
– Univariate and multi variate regression
– Principal component analysis
– Other data based models, e.g. artificial intelligence

 Challenges and uncertainties:
– Representation of processes in particular the episodic nature of them
– Anthropogenic influences, e.g. reservoirs
– Quality of data

23
Q

Measurement of Sediment Load

A

 Measuring sediment load is very expensive due to high labour cost and valuable devices

 Sediment load is typically measured on single locations, and sporadically. Often, bed load and suspended load are not measured at the same place and time.

 Data about sediment transport are scarce and associated with high uncertainty. Good data are available for some larger rivers.

 Solutions:
– Combine expert opinion and models with some field observations on different scales (field to catchment).
– Determine sediment load via the accumulation of sediments in the catchment, e.g. in reservoirs.
– Derive sediment load from deepening and widening of river beds.

24
Q

Measurement of Bed Load

See pict on slide 61

A

Direct methods:
 movable bed load traps
 fixed bed load traps

Indirect methods:
 acustic measurement
 tracers (load, colourant)

25
Q

Measurement of Bed Load – Example

See pict on slide 62

A

Bed-Load Measuring saystem Dellach/Drautal

-Processing unit
-River gauging
-Suspended load measurement
-Bed-load traps with scales
4D geophones
-Bridge Dellach-Drautal
-Flow velocity meter

26
Q

Measurement of Suspended Load

 Relevance:

A

 Relevance:
– estimation of aggradation, siltation etc.
– oxygen budget, particulate phosphorus transport
– validation of models

 Methods:
– sampling of water: filtering and gravimetric analysis
– measurement of turbidity with photometer or inspection glass
– radioactive measurement of transmission (abatement of radiation)

 Procedure:
– point, multi point or integrative measurements
– suspended load should be determined daily (or at least 2-5 times per week)