Sediment Transport over Ripples and Dunes Stephen R McLean, UC Santa Barbara Jonathan Nelson, USGS, Denver, CO Thanks to: Sandro Orlandi, University of.

Slides:



Advertisements
Similar presentations
Erosion Erosion = the transport of sediments from weathering. *Gravity and Water are biggest factors* 1. Streams 2. Glaciers 3. Landslides 4. Waves.
Advertisements

1B Clastic Sediments Lecture 28 BEDFORMS IN COHESIONLESS SUBSTRATE Structure of bedforms Formative conditions Unidirectional and Oscillating flows NH
Tsunami Induced Turbulent Coherent Structures Tsunami Induced TCS Nearbed TCS Shallow horizontal TCS Near-surface breaking TCS Harbors and Ports Pick up.
Doppler echocardiography & tissue doppler Dolly mathew.
For flow of 1 m/s in round-bottom channel of radius 1 m, what is the Reynold’s number? Is the flow laminar or turbulent? Re < 500 laminar Re > 2000 turbulent.
Sediment Transport Outline
Threshold of Grain Motion 1. Definition - “general sediment movement” beyond occasional motion a. more or less continuous b. includes grains on all surfaces.
Assessment of gravel transport characteristics of the upper Santa Ana River Scott Wright and Toby Minear USGS California Water Science Center Sacramento,
UNIVERSITY OF SOUTH CAROLINA Erosion rate formulation and modeling of turbidity current Ao Yi and Jasim Imran Department of Civil and Environmental Engineering.
Sediment Movement after Dam Removal
Process Geomorphology. 10/13 Objectives Learning Objective: Understand the concepts of driving and resisting forces, and constitutive equations in geomorphologic.
ROLE OF HEADLANDS IN LARVAL DISPERSAL Tim Chaffey, Satoshi Mitarai Preliminary results and research plan.
RELATIONS FOR THE CONSERVATION OF BED SEDIMENT
Equatorial Circulation Subtle changes in winds give rise to complicated surface current patterns Equatorial Undercurrent Focus on Pacific circulation,
Fluxes of water, sediment, and elements class 1.Introduce instrumentation and approach for surveying and flow gauging 2.Introduce and understand Manning’s.
Scaling Up Marine Sediment Transport Patricia Wiberg University of Virginia The challenge: How to go from local, event-scale marine sediment transport.
Computational Investigations of Gravity and Turbidity Currents Eckart Meiburg UC Santa Barbara Motivation Governing equations / computational approach.
Environmental Fluid Mechanics Laboratory
Suspended Load Above certain critical shear stress conditions, sediment particles are maintained in suspension by the exchange of momentum from the fluid.
HYDRAULICS AND SEDIMENT TRANSPORT: RIVERS AND TURBIDITY CURRENTS
2003 Overview of IST Group Results on the Sediment Benchmark 3 rd IMPACT Workshop Louvain-la-Neuve University of Beira Interior João Leal (UBI) Rui Ferreira.
Jiuxing Xing and Alan M. Davies
Sediment transport in wadi systems
Intro to Geomorphology (Geos 450/550) Lecture 5: watershed analyses field trip #3 – Walnut Gulch watersheds estimating flood discharges.
Methods A predictive method will be developed from NBSS measurements and vegetation/channel properties from the flume data. The predictive method will.
Channel Modification Washington Dept. Forestry, 2004, Channel Modification Techniques Katie Halvorson.
THE ROLE OF RELATIVE SUBMERGENCE ON CLUSTER MICROTOPOGRAPHY AND BEDLOAD PREDICTIONS IN MOUNTAIN STREAMS AN Thanos Papanicolaou and Casey Kramer IIHR Hydroscience.
LECTURE 8 LAYER-AVERAGED GOVERNING EQUATIONS FOR TURBIDITY CURRENTS
Suspended Load Bed Load 1. Bedload Transport transport rate of sediment moving near or in contact with bed particles roll or hop (saltate), with grain-to-grain.
Morphodynamics and hydraulics of vegetated river reaches: a case study on the Müggelspree in Germany Alexander Sukhodolov and Tatiana Sukhodolova Institute.
Boundary Layer Velocity Profile z ū Viscous sublayer Buffer zone Logarithmic turbulent zone Ekman Layer, or Outer region (velocity defect layer)
National Consultation with TNMC 3 May 2005, Bangkok WUP-FIN Phase II – Bank erosion study.
Fluid Flow in Rivers Outline 1.Flow uniformity and steadiness 2.Newtonian fluids 3.Laminar and turbulent flow 4.Mixing-length concept 5.Turbulent boundary.
1 Geometric and migrating characteristics of superimposed bedforms under oscillatory flows Ven Te Chow Hydrosystems Laboratory Department of Civil and.
The hydrologic cycle. Running water Streamflow Two types of flow determined primarily by velocity –Laminar flow –Turbulent flow Factors that determine.
The Littoral Sedimentation and Optics Model (LSOM)
R. Akahori & M.W. Schmeeckle
Mechanics and modeling of flow, sediment transport, and morphologic change in riverine lateral separation zones Brandy Logan, Jonathan Nelson, Rich McDonald,
15. Physics of Sediment Transport William Wilcock (based in part on lectures by Jeff Parsons) OCEAN/ESS 410.
Bedforms in Unidirectional Flow
Cross-shore sediment transport
ONE-DIMENSIONAL ANALYSIS ON BEDEVOLUTION ACCOMPANING BANK EROSION Satoru Nakanishi Hokkaido University Graduate School Kazuyoshi Hasegawa Hokkaido University.
Unidirectional Sedimentary Structures
1 A unified description of ripples and dunes in rivers 5 m Douglas Jerolmack, Geophysics, MIT; With David Mohrig and Brandon McElroy.
Sand Motion over Vortex Ripples induced by Surface Waves Jebbe J. van der Werf Water Engineering & Management, University of Twente, The Netherlands.
7. Bedforms in coarse-grained channels Step-pool units Cluster bedforms Riffle-pool sequences.
Aeolian Environments Navajo Sandstone (Jurassic, Utah)Sahara Desert.
Environmental Hydrodynamics Lab. Yonsei University, KOREA RCEM D finite element modeling of bed elevation change in a curved channel S.-U. Choi,
Incision dynamics and shear stress measurements in submarine channels experiments Pierre Lancien François Métivier Eric Lajeunesse Institut de Physique.
Sediment Transport Modelling Lab. The Law of the Wall The law of the wall states that the average velocity of a turbulent flow at a certain point is proportional.
Sergio Jaramillo Uribe Geno R. Pawlak University of Hawaii AUV-Based Observations of Rough Bed Hydrodynamics.
1D Hydraulic Modeling w/ LiDAR Data Noah J. Finnegan 1 1 UC Santa Cruz, Earth & Planetary Sciences.
Weakly nonlinear analysis of dunes by the use of a sediment transport formula incorporating the pressure gradient Satomi Yamaguchi (Port and airport Institute,
Quantification of Near-bed Swash-zone Velocities Using Particle Image Velocimetry Douglas Krafft (1), Jack A. Puleo (1), José Carlos Pintado Patiño (2)
Basic sediment transport
Dynamics & Mass transfer modelling Application Observations
WHAT CONTROLS BAR MIGRATION IN TIDAL CHANNELS?
The Hjulstrom Curve Predicting velocity.
Continuum Mechanics for Hillslopes: Part IV
Reynolds Number Froude Number
Summary In addition to the oceans, where else is water found on Earth?
Linear stability analysis of the formation of beach cusps
Ablation due to Oscillatory Boundary Layer:
Dune-Yardang Interactions in Becquerel Crater, Mars
LCDR John Hendrickson 17SEP2008
Boundary condition controls on the high sand flux regions of Mars
Fluvial Hydraulics CH-3
“Characteristics of Suspended Sediment and Flow in Downstream of Mekong River, Southern Vietnam” 5/22/2019 Duong Thai Bang (M2) (Supervised by Prof. Maki.
Longitudinal Profile Survey for Successful Culvert Replacement
Nature’s drag queens: how vegetation impacts aquatic flows† Marco Ghisalberti Centre for Water Research, University of Western Australia DIALOG VII.
Presentation transcript:

Sediment Transport over Ripples and Dunes Stephen R McLean, UC Santa Barbara Jonathan Nelson, USGS, Denver, CO Thanks to: Sandro Orlandi, University of Bologna Lindsay Gary, UCSB

Ultimate Goal: predict bedform evolution System: Response of flow to topography Response of sediment to flow Response of topography to sediment flux divergence What is the sediment flux over a dune?

Early, fixed bed experiment- effects of acceleration

S Shift relative to upstream ramp crest

Shift relative to reattachment

Research Goal: predict bedform evolution Predict transport rate (Nelson, et al. tomorrow) Measure transport rate Measure near-bed velocity statistics Determine effects of ripples

Experiments Goal: determine relationship between flow and transport 1) Characterize flow 2) Measure transport rate

Instrumentation: Acoustic Doppler Profiler Velocity along four beams (~1 mm bin spacing) ~20 Hz sampling freq; not simultaneous

Quad set-up

Streamwise velocity profile- no upstream ramp

Streamwise velocity profile- with upstream ramp

Reynolds stress- with upstream ramp

Instrumentation: Acoustic Doppler Profiler Velocity along four beams (~1 mm bin spacing) ~20 Hz sampling freq; not simultaneous Multiple transducer array (MTA) 32 acoustic transducers (20mm spacing)

Estimating Transport rate For two-dimensional flow erosion equation yields:

Flat bed downstream of ramp

Time stack- no upstream ramp

Change in bed elevation- no upstream ramp

Time stack – with upstream ramp

Change in bed elevation- with upstream ramp

Stress and transport- no upstream ramp

Nondimensional transport- no upstream ramp

Stress and transport- with upstream ramp

Non-dimensional transport- with upstream ramp

Stress and transport with and without upstream ramp

Comparison with and without upstream ramp

Stress and transport with and without upstream ramp

Comparison between beginning and end of run

General Observations Flow/transport relation not strongly affected by acceleration –Transport decreases as acceleration increases –Near-bed flow decreases as acceleration increases also Concept of critical shear stress plays no role in lee of a separation zone Ripples form almost immediately for the flat bed case Ripples form on steep slopes with no upstream flow separation Ripples do not form on steep slopes downstream of flow separation Ripples seem to enhance transport

Erosion equation versus ripple migration