Seminar Coastal Morphodynamics Lecturers

Seminar Coastal Morphodynamics Lecturers

Seminar Coastal Morphodynamics IMAU, Utrecht University, 2008 Lecturers: Prof. dr. Paolo Blondeaux Prof. dr. Giovanna Vittori Dpt. of Environmental Engineering University of Genoa, Italy Huib de Swart 2 1 General objective of this seminar Discuss physical processes that cause the presence of undulations of the sea bottom Example 1: Ripples at the beach Horizontal length scale ~ 10 cm ; height ~ 2 cm Generation timescale ~ hours Due to: waves Relevance: wave prediction, estimation of sediment transport 3 Example 2: Tidal sand waves Horizontal length scale ~ 500 m; height ~ 2 m Generation timescale ~ years Due to: tides Relevance: e.g, buckling of pipelines, navigation 4 2 Sand waves in the Marsdiep 5 Example 3: Sand ridges on the outer and inner shelf Britain Netherlands North Sea Tidal sand ridges Shoreface-connected sand ridges Horizontal length scale ~ km; height ~ 5-10 m Generation timescale ~ 100 years Due to: tides and storm-driven currents Relevance: sand mining, coastal stability 6 3 Research questions 1. Which mechanisms are responsible for the formation and maintenance of rhythmic topography in coastal seas? 2. Can we predict the characteristics of bedforms? • spatial pattern • migration speed • height 3. What is the response of bottom patterns to - human interventions (e.g., extraction of sand)? - sea level changes? 7 Research approaches: 1. Collection and analysis of field observations (identify phenomena+ describe behaviour) Problems: • lack of data • selection of spatial + temporal resolution • selection of spatial + temporal extent • what is transient/nontransient behaviour? 8 4 2. Collection and analysis of laboratory data C. Paolo Univ. of Minnesota Advantages: data obtained under controlled conditions Problems: link to reality (scaling problems) 9 3. Use of empirical or semi-empirical models Model is proposed, field data -> parameter values, next predictions Example: Regeneration of sand waves after dredging (Seto Inland Sea, Japan) Knaapen & Hulscher (2005) Advantages: fast and flexible Disadvantage: yields little insight in basic physics 10 5 4. Use process-oriented numerical models These models use physical laws for water motion, sediment transport and bottom evolution Examples: DELFT3D-MOR MIKE21 (Denmark) Telemac (France) 11 Example: morphodynamic simulation Dutch coastal zone (near IJmuiden) with Delft3D Lesser et al (2004) Advantages: based on physics, results often reliable and useful Disadvantages: slow, difficult to gain insight 12 6 4. Use idealised process-oriented models -Based on simplified descriptions regarding the • geometry • physical processes involved -Designed to gain understanding about the basic physics Example 1: model for tidal sand waves sea surface z tidal current x bottom 13 Example 2: Model for shoreface-connected sand ridges Advantages: fast + flexible, suitable for sensitivity studies Disadvantages: how to choose relevant processes? link with reality 14 7 Idealised models are successful in explaining the formation of many different types of bottom patterns Two types of models: 1. Template models -pattern in the water motion forces the pattern in the bottom -no feedback bottom water motion Example of template pattern: submarine longshore bars 15 2. Self-organisation models -bed forms develop as inherent (or free) instabilities of the coupled water-coupled system -feedback water motion and erodible bottom is crucial side view: brown: bottom blue: water yellow: sand flux growth decay UNSTABLE STABLE spatial/temporal scales of bedforms are uncorrelated with those of external forcing 16 8 Specific objectives of this seminar 1. Discuss structure of models that simulate water motion + their feedbacks with sediment transport and morphology in coastal seas 2. Demonstrate that many bottom patterns in coastal seas emerge as inherent instabilities of the coupled water-bottom system (focus on sand ridges, sand waves and ripples) 3. Behaviour of bedforms can be analysed with mathematical methods (stability analysis) 17 Structure of morphodynamic models: water motion bottom evolution sediment transport We need to - solve the flow structure - find expressions for transport of sediment (due to the water motion) - evolution of the bottom 18 9 Four steps to explore morphodynamic self-organisation: 1. Formulation of a model : water motion bottom evolution sediment transport 2. Find an equilibrium state (without bedforms) 3. Perform linear stability analysis dynamics of small perturbations, arbitrary scales, do they grow? each perturbation -> growth rate mode with the largest growth rate: the preferred mode => spatial pattern, migration speed, growth time scale 4. Perform nonlinear (stability) analysis finite-amplitude behaviour of bars and ridges 19 Example of model output (here: shoreface-connected sand ridges) growth rate versus longshore wavenumber spatial patterns of modes spacing: 7.6 km light colours: crests timescale: ~1000 yr dark colours: troughs migration: 2 m/yr 20 10 Overview of this seminar: 9 oral sessions (default: Monday 11.00-13.00) 9 practise periods (Wednesday 9.00-11.00) Specific time schedule: www.phys.uu.nl/~deswart/morpho08_seminar Credits (3.75 ECTS) will be based on * presence at oral lectures * answers to exercises during practise periods 21 Oral sessions • based on recent key literature • read 1 paper/session as preparation Practise periods • questions about theory • simulations with numerical codes 22 11 Session 2: Modelling sediment transport (29-09-2008) Literature: Huntley, D.A. and A.J. Bowen 1990. Modeling sand transport on continental shelves. In: Modelling Marine Systems 1, 222-254. 23 Session 3: Introduction boundary layer theory (06-10) • Internal friction and coastal morphodynamics • Laminar versus turbulent flow • Vertical structure of oscillatory currents and streaming sea surface residual circulation cells Literature: Mei, C.C. et al, 2007. The applied dynamics of ocean surface waves, section 9.2. World Scientific. 24 12 Session 4: Tidal sand ridges (13-10-2008) Literature: Huthnance, J. 1982. On one mechanism forming linear sand banks. Est. Coastal Shelf Sci. 14, 77-97. 25 Session 5: Sand waves (20-10-2008) Literature: Besio, G., P. Blondeaux, M. Brocchini and G. Vittori, 2004. On the modelling of sand wave migration. J. Geophys. Res. 109 C04018. 26 13 Session 6: Shoreface-connected sand ridges (27-10) Literature: Trowbridge, J. 1995. A mechanism for the formation and maintenance of shore-oblique sand ridges on storm-dominated shelves. J. Geophys. Res. 100 (C8), 16071-16086. 27 Session 7: Turbulent boundary layers under sea waves (10-11-2008) Literature: lecture notes of G. Vittori 28 14 Session 8: Turbulent bottom boundary layers II (17-11) Computed shear stress at the wall versus dimensionless time t Literature: lecture notes of G. Vittori 29 Session 9: Sand ripples under sea waves (24-11) Literature: lecture notes of G. Vittori 30 15 31 Session 8: Turbulent bottom boundary layers II (17-11) eddy viscosity height Literature: lecture notes of G. Vittori 32 16 Session 9: Two equations models (date: ….) Computed shear stress at the wall versus dimensionless time t Literature: lecture notes of G. Vittori 33 17.

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