Modeling the Impact of Extreme Events on Margin Sedimentation

Similar documents
Swash Zone Dynamics: Modeling and Data Analysis

Testing Turbulence Closure Models Against Oceanic Turbulence Measurements

SW06 Shallow Water Acoustics Experiment Data Analysis

Parameterizing the Effects of Upper-Ocean Large Eddies on Air-Sea Interaction

Marginal Sea - Open Ocean Exchange

Mine Burial Studies with a Large Oscillating Water-Sediment Tunnel (LOWST)

Modeling of Coastal Ocean Flow Fields

Generation and Propagation of Internal Solitary Waves on the Continental Shelf and Slope

Determining the Stratification of Exchange Flows in Sea Straits

Internal Tide Generation in the Indonesian Seas

Mass Transport by Second Mode Internal Solitary Waves

Super-Parameterization of Boundary Layer Roll Vortices in Tropical Cyclone Models

Ocean Acoustics Turbulence Study

Scattering of Internal Gravity Waves at Finite Topography

Super-Parameterization of Boundary Layer Roll Vortices in Tropical Cyclone Models

Closed-form and Numerical Reverberation and Propagation: Inclusion of Convergence Effects

Topographic Effects on Stratified Flows

Coastal Mixing and Optics

Shelf And Slope Sediment Transport In Strataform

Coupled Ocean-Atmosphere Modeling of the Coastal Zone

Ocean Model Development for COAMPS

Margin Morphodynamics: Debris Flows, Turbidity Currents and Experimental Margin Stratigraphy

FRACTAL CONCEPTS AND THE ANALYSIS OF ATMOSPHERIC PROCESSES

Report Documentation Page

Models of Marginal Seas Partially Enclosed by Islands

Understanding Near-Surface and In-cloud Turbulent Fluxes in the Coastal Stratocumulus-topped Boundary Layers

Analysis of South China Sea Shelf and Basin Acoustic Transmission Data

Flocculation, Optics and Turbulence in the Community Sediment Transport Model System: Application of OASIS Results

Predicting Tropical Cyclone Formation and Structure Change

High Resolution Surface Characterization from Marine Radar Measurements

Analysis of Mixing and Dynamics Associated with the Dissolution of Hurricane-Induced Cold Wakes

Sediment Flux and Trapping on the Skagit Tidal Flats

Computer Simulation of Sand Ripple Growth and Migration.

A 1/10th Degree Global Ocean Simulation Using the Parallel Ocean Program

Advanced Numerical Methods for NWP Models

Internal Waves and Mixing in the Aegean Sea

Dynamics of Boundary Currents and Marginal Seas

Two-Dimensional Simulation of Truckee River Hydrodynamics

Diagonal Representation of Certain Matrices

INTERACTION AND REMOTE SENSING OF SURFACE WAVES AND TURBULENCE

Grant Number: N IP To compare obtained theoretical results with NPAL experimental data.

Regional Stratification and Shear of the Various Streams Feeding the Philippine Straits ESR Component

PIPS 3.0. Pamela G. Posey NRL Code 7322 Stennis Space Center, MS Phone: Fax:

Understanding Near-Surface and In-Cloud Turbulent Fluxes in the Coastal Stratocumulus-Topped Boundary Layers

Weak Turbulence in Ocean Waves

High-Fidelity Computational Simulation of Nonlinear Fluid- Structure Interaction Problems

Use of Wijsman's Theorem for the Ratio of Maximal Invariant Densities in Signal Detection Applications

Nonlinear Internal Waves: Test of the Inverted Echo Sounder

Sea Ice Model for Marginal Ice Zone

An Examination of 3D Environmental Variability on Broadband Acoustic Propagation Near the Mid-Atlantic Bight

Impact of Typhoons on the Western Pacific Ocean DRI: Numerical Modeling of Ocean Mixed Layer Turbulence and Entrainment at High Winds

Range-Dependent Acoustic Propagation in Shallow Water with Elastic Bottom Effects

An Observational and Modeling Study of Air-Sea Fluxes at Very High Wind Speeds

Broadband matched-field source localization in the East China Sea*

Modeling the Formation and Offshore Transport of Dense Water from High-Latitude Coastal Polynyas

Improved Parameterizations Of Nonlinear Four Wave Interactions For Application In Operational Wave Prediction Models

Using Dye to Study Lateral Mixing in the Ocean: 100 m to 1 km

Volume 6 Water Surface Profiles

Satellite Observations of Surface Fronts, Currents and Winds in the Northeast South China Sea

Contract No. N C0123

Generation and Propagation of Internal Solitary Waves on the Continental Shelf and Slope

System Reliability Simulation and Optimization by Component Reliability Allocation

Report Documentation Page

Attribution Concepts for Sub-meter Resolution Ground Physics Models

Improvement of Mesoscale Numerical Weather Prediction For Coastal Regions of Complex Terrain FY2003

SENSORS FOR MEASURING THE VOLUME SCATTERING FUNCTION OF OCEANIC WATERS

Grant Number: N IP

Award Number N

Sediment Dispersal from the Apennine Rivers

Report Documentation Page

Estimation of Vertical Distributions of Water Vapor from Spaceborne Observations of Scattered Sunlight

Assimilation of Synthetic-Aperture Radar Data into Navy Wave Prediction Models

Award # N LONG TERM GOALS

Coastal Engineering Technical Note

Statistical Prediction of Ocean Circulation and Trajectories

DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited.

Direct Numerical Simulation of Aeolian Tones

Analysis of Infrared Measurements of Microbreaking and Whitecaps

Nonlinear Internal Tide Generation at the Luzon Strait: Integrating Laboratory Data with Numerics and Observation

P. Kestener and A. Arneodo. Laboratoire de Physique Ecole Normale Supérieure de Lyon 46, allée d Italie Lyon cedex 07, FRANCE

Rogue Wave Statistics and Dynamics Using Large-Scale Direct Simulations

Estimation of Vertical Distributions of Water Vapor and Aerosols from Spaceborne Observations of Scattered Sunlight

Curating and Maintenance of the Sediment Library and Dredge Collection

DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited.

REGENERATION OF SPENT ADSORBENTS USING ADVANCED OXIDATION (PREPRINT)

DIRECTIONAL WAVE SPECTRA USING NORMAL SPREADING FUNCTION

Crowd Behavior Modeling in COMBAT XXI

Analysis Comparison between CFD and FEA of an Idealized Concept V- Hull Floor Configuration in Two Dimensions. Dr. Bijan Khatib-Shahidi & Rob E.

HYCOM Caspian Sea Modeling. Part I: An Overview of the Model and Coastal Upwelling. Naval Research Laboratory, Stennis Space Center, USA

CRS Report for Congress

Characterization of Caribbean Meso-Scale Eddies

DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Lateral Mixing

Upper Ocean Measurements of Water Masses and Circulation in the Japan Sea

The Mechanics of Bubble Growth and Rise in Sediments

Detection of Submerged Sound Sources

Inferring Atmospheric Turbulence Structure Using Synthetic Aperture Radar Images Of The Ocean Surface

A report (dated September 20, 2011) on. scientific research carried out under Grant: FA

NAVGEM Platform Support

Evolution of Tropical Cyclone Characteristics

Comparative Analysis of Flood Routing Methods

Transcription:

Modeling the Impact of Extreme Events on Margin Sedimentation Jasim Imran Department of Civil and Environmental Engineering, University of South Carolina, 3 Main Street, Columbia, SC 2928. phone: (83) 777-121 fax: (83) 777-67 email: imran@engr.sc.edu Award Number: N14-4-1-168 LONG-TERM GOALS To understand the mechanics of hyperpycnal flow generated from the plunging of small and medium size rivers and how these extreme events affect the transport of terrestrial sediment and how they influence the mixing processes in the coastal ocean. OBJECTIVES To develop a two dimensional vertical structure finite volume model of density and turbidity current To verify this model against available experimental data. To apply the model at the field scale to study the affect of stratification on a plunging density current. To study the generation of internal wave by the passage of a hyperpycnal flow (turbidity current). APPROACH A two-dimensional vertical structure model has been developed. This model solves the Reynoldsaveraged Navier-Stokes (RANS) equations along with species mass conservation equations for nonorthogonal structured grid in order to obtain flow variables that are non-uniform over depth. Closure for the turbulence stress terms is obtained by using the buoyancy modified k-ε model. The governing equations are discretized using an implicit finite volume scheme for non-orthogonal grid system. In this method, non-orthogonality has been addressed in the process of approximating the convective and diffusive flux through the cell face without transforming the grid to an orthogonal curvilinear coordinate. Collocated arrangement of the variables has been used for the present grid system. For the approximation of the convective and diffusive terms in the governing equations, we used differed correction approach which is a blend of lower order scheme (e.g., first order upwind scheme, UDS) with higher order scheme (e.g., second order central difference scheme, CDS). An implicit three-time level second order scheme is used for time integration. Strongly Implicit Procedure (SIP) has been used in order to solve the discretized governing equations by iteration. The pressure correction equation developed from mass conservation equation is solved using the PISO (Pressure Implicit with Splitting of Operators) algorithm. The present model allows specification of different types of boundary conditions depending on the nature of the flow. At the inlet boundary, distribution of all 1

Report Documentation Page Form Approved OMB No. 74-188 Public reporting burden for the collection of information is estimated to average 1 hour per response, including the time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing the collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite 124, Arlington VA 2222-432. Respondents should be aware that notwithstanding any other provision of law, no person shall be subject to a penalty for failing to comply with a collection of information if it does not display a currently valid OMB control number. 1. REPORT DATE 3 SEP 24 2. REPORT TYPE 3. DATES COVERED --24 to --24 4. TITLE AND SUBTITLE Modeling the Impact of Extreme Events on Margin Sedimentation 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) 5d. PROJECT NUMBER 5e. TASK NUMBER 5f. WORK UNIT NUMBER 7. PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES) Department of Civil and Environmental Engineering,,University of South Carolina,3 Main Street,,Columbia,,SC,2928 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 1. SPONSOR/MONITOR S ACRONYM(S) 12. DISTRIBUTION/AVAILABILITY STATEMENT Approved for public release; distribution unlimited 13. SUPPLEMENTARY NOTES 14. ABSTRACT 11. SPONSOR/MONITOR S REPORT NUMBER(S) 15. SUBJECT TERMS 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT a. REPORT unclassified b. ABSTRACT unclassified c. THIS PAGE unclassified Same as Report (SAR) 18. NUMBER OF PAGES 6 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

dependent variables should have to be prescribed. At the outflow boundary, normal gradients of all dependent variables are set to zero, i.e., variables at this boundary are extrapolated from the interior domain. Open surfaces are treated as symmetry boundary condition where zero convective and diffusive flux is considered across this surface. At high Reynolds number flow, the viscous sub-layer near a solid boundary is so thin that it is difficult to use enough grid points to resolve it. Therefore, at the solid boundary, velocity profile is set using the wall functions approach. The work has been primarily carried out by a doctoral student Sadia M. Khan and it contributes to her dissertation. WORK COMPLETED A 2-D vertical structure finite volume model of density driven flow has been developed. The model utilizes the buoyancy modified k-ε model for turbulence closure. A non-orthogonal grid system has been used in the model that can handle a wide variety of boundary conditions. The model has been verified against two sets of experiments on the generation of internal waves by the passage of a gravity current in a stratified flow. In one, the current is released over a ramp and in the other, the current is released on a horizontal bed. In both cases, the model captures the generation of internal waves and other aspects of the flow and matches the experimental results satisfactorily. The model has been applied at a larger scale to study the interaction between a plunging density flow and a stratified environment. It has been found that the passage of a hyperpycnal flow generates a solitary wave with its maximum amplitude occurring above the head of the current. We will continue our numerical experiment by considering stratification data obtained from the field by researchers involved in the STRATAFORM and EuroSTRATAFORM Projects. RESULTS The model has been verified by comparing the model prediction with experimental results. For this purpose, we have considered two sets of experiments carried out by Maxworthy et al. (22) and Monaghan et al. (1999). In the first experimental setup, internal waves have been generated by density current in a tank with horizontal bottom (Maxworthy et al. 22). They have run several experiments for sub- and super-critical flow conditions where heavy fluid was released from behind the lock gate to the lower boundary of the tank containing linearly stratified ambient fluid. The second set of experiments carried out by Monaghan et al. (1999) generated internal solitary wave when density current was descending down a ramp into a two-fluid system. We have run our model using these two experimental setups and found that model predictions are in good agreement with the experimental results. Figure 1 shows the comparison of some of the model result with the experimental results of Maxworthy et al. (22). After validation of the model, we applied it to study the generation of internal waves due to plunging of a river. We considered a 1 m long domain with Steep bottom slope of 3 o. Boundary conditions used in this case can be summarized as follows: at inflow boundary (1.3 meter of depth), it is considered that a river is continuously discharging heavy density water (density around 145 kg / m 3 ) with a constant velocity of 1.625 m/s. For initial stratification, linear density profile is considered for the ambient ocean water, i.e., we assumed constant density of 126 kg/m 3 at the top surface and it will 2

linearly increase with depth. Figure 2 shows the time sequence of the evolution of density current into a linearly stratified medium due to plunging of river. It is observed from the results that a large amplitude solitary wave develops above the head of the density current. After plunging into ocean, the density current has created disturbance in the stable ambient ocean stratification. Figure 3 shows the intense mixing occurring in the water column just at the location of the current head after 8 seconds. The detailed results will be published in a peer reviewed journal. A manuscript is currently under preparation. IMPACT/APPLICATIONS The development of the numerical model of density current provides an opportunity to study the impact of density driven flow on the generation of internal waves. Internal waves are common oceanographic phenomenon which results from disturbances created into stable ocean stratification. These waves can lead to vigorous turbulence and mixing in the water column. Internal waves can also significantly affect the acoustics. Recently, researchers have been paying attention to the density currents as a potential force for generating internal waves. Density currents can be generated by retrogressive slope failure, storm, or due to the plunging of a river. The non-depth-averaged model developed here allows us to study whether a density current can generate an internal wave and how the passage of the density current affects the stability of a stratified environment. TRANSITIONS We consider that the development of a vertical structure model of density driven flow is an important progress towards understanding the complex interaction of plunging river flow, stratified environment of the ocean, and the bottom boundary. We plan to incorporate an erodible bottom boundary to the model. We also plan to study the convective sedimentation process using this model. Experimental data from the work of Jeff Parsons will be useful for this purpose. The model can also be incorporated in the 3-D Sedflux model of James Syvitski. RELATED PROJECTS This project is closely related to an NSF funded project CAREER: Experimental and Numerical Modeling of Flow and Morphology Associated with Meandering Submarine Channels and an industry funded project 3-D Numerical modeling of turbidity current. The model will be further verified and applied at the field scale using stratification data obtained by field researchers involved in the EuroSTRATAFORM Project. REFERENCES Maxworthy, T., Leilich, J., Simpson, J. E., Meiburg, E. H. (22). The propagation of a gravity current into a linearly stratified medium. J. Fluid Mech., 453, 371-394. Monaghan, J. J., Cas, R. A. F., Kos, A. M., Hallworth, M. (1999). Gravity current descending a ramp in a stratified tank, J. Fluid Mech., 379, 39-69. 3

(a) (b) (c) (d).75 1.35 1.95 Model Prediction.6 1.2 1.8.45 DENS: 112 123 133 143 153 163 173 183 1.5 1.65.3.9 DENS: 112 123 133 143 153 163 173 183 (kg / m 3 ) 1.5 (kg / m 3 ).15.75 1.35 2.1 1.95.6 1.2.4.8 1.2 1.6 2 2.4.45 1.5 1.8 1.65.3.9 (kg / m 3 ) DENS: 112 123 133 143 153 163 173 183.15.75 1.5 1.35.6 1.2.4.8 1.2 1.6 2 2.4.45 1.5.3.9 (kg / m 3 ) DENS: 112 123 133 143 153 163 173 183.15.75.6.4.8 1.2 1.6 2 2.4.45.3.15.4.8 1.2 1.6 2 2.4 Experimental Results Figure 1. Comparison of the model prediction with experimental results. Left: simulation; Right: photographs from experiment of Maxworthy et al. (22). Time sequences are (a) 4s; (b) 6s; (c) 1s and (d) 12s after opening the gate. 4

(a) Time = 16 sec 6 4 2 1 2 3 4 5 6 7 8 9 1 (b) 6 Time = 48 sec 4 2 1 2 3 4 5 6 7 8 9 1 (c) Time = 8 sec 6 4 2 1 2 3 4 5 6 7 8 9 1 Distance in stream-wise direction (m) Figure 2. Time sequence of the generation of internal solitary waves due to the plunging of a density current in a linearly stratified medium. 6 Reference vector 1. m/s 4 127.24 128.47 127.24 129.69 13.71 132.15 128.47 133.46 129.69 2 134.61 13.71 4 5 6 7 Distance in stream-wise direction (m) Figure 3. Intense mixing occurs near the head of the current shown in Figure 2. 5