Validation and Verification of Moving Boundary Models of Land Building Processes Vaughan R. Voller National Center for Earth-surface Dynamics Civil Engineering,

Slides:



Advertisements
Similar presentations
Guided Notes on Erosion and Deposition
Advertisements

Chapter 9 Water Erosion and Deposition
1 Characterizing the Impact of Horizontal Heat Transfer on the Linear Relation of Heat Flow and Heat Production Ronald G. Resmini Department of Geography.
Sediment Movement after Dam Removal
Deposition.
Effect of Subsidence Styles and Fractional Diffusion Exponents on Depositional Fluvial Profiles Vaughan Voller: NCED, Civil Engineering, University of.
Application of the Enthalpy Method: From Crystal Growth to Sedimentary Basins Grain Growth in Metal Solidification From W.J. Boettinger  m  10km “growth”
Moving Boundaries in Earthscapes Damien T. Kawakami, V.R. Voller, C. Paola, G. Parker, J. B. Swenson NSF-STC
National Center for Earth-surface Dynamics Modeling physical and ecological dynamics of channel systems that shape Earth’s surface Moving boundary problems.
National Center for Earth-surface Dynamics Modeling physical and ecological dynamics of channel systems that shape Earth’s surface Moving boundary problems.
Mathematical Models of Sediment Transport Systems
An attempt to provide a physical interpretation of fractional transport in heterogeneous domains Vaughan Voller Department of Civil Engineering and NCED.
Voller, University of Minnesota Application of an Enthalpy Method for Dendritic Solidification Vaughan R. Voller and N. Murfield.
An Enthalpy—Level-set Method Vaughan R Voller, University of Minnesota + + speed def. Single Domain Enthalpy (1947) Heat source A Problem of Interest—
The Marssim Model The skeleton is a pretty generic landform evolution model: – Weathering – Non-linear diffusive creep – Bedrock channels erosion by any.
1D SEDIMENT TRANSPORT MORPHODYNAMICS with applications to RIVERS AND TURBIDITY CURRENTS © Gary Parker November, CHAPTER 24: APPROXIMATE FORMULATION.
Can a fractional derivative diffusion equation model Laboratory scale fluvial transport Vaughan Voller * and Chris Paola Confusion on the incline * Responsible.
National Center for Earth-surface Dynamics an NSF Science and Technology Center MOVING BOUNDARY PROBLEMS ON THE EARTHS SURFACE V.R. Voller+,
Session III: Computational Modelling of Solidification Processing Analytical Models of Solidification Phenomena V. Voller QUESTION: As models of solidification.
Non-local Transport in Channel Networks Vaughan Voller Civil Engineering University of Minnesota Tetsuji Muto, Wonsuck Kim, Gary Parker, John Swenson,
An Enthalpy Based Scheme for Simulating Dendritic Growth V.R. Voller 4d o (blue) 3.25d o (black) 2.5d o (red) Dendrite shape with 3 grid sizes shows reasonable.
James P.M. Syvitski Environmental Computation and Imaging Facility INSTAAR, CU-Boulder Earth-surface Dynamics Modeling & Model Coupling.
GROWING NUMERICAL CRYSTALS Vaughan Voller, and Man Liang, University of Minnesota We revisit an analytical solution in Carslaw and Jaeger for the solidification.
Sculpting Earth’s Surface
1D SEDIMENT TRANSPORT MORPHODYNAMICS with applications to RIVERS AND TURBIDITY CURRENTS © Gary Parker November, CHAPTER 15: EXTENSION OF 1D MODEL.
An example moving boundary problem Dry porous media Saturated porous media x = 0 x = s(t) h(0) = L Fixed Head If water head remains at fixed value L at.
Moving Boundary Problems are Us The development and application of numerical methods for transport models towards an integrated frame-work for modeling.
Fresh Water Systems Parkside Junior High 2010/11 Mrs. Doig-Gray and Mrs. Friesen.
Erosion and Deposition
Surface Water Chapter 9.
Response of river systems to tectonic deformation Chris Paola* St Anthony Falls Lab University of Minnesota * On behalf of the experimental stratigraphy.
Streams and Drainage Systems The most important source of moving water.
Ch.13, Sec.2 – Stream Erosion & Deposition
LL-III physics-based distributed hydrologic model in Blue River Basin and Baron Fork Basin Li Lan (State Key Laboratory of Water Resources and Hydropower.
A MULTI-SCALE/MULTI-PHYSICS MODELING FRAMEWORK FOR SOLIDIFICATION SYSTEMS Vaughan R Voller Saint Anthony Falls Lab University of Minnesota Acknowledgments.
RIVER RESPONSE TO POST-GLACIAL SEA LEVEL RISE: THE FLY-STRICKLAND RIVER SYSTEM, PAPUA NEW GUINEA Gary Parker, Tetsuji Muto, Yoshihisa Akamatsu, Bill Dietrich,
1 LECTURE 12 MORPHODYNAMICS OF 1D SUBMARINE/SUBLACUSTRINE FANS CEE 598, GEOL 593 TURBIDITY CURRENTS: MORPHODYNAMICS AND DEPOSITS As the Colorado River.
Materials Process Design and Control Laboratory MULTISCALE MODELING OF ALLOY SOLIDIFICATION LIJIAN TAN NICHOLAS ZABARAS Date: 24 July 2007 Sibley School.
Hinterlands sea alluvial plain alluvial river bedrock river QUESTION: What is the role of relative sea level in controlling alluvial aggradation and degradation?
An Enthalpy Model for Dendrite Growth Vaughan Voller University of Minnesota.
1 MODELING OF LAND BUILDING IN THE MISSISSIPPI DELTA: A TEMPLATE FOR RECONSTRUCTION Wonsuck Kim & Gary Parker, University of Illinois As part of a much.
Stream Erosion and Transport
Landforms E.8.C.5 Students know how geologic processes account for state and regional topography. E/S (DOK 2) What are Landforms? Cornell Notes in your.
MA354 An Introduction to Math Models (more or less corresponding to 1.0 in your book)
National Center for Earth-surface Dynamics an NSF Science and Technology Center V.R. Voller+, J. B. Swenson*, W. Kim+ and C. Paola+ +
13.2 Stream Erosion and Deposition
AIM: What are the parts of a stream/river?
Geographic Features.
As you know from Chapter 2, weathering is the breakdown of rocks into smaller pieces. So what is erosion? Erosion is the movement of the broken or weathered.
Transpiration Similar to evaporation, this is the loss of water through plants. – Pores in leaves (stomata) are opened to release oxygen and water vapor.
Environmental Hydrodynamics Lab. Yonsei University, KOREA RCEM D finite element modeling of bed elevation change in a curved channel S.-U. Choi,
By, Janet Hooks RIVERS & STREAMS. The bumpiness or flatness of the land is called TOPOGRAPHY. The topography of the land determines how fast water will.
National Center for Earth-surface Dynamics ENABLING LANDSCAPE SUSTAINABILITY The Mississippi Delta Gary Parker, University of Illinois From NASA.
Boundary layer models of Martian hydrothermal systems Kate Craft 11/2/2007.
SALT WATER INTRUSION By, Steffi Roy PR11CE2005 Water Institute
A Mesh-less method for solutions of the Stefan Problem
Direction and Non Linearity in Non-local Diffusion Transport Models
Jeopardy Vocab Water Glaciers and Wind Waves and Mass Wasting Misc.
Freshwater Systems less than 1% of the water on Earth is available for us as freshwater freshwater exists as surface water groundwater.
Chapter 9 Water Erosion and Deposition
What is the future of applied mathematics? Chris Budd.
You have learned how to interpret how landforms are the result of a combination of constructive and destructive forces such as deposition of sediment and.
Chapter 18.
Water Cycle, Groundwater, Aquifers, Caves
1ST YEAR OF ESO RIVERS PROFESOR TIERNO GALVÁN SECONDARY SCHOOL.
Clipper Cutters Nebraska Date:? Pg:?
The Flow of Freshwater.
Streams and Drainage Systems
Modeling Phase Changes in Finite Element Analysis
You have learned how to interpret how landforms are the result of a combination of constructive and destructive forces such as deposition of sediment and.
Presentation transcript:

Validation and Verification of Moving Boundary Models of Land Building Processes Vaughan R. Voller National Center for Earth-surface Dynamics Civil Engineering, University of Minnesota Wax LakeSolid Crystal Growing in undercooled melt Tetsuji Muto, Wonsuck Kim, Chris Paola, Gary Parker, John Swenson, Jorge Lorenzo Trueba, Man Liang

Fans Toes Shoreline MovinG Boundaries in the Landscape

1km Examples Badwater Deathvalley Sediment Fans Sediment Delta

sediment h(x,t) x = u(t) bed-rock ocean x shoreline x = s(t) land surface  

An Ocean Basin The Swenson Analogy: Melting vs. Shoreline movement Swenson et al, Eur J App Math, 2000

Physical Process Isolate Key Phenomena Experiment Phenomenological Assumptions Model Approximation Assumptions Numerical Solution Validation: If assumptions for Analytical solution are consistent with Physical assumptions In experiment Can VALIDATE phenomenological assumptions Verification: Comparison of numerical and analytical predictions VERIFY Numerical Approach The Modeling Paradigm Limit Case Assumptions Analytical Solution

CASE OF CONSTANT BASE LEVEL and Bed Rock The delta progrades into standing water. The rate of progradation slows in time as deeper water is invaded. The bedrock-alluvial transition migrates upstream. Slide from MUTO and PARKER---Muto Experiments

Experiments and image analysis by Tetsuji Muto and Wonsuck Kim, In slot flume

q0q0 h A mathematical model based on the Swenson Stefan Analogy with Fixed base slope and sea level Note 4 conditions 2 for the 2 nd order equations 2 for the 2 moving boundaries

Similarity Solution

q0q0 h To develop numerical solution write problem in terms of Total Sediment Balance (enthalpy). Then there is NO need to treat shoreline conditions making for an easier numerical solution “Latent Heat” Amount of sediment that needs to be provided To move shoreline a unit distance (L = 0 in sub-aerial) Numerical Solution

q k=k-1 k-1 k i-1i i+1 ONLAP CONDITION h q q On-lap update—if Update on-lap node flag 1<L<0

Physical Process Isolate Key Phenomena Experiment Phenomenological Assumptions Model Approximation Assumptions Numerical Solution Validation: If assumptions for Analytical solution are consistent with Physical assumptions In experiment Can VALIDATE phenomenological assumptions The Modeling Paradigm Limit Case Assumptions Analytical Solution

seawardlandward Experiments Analytical Solution Get Fit by choosing diffusivity Bed porosity fixed at 30% Experiment vs. Analytical: VALIDATION Two Consistency Checks 1. Compare physical and Predicted surfaces A little more concaved than we would like (experiment may be better modeled by Non-linear diffusion) 2. Across a range of experiments best fit diffusivity should scale with water discharge Reasonable

Physical Process Isolate Key Phenomena Experiment Phenomenological Assumptions Model Approximation Assumptions Numerical Solution The Modeling Paradigm Limit Case Assumptions Analytical Solution Verification: Comparison of numerical and analytical predictions VERIFY Numerical Approach

NUMERICAL VS. ANALYTICAL: Verification

An Interesting Limit Case q0q0 No- on-lap A horizontal fluvial surface coinciding with sea level

In a Two-Dimensional plan view this limit case gets a little more interesting

Current: Towards a CAFÉ Delta Model (Voller, Paola, Man-Ling) The simulation shows a “particle” solution of the filling model. This is based on the introduction, probabilistic movement, and deposition of particles in the domain. IT can be shown that this is a solution of the discrete equations associated with a Finite Element Model of the governing equations. Cellular RULES can be introduced by linking the probability of particle movement to the path taken. Thereby modeling channels and vegetation. Can make physical arguments that a suitable Background model is the filling of a thin-cavity (Hele-Shaw cell) CAFÉ—Background deterministic (PDE) model solved with Finite Elements Superimposed with a Cellular (rule based Model)

Some Examples Uniform Probs High Middle Prob High Edge Efi Research Question: How is CADFE model based on a “normal” PDE Related to a “fractional derivative PDE”

Saltwater intrusion occurs when saltwater from the Gulf moves into areas that have formerly been influenced by freshwater. As saltwater intrudes into a fresh marsh, the habitat will be altered as the plants and organisms that once thrived in the freshwater marsh cannot survive in saltwater. If the intrusion of saltwater is gradual enough, plants and organisms that can survive in a saltwater habitat begin to invade and grow, eventually establishing a brackish marsh. If saltwater vegetation does not replace the freshwater plants, the area will become exposed mud flats, and they are likely to revert to open water. This process is common in an abandoned delta lobe where the discharge of the river decreases or even in areas of the modern delta where freshwater is diverted or maintained within existing channels.