MODEL RESPONSE SENSITIVITY TO WAVES, NONLINEAR ADVECTION, AND BOTTOM FRICTION Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, 2013 1 Patrick Corbitt.

Slides:



Advertisements
Similar presentations
INWAVE: THE INFRAGRAVITY WAVE DRIVER OF THE COAWST SYSTEM
Advertisements

Section 2: The Planetary Boundary Layer
Modeling to Revise Coastal Inundation and Flooding Estimates in Georgia and Northeast Florida Association of State Flood Plain Managers Conference May.
The Quasi-Geostrophic Omega Equation (without friction and diabatic terms) We will now develop the Trenberth (1978)* modification to the QG Omega equation.
Tropical Cyclones Chapter 11 Meteorology 1010 Professor Bunds Utah Valley University.
CHAPTER 5: PREDICTING STORM SURGE LESSONS FROM HURRICANE IKE.
Circulation in the atmosphere
Ocean & Atmospheric circulation redux 1) Unequal planetary heating creates pressure gradients which make winds blow on ocean surface in trade-wind & westerly.
D A C B z = 20m z=4m Homework Problem A cylindrical vessel of height H = 20 m is filled with water of density to a height of 4m. What is the pressure at:
General Circulation and Climate Zones Martin Visbeck DEES, Lamont-Doherty Earth Observatory
STORM SURGE. Composed of several attributes: A)Barometric – Coastal water response to low pressure at center of storm B) Wind stress – frictional drag.
AOSS 321, Winter 2009 Earth System Dynamics Lecture 9 2/5/2009 Christiane Jablonowski Eric Hetland
ATMOSPHERIC CIRCULATION. Atmospheric and Oceanic Circulation Wind Essentials Driving Forces Within the Atmosphere Atmospheric Patterns of Motion Oceanic.
The Ocean General Circulation (satellite). Mean Circulation in the Ocean Gulf Stream.
Institute of Oceanogphy Gdańsk University Jan Jędrasik The Hydrodynamic Model of the Southern Baltic Sea.
The General Circulation of the Atmosphere Background and Theory.
1 Weather and Climate Bay Area Earth Science Institute (BAESI) Pressure San Jose State University, January 24, 2004
An Assimilating Tidal Model for the Bering Sea Mike Foreman, Josef Cherniawsky, Patrick Cummins Institute of Ocean Sciences, Sidney BC, Canada Outline:
Things to look for on the weather maps Visible and IR satellite images (& radar too): Look at cloud movements and locations - do they correlate with what.
19 December ConclusionsResultsMethodologyBackground Chip HelmsSensitivity of CM1 to Initial θ' Magnitude and Radius Examining the Sensitivity of.
What may have happened here had Hurricane Ivan visited us instead of Pensacola? R.H. Weisberg and L. Zheng College of Marine Science University of South.
IOOS/SURA Extratropical Storm Inundation Testbed: Preliminary Results for Scituate, Massachusetts Changsheng Chen, Qichun Xu, Jianhua Qi and Huichan Lin.
Test of improved boundaries configuration for the Tagus Estuary Pre-operational Model (OM) Ângela Canas Maretec SANEST.
OCEN 201 Introduction to Ocean & Coastal Engineering Ocean Environment &Waves Jun Zhang
USF FVCOM Tropical Cyclone Inundation Testbed Progress by Robert H. Weisberg, Lianyuan Zheng and Yong Huang College of Marine Science University of South.
The troposphere, except in shallow, narrow, rare locations, is stable to dry processes. For the purpose of synoptic analysis, these areas can be ignored.
Momentum Equations in a Fluid (PD) Pressure difference (Co) Coriolis Force (Fr) Friction Total Force acting on a body = mass times its acceleration (W)
Modeling the upper ocean response to Hurricane Igor Zhimin Ma 1, Guoqi Han 2, Brad deYoung 1 1 Memorial University 2 Fisheries and Oceans Canada.
 Hurricanes are areas of low air pressure that form over oceans in tropical climate regions.  Hurricanes hit land with tremendous force, bringing.
CLOSED ENERGY BUDGETS FOR REGIONAL NUMERICAL SIMULATIONS Parker MacCready University of Washington.
For a rotating solid object, the vorticity is two times of its angular velocity Vorticity In physical oceanography, we deal mostly with the vertical component.
FLUID ROTATION Circulation and Vorticity. Arbitrary blob of fluid rotating in a horizontal plane Circulation: A measure of the rotation within a finite.
For a rotating solid object, the vorticity is two times of its angular velocity Vorticity In physical oceanography, we deal mostly with the vertical component.
Ocean Currents Ocean Density. Energy in = energy out Half of solar radiation reaches Earth The atmosphere is transparent to shortwave but absorbs longwave.
The Ocean General Circulation. Mean Circulation in the Ocean Gulf Stream.
© 2011 Pearson Education, Inc. CHAPTER 6 Air-Sea Interaction.
Typical Mean Dynamic Balances in Estuaries Along-Estuary Component 1. Barotropic pressure gradient vs. friction Steady state, linear motion, no rotation,
MODEL RESPONSE SENSITIVITY TO WAVES, NONLINEAR ADVECTION, AND BOTTOM FRICTION Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Patrick Corbitt.
CEE 262A H YDRODYNAMICS Lecture 13 Wind-driven flow in a lake.
Modelling 2: Introduction to modelling assignment. A basic physical-biological model. Model equations. Model operation. The assignment.
Conservation of Salt: Conservation of Heat: Equation of State: Conservation of Mass or Continuity: Equations that allow a quantitative look at the OCEAN.
Physical Conditions 9/16-9/ including Hurricane Isabel inches Hg ft (MLLW) knots inches Atmospheric Pressure.
Naeko Takahashi Qing Wang Scott C. Hagen, Ph.D., P.E. Astronomic Tides, Flows and Hurricane Storm Surge Modeling of the Pascagoula River, MS March 4, 2009.
Atmospheric Circulation. The Earth’s energy is partly redistributed by atmospheric circulation. 1.Factors in the Cirulation of Air include; Pressure Gradient.
Tropical Report: Modeling Hurricane Ike with SLOSH Don Slinn, Jeff Ren, Go Fujita Univ of Florida Coastal Engineering.
Circulation in the atmosphere Circulation in the Atmosphere.
Wind-driven circulation II ●Wind pattern and oceanic gyres ●Sverdrup Relation ●Vorticity Equation.
Circulation in the atmosphere Lecture 06 Circulation in the Atmosphere.
The Atmospheric Response to Changes in Tropical Sea Surface Temperatures An overview of Gill, A.E., 1980, Some simple solutions for heat- induced tropical.
1. The geostrophic wind: scale analysis 2. Effects of friction 3. The gradient wind ATOC 4720 class33.
Free Surface Hydrodynamics 2DH and 3D Shallow Water Equations Prof. Dano Roelvink.
Typical Mean Dynamic Balances in Estuaries Along-Estuary Component 1. Barotropic pressure gradient vs. friction Steady state, linear motion, no rotation,
ATS/ESS 452: Synoptic Meteorology Wednesday 09/10/2014 Quiz! (Short?) Weather Discussion Continue Review Material Geostrophic Wind Continuity Vorticity.
Class Meeting Nov. 26, 2:00pm-4:45pm
Assume geostrophic balance on -plane approximation, i.e.,
Importance of high-resolution modeling for storm surge, hurricane waves, coastal water levels, and currents in Puerto Rico and the U.S. Virgin Islands.
Coupled atmosphere-ocean simulation on hurricane forecast
Damped Inertial oscillations
ATS/ESS 452: Synoptic Meteorology
5th Workshop on "SMART Cable Systems: Latest Developments and Designing the Wet Demonstrator Project" (Dubai, UAE, April 2016) Contribution of.
ATOC 4720 class32 1. Forces 2. The horizontal equation of motion.
ATOC 4720 class37 1. The vertically averaged divergence
Ocean Currents.
Classes of Tornadoes… Main Types of Tornadoes
Combination of oceanographic data with wind data acquired during the cruise to try to draw conclusions on wind stress, Ekman transport and Ekman layer.
Coastal Erosion Workshop
ATOC 4720: class 43: Final review (continue)
Eutrophication indicators PSA & EUTRISK
Hurricane Created by Alana Luke Velasquez
Ocean Currents.
Presentation transcript:

MODEL RESPONSE SENSITIVITY TO WAVES, NONLINEAR ADVECTION, AND BOTTOM FRICTION Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Patrick Corbitt Kerr, P.E. University of Notre Dame

Part I Wave Bottom Friction Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, If circulation models are sensitive to bottom friction on the Louisiana-Texas shelf, what is the sensitivity of wave models to bottom friction formulation in that region?

Wave Bottom Friction Friction Formulations 3 Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Variable Bottom Material JONSWAP Formulation Bottom Friction in SWAN Recommend by Literature Muddy Bottom? Madsen Formulation Based on Manning’s n

A CB

D GE

H JI

Wave Bottom Friction Summary of Findings 7 Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Model Response Sensitivity to Wave Bottom Friction Formulation – Madsen and JONSWAP formulations are both adequate – The JONSWAP friction coefficient is sensitive to bottom type, therefore a C jfon =0.019m 2 s -3 should be used for the muddy LATEX shelf.

Part II Component Contributions Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, What is the spatial and temporal contributions of wave radiation stress and non-linear advection terms in a hurricane storm surge model and how do these processes compare with the other components of the shallow water equations?

Contribution of Non-Linear Advection OVERALL TEMPORAL

Contribution of Wave Radiation Stress OVERALL TEMPORAL

Component Contributions Scaling Ike at 5 Locations 11 Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Local Non-Linear Advection Coriolis Surface Gradient Atmospheric Pressure Tidal Potential Gradient Wind Stress Wave Radiation Stress Gradient Bottom Friction Diffusion (Momentum) Terms

LOCATION 1 Significant Terms: Pressure Surface Local Coriolis

LOCATION 2 Major Terms: Local Coriolis Pressure Surface Moderate Terms: Advection Wind

LOCATION 3 Significant Terms: Surface Wind Bottom Coriolis Local Advection

LOCATION 4 Significant Terms: Surface Wind Advection Wave Bottom Coriolis

LOCATION 5 Significant Terms: Bottom Surface Wind

Component Contributions Summary of Findings 17 Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30, Galveston, TX Component Contributions for Hurricane Ike (2008) – Non-linear advection captures 10-20cm of geostrophic setup and increases resonant waves by 30-40cm. – Wave radiation stress adds cm to maximum water levels and is responsible for an earlier rise in water levels. – Bottom Friction and Coriolis were significant components in the development of Ike’s Forerunner.

QUESTIONS 18 Patrick C. Kerr 17 th ADCIRC WORKSHOP April 29-30,