Downscaling and Parameterization. by Jun-Ichi Yano
|
|
- Cordelia Russell
- 5 years ago
- Views:
Transcription
1 Downscaling and Parameterization by Jun-Ichi Yano
2 main references: J.-I. Yano, J.-L. Redelsperger, F. Guichard, and P. Bechtold, 2005: Mode Decomposition As a Methodology For Developing Convective-Scale Representations in Global Models. Quator. J. Roy. Meteor. Soc., 131, J.-I. Yano, 2010, Downscaling, Parameterization, Decomposition, Compression: A Perspective from the Multiresolutional Analysis. Adv. Geophy., 23,
3 Focus: Convective Precipitating Systems Key Words: Subgrid-Scale Representation Downscaling, Parameterization Probability (Bayesian) Data Assimilation Mass Flux NAM-SCA
4 Focus: Convective Precipitating Systems Key Word: Subgrid-Scale Representation
5 Focus: Convective Precipitating Systems Key Word: Subgrid-Scale Representation
6 Subgrid-Scale Representation Subgrid-Scale? Model Resolution Explicit Horizontal Scale
7 Downscaling: Subgrid-scale space-time details (e.g., Rainfall Distribution) Parameterization: Feedbacks of subgrid-scale processes to the resolved scales (e.g., Condensative Heating Rate)
8
9 Subgrid-Scale Physical Representation: full physical system: average over the grid-box =Q parameterization? =?: Downscaling
10 Downscaling Global Model Subgrid-Scale Processes Parameterization (e.g., Rainfall)?
11
12
13
14 Questions: Why the current downscaling and parameterization don t mutually work as inverse operations? How to construct the downscaling and parameterization together consistently?: Representation Problem
15 Example of subgrid-scale physical processes: Atmospheric Convection: Full System? (CRM) Representation
16 How to construct a subgrid-scale representation consistently? 1. Identify the Basic Elements for subridscale processes (e.g., plume) 2. Mode Decomposition (efficient representation): Mode=Basic physical elements 3. Compression (mode truncation): Parameterization 4. Decompression (inversion to the physical space): Downscaling
17 Mode Decomposition : Mode Decomposition: where χ l (x,y) :modes (l = 1,.N) :expansion coefficients e.g., Fourier Mass-Fluxes (convection) Basins (hydrology) Wavelets (multiresolutional analysis)
18 Subgrid-Scale Representation Problem: Downscaling Compression parameterization Physical Space Decompression? Compressed Space (e.g., MassFlux)
19 NB: Basic Set of Modes must be chosen so that it fits well to the geometrical structures of the subgrid-scale processes
20 What should be Represented?: ~200km cumulus convection (convective towers) ~20km stratiform clouds (mesoscale) Ensemble of «Plumes»
21 Ensemble of «Plumes»: Spatially-localized features of various different scales (e.g., convective updrafts, downdrafts, mesoscale organizations) A Particular Mode Decomposition Approach: Multiresolutional Analysis e.g., Wavelet
22
23
24 Limit of the Wavelet Approach: Difficulty of Efficient Real (physical) Space Manipulation: Plume (MassFlux) Decomposition
25 Single Plume (MassFlux) Mode : Segmentally-Constant Approximation (SCA) w c, θ c,.ϕ c w e, θ e,.ϕ e x Convective Plume Environment
26 Plumes: Segmentally-Constant Approximation (SCA) Temperature Anomaly (K)
27 NAM-SCA NAM:Nonhydrostatic Anelastic Model
28 Plumes: Segmentally-Constant Approximation (SCA) Temperature Anomaly (K)
29 Updraft + Downdraft: A simple demonstration Without environment Hypothesis with NAM-SCA: w(m/s) θ(k)
30 Truncated NAM-SCA: More Physical Processes:
31 Truncated NAM-SCA: W (m/s) θ (K) qv (g/kg) qc (g/kg) qp (g/kg)
32 Final SCA-Archtype Model? 2D 4-segment model: Axisymmetric 3-segment model:
33 Numerical Archetype: Fixed Distribution of Finite-Volume Elements Cloud Water (g/kg)
34 Tropical Squall-line (GATE Phase III) W (m/s) θ (K) qv (g/kg) qc (g/kg) qp (g/kg)
35 Downscaling and Parameterization [Summary] Two closely linked operations Downscaling is a pre-condition for Parameterization Parameterization implicitly/partially contains Downscaling Probablistic(Bayesian) Perspectives Link to Data Assimilation Example: NAM-SCA
36 Subgrid-Scale Information Useful for Downscaling Contained in Parameterization cloud fraction convective precipitation rate convective mass-flux = convection fraction x convective vertical velocity subgrid-scale distribution of water subgrid-scale vertical (heat) transport etc
37 Needs For More Coordinated Downscaling-Parameterization Studies
38 Conclusions Limitations of Traditional Approaches: Parameterization: No Interactions between the subgrid-scale elments: No Geometrical Information Downscaling: No Physics (statistical) or Off-Line (regionalization)
39 Conclusions Subgrid-Scale Representation (SSR): Downscaling Parameterization Multiresolutional Analysis: A Systematic Approach: Mode Decomposition: Compression & Decompression Example of SSR: NAM-SCA: Nonhydrostatic Anelastic Model with Segmentally-Constnat Appoximation: decomposition by ensemble of plumes Limitations of Traditional Approaches:
Mass-flux parameterization in the shallow convection gray zone
Mass-flux parameterization in the shallow convection gray zone LACE stay report Toulouse Centre National de Recherche Meteorologique, 15. September 2014 26. September 2014 Scientific supervisor: Rachel
More informationWhere is the Interface of the Stratocumulus-Topped PBL?
2626 J O U R N A L O F T H E A T M O S P H E R I C S C I E N C E S VOLUME 62 Where is the Interface of the Stratocumulus-Topped PBL? C.-H. MOENG National Center for Atmospheric Research,* Boulder, Colorado
More informationAn Improved Framework for Superparameterization
1940 JOURNAL OF THE ATMOSPHERIC SCIENCES An Improved Framework for Superparameterization WOJCIECH W. GRABOWSKI National Center for Atmospheric Research,* Boulder, Colorado (Manuscript received 29 May 2003,
More informationClouds in global models are variable
Clouds in global models are variable There s explicit variability within grid columns: Vertical structure ( overlap ) + fractional cloudiness = internally variable columns Let s take a look at how overlap
More informationThe role of organiza.on in tropical large- scale, convec.ve interac.ons
The role of organiza.on in tropical large- scale, convec.ve interac.ons Emily M. Riley University of Miami RSMAS CMMAP Mee9ng 22 24 January 213 Advisor: Brian Mapes, Collaborators: Stefan Tulich and Zhuming
More informationVI Workshop Brasileiro de Micrometeorologia
Validation of a statistic algorithm applied to LES model Eduardo Bárbaro, Amauri Oliveira, Jacyra Soares November 2009 Index Objective 1 Objective 2 3 Vertical Profiles Flow properties 4 Objective 1 The
More informationALADIN-2007-Oslo (Norway) April 2007
Improving the SURFEX/TEB scheme: 1 D validation in a street canyon R. Hamdi and V. Masson SURFEX coupled off line to ALADIN: preliminary results over Belgium R. Hamdi and A. Deckmyn ALADIN-2007-Oslo (Norway)
More informationGeorge H. Bryan, Richard Rotunno, National Center for Atmospheric Research, Boulder, Colorado, USA
8C.7 THE EFFECTS OF TURBULENCE ON HURRICANE INTENSITY George H. Bryan, Richard Rotunno, National Center for Atmospheric Research, Boulder, Colorado, USA and Yongsheng Chen York University, Toronto, Ontario,
More informationMODELED MESOSCALE GRAVITY WAVES: CONTINUOUS SPECTRUM AND ENERGY CASCADE Chungu Lu 1, Steven Koch, Fuqing Zhang, and Ning Wang
P6.5 MODELED MESOSCALE GRAVITY WAVES: CONTINUOUS SPECTRUM AND ENERGY CASCADE Chungu Lu 1, Steven Koch, Fuqing Zhang, and Ning Wang NOAA Research-Forecast Systems Laboratory, Boulder, Colorado [In collaboration
More informationGREYBLS: modelling GREY-zone Boundary LayerS
GREYBLS: modelling GREY-zone Boundary LayerS Bob Beare, Bob Plant, Omduth Coceal, John Thuburn, Adrian Lock, Humphrey Lean 25 Sept 2013 Introduction NWP at grid lengths 2 km - 100 m now possible. Introduction
More informationThe inclusion of cloudy radiances in the NCEP GSI analysis system
he inclusion of cloudy radiances in the NCEP GSI analysis system 1,2,3 Min-Jeong Kim 1 Fuzhong Weng and 2 John Derber 1.NOAA/NESDIS/SAR 2. Joint Center for Satellite Data Assimilation (JCSDA) 3. CIRA,
More informationStochastic subgrid scale modeling
Stochastic subgrid scale modeling Daan Crommelin Centrum Wiskunde & Informatica, Amsterdam joint work with Eric Vanden-Eijnden, New York University NDNS+, 15 april 21 p. 1/24 The parameterization problem:
More informationA Multiscale Non-hydrostatic Atmospheric Model for Regional and Global Applications
A Multiscale Non-hydrostatic Atmospheric Model for Regional and Global Applications James D. Doyle 1, Frank Giraldo 2, Saša Gaberšek 1 1 Naval Research Laboratory, Monterey, CA, USA 2 Naval Postgraduate
More informationAbout the SPEEDY model (from Miyoshi PhD Thesis):
SPEEDY EXPERIMENTS. About the SPEEDY model (from Miyoshi PhD Thesis): The SPEEDY model (Molteni 2003) is a recently developed atmospheric general circulation model (AGCM) with a spectral primitive-equation
More informationBob Beare University of Exeter Thanks to Adrian Lock, John Thuburn and Bob Plant
Modelling convective boundary layers in the terra-incognita 4800 800 m resolution 3.0 h 4800 50 m resolution 3.0 h 2880 2880 960 960 y (m) y (m) -960-960 -2880-2880 -4800-4800 -2400 0 2400 4800 x (m) -4800-4800
More informationParameterizing Cloud Layers and their Microphysics
Parameterizing Cloud Layers and their Microphysics Vincent E. Larson Atmospheric Science Group, Dept. of Math Sciences University of Wisconsin --- Milwaukee I acknowledge my collaborators: Adam Smith,
More informationA Multiscale Nested Modeling Framework to Simulate the Interaction of Surface Gravity Waves with Nonlinear Internal Gravity Waves
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. A Multiscale Nested Modeling Framework to Simulate the Interaction of Surface Gravity Waves with Nonlinear Internal Gravity
More informationA Cloud-Resolving Model with an Adaptive Vertical Grid for Boundary Layer Clouds
1058 J O U R N A L O F T H E A T M O S P H E R I C S C I E N C E S VOLUME 68 A Cloud-Resolving Model with an Adaptive Vertical Grid for Boundary Layer Clouds ROGER MARCHAND AND THOMAS ACKERMAN Joint Institute
More informationPUBLICATIONS. Journal of Advances in Modeling Earth Systems
PUBLICATIONS Journal of Advances in Modeling Earth Systems RESEARCH ARTICLE 10.1002/2015MS000572 Key Points: Influence of domain size and vertical and horizontal resolution in ILES of the STBL is investigated
More informationHydrologic modelling at a continuous permafrost site using MESH. S. Pohl, P. Marsh, and S. Endrizzi
Hydrologic modelling at a continuous permafrost site using MESH S. Pohl, P. Marsh, and S. Endrizzi Purpose of Study Test the latest version of MESH at a continuous permafrost site Model performance will
More informationEULAG: high-resolution computational model for research of multi-scale geophysical fluid dynamics
Zbigniew P. Piotrowski *,** EULAG: high-resolution computational model for research of multi-scale geophysical fluid dynamics *Geophysical Turbulence Program, National Center for Atmospheric Research,
More informationSuper-Parameterization of Boundary Layer Roll Vortices in Tropical Cyclone Models
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Super-Parameterization of Boundary Layer Roll Vortices in Tropical Cyclone Models PI Isaac Ginis Graduate School of Oceanography
More informationGlobal non-hydrostatic modelling using Voronoi meshes: The MPAS model
Global non-hydrostatic modelling using Voronoi meshes: The MPAS model William C. Skamarock, Joseph B. Klemp, Michael Duda, Laura Fowler and Sang-Hun Park National Center for Atmospheric Research Boulder,
More informationFree Convection in a Water Glass
Solved with COMSOL Multiphysics 4.1. Free Convection in a Water Glass Introduction This model treats free convection in a glass of water. Free convection is a phenomenon that is often disregarded in chemical
More informationDirect radiative forcing of aerosol
Direct radiative forcing of aerosol 1) Model simulation: A. Rinke, K. Dethloff, M. Fortmann 2) Thermal IR forcing - FTIR: J. Notholt, C. Rathke, (C. Ritter) 3) Challenges for remote sensing retrieval:
More informationContinued Investigation of Small-Scale Air-Sea Coupled Dynamics Using CBLAST Data
Continued Investigation of Small-Scale Air-Sea Coupled Dynamics Using CBLAST Data Dick K.P. Yue Center for Ocean Engineering Department of Mechanical Engineering Massachusetts Institute of Technology Cambridge,
More informationGEOG 4110/5100 Advanced Remote Sensing Lecture 4
GEOG 4110/5100 Advanced Remote Sensing Lecture 4 Geometric Distortion Relevant Reading: Richards, Sections 2.11-2.17 Review What factors influence radiometric distortion? What is striping in an image?
More informationHPC Methods for Coupling Spectral Cloud Microphysics with the COSMO Model
Center for Information Services and High Performance Computing (ZIH) HPC Methods for Coupling Spectral Cloud Microphysics with the COSMO Model Max Planck Institute for Meteorology 17 March 2011 Matthias
More informationHorizontal Mixing in the WRF-ARW Model. Russ Schumacher AT April 2006
Horizontal Mixing in the WRF-ARW Model Russ Schumacher AT 730 5 April 2006 Overview Description of implicit and explicit horizontal mixing in WRF Evaluation of WRF s implicit mixing Model options for explicit
More informationUsing visible and near-infrared satellite observations for convective-scale data assimilation
Using visible and near-infrared satellite observations for convective-scale data assimilation Leonhard Scheck1,2, Bernhard Mayer2, Martin Weissmann1,2 1) Hans-Ertl-Center for Weather Research, Data Assimilation
More informationlecture 8 Groundwater Modelling -1
The Islamic University of Gaza Faculty of Engineering Civil Engineering Department Water Resources Msc. Groundwater Hydrology- ENGC 6301 lecture 8 Groundwater Modelling -1 Instructor: Dr. Yunes Mogheir
More informationMeasurement of Convective Entrainment Using Lagrangian Particles
266 J O U R N A L O F T H E A T M O S P H E R I C S C I E N C E S VOLUME 7 Measurement of Convective Entrainment Using Lagrangian Particles KYONGMIN YEO AND DAVID M. ROMPS Earth Sciences Division, Lawrence
More informationReflectivity modeling for stratified anelastic media
Reflectivity modeling for stratified anelastic media Peng Cheng and Gary F. Margrave Reflectivity modeling ABSTRACT The reflectivity method is widely used for the computation of synthetic seismograms for
More information(x, y, z) m 2. (x, y, z) ...] T. m 2. m = [m 1. m 3. Φ = r T V 1 r + λ 1. m T Wm. m T L T Lm + λ 2. m T Hm + λ 3. t(x, y, z) = m 1
Class 1: Joint Geophysical Inversions Wed, December 1, 29 Invert multiple types of data residuals simultaneously Apply soft mutual constraints: empirical, physical, statistical Deal with data in the same
More informationLarge Eddy Simulation Applications to Meteorology
Large Eddy Simulation Applications to Meteorology Marcelo Chamecki Department of Meteorology The Pennsylvania State University Tutorial School on Fluid Dynamics: Topics in Turbulence May 27 th 2010, College
More informationIntroduction to C omputational F luid Dynamics. D. Murrin
Introduction to C omputational F luid Dynamics D. Murrin Computational fluid dynamics (CFD) is the science of predicting fluid flow, heat transfer, mass transfer, chemical reactions, and related phenomena
More informationA mass-conservative version of the semi- Lagrangian semi-implicit HIRLAM using Lagrangian vertical coordinates
A mass-conservative version of the semi- Lagrangian semi-implicit HIRLAM using Lagrangian vertical coordinates Peter Hjort Lauritzen Atmospheric Modeling & Predictability Section National Center for Atmospheric
More informationUsing the Scaling Equations to Define Experimental Matrices for Software Validation
Using the Scaling Equations to Define Experimental Matrices for Software Validation Richard R. Schultz, Edwin Harvego, Brian G. Woods, and Yassin Hassan V&V30 Standards Committee Presentation Content Description
More informationDevelopment and Testing of a Next Generation Spectral Element Model for the US Navy
Development and Testing of a Next Generation Spectral Element Model for the US Navy Alex Reinecke 1, Kevin Viner 1, James Doyle 1, Sasa Gabersek 1, Matus Martini 2, John Mickalakes 3, Dave Ryglicki 4,
More informationFlow Structures Extracted from Visualization Images: Vector Fields and Topology
Flow Structures Extracted from Visualization Images: Vector Fields and Topology Tianshu Liu Department of Mechanical & Aerospace Engineering Western Michigan University, Kalamazoo, MI 49008, USA We live
More informationMulti-Resolution Climate Ensemble Parameter Analysis with Nested Parallel Coordinates Plots
Multi-Resolution Climate Ensemble Parameter Analysis with Nested Parallel Coordinates Plots Junpeng Wang, Xiaotong Liu, Han-Wei Shen, Member, IEEE, and Guang Lin Fig. 1. The proposed visual analytics system:
More informationQuantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Quantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement Lian Shen Department of Mechanical Engineering
More informationBoundary Layer Parameterization
Boundary Layer Parameterization Bob Plant With thanks to: R. Beare, S. Belcher, I. Boutle, O. Coceal, A. Grant, D. McNamara NWP Physics Lecture 3 Nanjing Summer School July 2014 Outline Motivation Some
More informationOptimal Wavelet Features for an Infrared Satellite Precipitation Estimate Algorithm
Optimal Wavelet Features for an Infrared Satellite Precipitation Estimate Algorithm Majid Mahrooghy 1, 2, Valentine G. Anantharaj 2, Nicolas H. Younan 1, 2, and James Aanstoos 2 1 Department of Electrical
More informationJunhong Wei Goethe University of Frankfurt. Other contributor: Prof. Dr. Ulrich Achatz, Dr. Gergely Bölöni
Efficient modelling of the gravity-wave interaction with unbalanced resolved flows: Pseudo-momentum-flux convergence vs direct approach Junhong Wei Goethe University of Frankfurt Other contributor: Prof.
More informationModule 1: Introduction to Finite Difference Method and Fundamentals of CFD Lecture 6:
file:///d:/chitra/nptel_phase2/mechanical/cfd/lecture6/6_1.htm 1 of 1 6/20/2012 12:24 PM The Lecture deals with: ADI Method file:///d:/chitra/nptel_phase2/mechanical/cfd/lecture6/6_2.htm 1 of 2 6/20/2012
More informationIntroduction to Computational Fluid Dynamics Mech 122 D. Fabris, K. Lynch, D. Rich
Introduction to Computational Fluid Dynamics Mech 122 D. Fabris, K. Lynch, D. Rich 1 Computational Fluid dynamics Computational fluid dynamics (CFD) is the analysis of systems involving fluid flow, heat
More informationStratocumulus over SouthEast Pacific: Idealized 2D. simulations with the Lagrangian Cloud Model
Stratocumulus over SouthEast Pacific: Idealized 2D simulations with the Lagrangian Cloud Model M. Andrejczuk, A. Gadian, A. Blyth Corresponding Author: M. Andrejczuk M.Andrejczuk@leeds.ac.uk School of
More informationOptical Theory Basics - 2 Atmospheric corrections and parameter retrieval
Optical Theory Basics - 2 Atmospheric corrections and parameter retrieval Jose Moreno 3 September 2007, Lecture D1Lb2 OPTICAL THEORY-FUNDAMENTALS (2) Radiation laws: definitions and nomenclature Sources
More informationSeptember 18, B Math Test Chapter 1 Name: x can be expressed as: {y y 0, y R}.
September 8, 208 62B Math Test Chapter Name: Part : Objective Questions [ mark each, total 2 marks]. State whether each of the following statements is TRUE or FALSE a) The mapping rule (x, y) (-x, y) represents
More informationCHAPTER 3 DIFFERENT DOMAINS OF WATERMARKING. domain. In spatial domain the watermark bits directly added to the pixels of the cover
38 CHAPTER 3 DIFFERENT DOMAINS OF WATERMARKING Digital image watermarking can be done in both spatial domain and transform domain. In spatial domain the watermark bits directly added to the pixels of the
More informationConvection Cooling of Circuit Boards 3D Natural Convection
Convection Cooling of Circuit Boards 3D Natural Convection Introduction This example models the air cooling of circuit boards populated with multiple integrated circuits (ICs), which act as heat sources.
More informationR&D on dynamical kernels and subkm scale modeling with ALADIN/AROME. 35th EWGLAM and 20th SRNWP Meeting
R&D on dynamical kernels and subkm scale modeling with ALADIN/AROME 35th EWGLAM and 20th SRNWP Meeting Outline 1. 500m resolution experiments 2. Scalability 3. Ongoing research in Meteo-France with dynamics
More informationMultivariate-Spline and Scale-Specific Solution for Variational Analyses
FEBRUARY 4 NOTES AND CORRESPONDENCE 39 Multivariate-Spline and Scale-Specific Solution for Variational Analyses TOSHIO M. CHIN RSMAS/MPO, University of Miami, Miami, Florida, and et Propulsion Laboratory,
More informationPrinciples of the Global Positioning System Lecture 15" Propagation Medium: Neutral atmosphere" Basic atmospheric structure"
12.540 Principles of the Global Positioning System Lecture 15" Prof. Thomas Herring" Room 54-820A; 253-5941" tah@mit.edu" http://geoweb.mit.edu/~tah/12.540 " Propagation Medium: Neutral atmosphere" Summary"
More informationThe Spherical Harmonics Discrete Ordinate Method for Atmospheric Radiative Transfer
The Spherical Harmonics Discrete Ordinate Method for Atmospheric Radiative Transfer K. Franklin Evans Program in Atmospheric and Oceanic Sciences University of Colorado, Boulder Computational Methods in
More informationScalable Dynamic Load Balancing of Detailed Cloud Physics with FD4
Center for Information Services and High Performance Computing (ZIH) Scalable Dynamic Load Balancing of Detailed Cloud Physics with FD4 Minisymposium on Advances in Numerics and Physical Modeling for Geophysical
More informationCrosswell Imaging by 2-D Prestack Wavepath Migration
Crosswell Imaging by 2-D Prestack Wavepath Migration Hongchuan Sun ABSTRACT Prestack wavepath migration (WM) is applied to 2-D synthetic crosswell data, and the migrated images are compared to those from
More informationGOES-R AWG Radiation Budget Team: Absorbed Shortwave Radiation at surface (ASR) algorithm June 9, 2010
GOES-R AWG Radiation Budget Team: Absorbed Shortwave Radiation at surface (ASR) algorithm June 9, 2010 Presented By: Istvan Laszlo NOAA/NESDIS/STAR 1 ASR Team Radiation Budget AT chair: Istvan Laszlo ASR
More informationGeometric adaptation and parameterization of subspacebased reduced models
Platzhalter für Bild, Bild auf Titelfolie hinter das Logo einsetzen Geometric adaptation and parameterization of subspacebased reduced models Ralf Zimmermann, AG Numerik, ICM, TU Braunschweig Workshop:
More information1. Interpreting the Results: Visualization 1
1. Interpreting the Results: Visualization 1 visual/graphical/optical representation of large sets of data: data from experiments or measurements: satellite images, tomography in medicine, microsopy,...
More informationRK-Time Integration and High-Order Spatial Discretization a New Dynamical Core for the LMK
RK-Time Integration and High-Order Spatial Discretization a New Dynamical Core for the LMK Jochen Förstner Deutscher Wetterdienst, Kaiserleistraße 35, 63067 Offenbach am Main jochen.foerstner@dwd.de COSMO
More informationValidation of inferred high resolution ocean pco2 and air-sea fluxes with in-situ and remote sensing data.
Validation of inferred high resolution ocean pco2 and air-sea fluxes with in-situ and remote sensing data. Ismael Hernandez, Hussein Yahia, Joël Sudre, Véronique Garçon, Christoph Garbe, Boris Dewitte,
More informationComparative Study between DCT and Wavelet Transform Based Image Compression Algorithm
IOSR Journal of Computer Engineering (IOSR-JCE) e-issn: 2278-0661,p-ISSN: 2278-8727, Volume 17, Issue 1, Ver. II (Jan Feb. 2015), PP 53-57 www.iosrjournals.org Comparative Study between DCT and Wavelet
More informationConstraining Rainfall Replicates on Remote Sensed and In-Situ Measurements
Constraining Rainfall Replicates on Remote Sensed and In-Situ Measurements Seyed Hamed Alemohammad, Dara Entekhabi, Dennis McLaughlin Ralph M. Parsons Laboratory for Environmental Science and Engineering
More informationHomogenization and numerical Upscaling. Unsaturated flow and two-phase flow
Homogenization and numerical Upscaling Unsaturated flow and two-phase flow Insa Neuweiler Institute of Hydromechanics, University of Stuttgart Outline Block 1: Introduction and Repetition Homogenization
More informationAdvanced Numerical Methods for NWP Models
Advanced Numerical Methods for NWP Models Francis X. Giraldo Naval Postgraduate School Monterey, CA 93943-5502 phone: (831) 656-2293 fax: (831) 656-2355 e-mail: fxgirald@nps.edu Award #: N0001406WX20257
More informationusrdef 1dsur spec: specifies the setup of boundary forcing for water column applications (1-D mode)
Chapter 17 Surface forcing and nesting This chapter discusses the setup of the surface forcing needed for the application of surface boundary conditions and the procedures for defining nesting. The following
More informationSpatial Hydrologic Modeling Using NEXRAD Rainfall Data in an HEC-HMS (MODClark) Model
v. 10.0 WMS 10.0 Tutorial Spatial Hydrologic Modeling Using NEXRAD Rainfall Data in an HEC-HMS (MODClark) Model Learn how to setup a MODClark model using distributed rainfall data Objectives Read an existing
More informationA 3D VOF model in cylindrical coordinates
A 3D VOF model in cylindrical coordinates Marmar Mehrabadi and Markus Bussmann Department of Mechanical and Industrial Engineering, University of Toronto Recently, volume of fluid (VOF) methods have improved
More informationA refined statistical cloud closure using double-gaussian probability density functions
Geosci. Model Dev., 6, 1641 1657, 2013 doi:10.5194/gmd-6-1641-2013 Author(s) 2013. CC Attribution 3.0 License. Geoscientific Model Development Open Access A refined statistical cloud closure using double-gaussian
More informationQuantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement
DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Quantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement Lian Shen Department of Mechanical Engineering
More informationYOTC dataset analysis, MJO sensitivity, and ECMWF forecast skill
YOTC dataset analysis, MJO sensitivity, and ECMWF forecast skill Thank You Organizers (Mitch, Duane, Jenny Lin) Peter Bechtold 1, Frederic Vitart 1, Linda Hirons 2, Sanda Ðivanović 3 1 ECMWF 2 Reading
More informationEfficient 3D Gravity and Magnetic Modeling
Efficient 3D Gravity and Magnetic Modeling X. Li Fugro Gravity & Magnetic Services Inc., Houston, Texas, USA Summary There are many different spatial-domain algorithms for 3D gravity and magnetic forward
More informationHow TMG Uses Elements and Nodes
Simulation: TMG Thermal Analysis User's Guide How TMG Uses Elements and Nodes Defining Boundary Conditions on Elements You create a TMG thermal model in exactly the same way that you create any finite
More informationData-Driven Modeling. Scientific Computation J. NATHAN KUTZ OXPORD. Methods for Complex Systems & Big Data
Data-Driven Modeling & Scientific Computation Methods for Complex Systems & Big Data J. NATHAN KUTZ Department ofapplied Mathematics University of Washington OXPORD UNIVERSITY PRESS Contents Prolegomenon
More informationCalculation Methods. IES Virtual Environment 6.4 CIBSE Heat Loss & Heat Gain (ApacheCalc)
Calculation Methods IES Virtual Environment 6.4 CIBSE Heat Loss & Heat Gain (ApacheCalc) Contents Calculation Methods...1 1 Introduction...3 2 Heat Loss...4 2.1 Heat Loss Methodology... 4 3 Heat Gain...5
More informationParallel Computing. Parallel Algorithm Design
Parallel Computing Parallel Algorithm Design Task/Channel Model Parallel computation = set of tasks Task Program Local memory Collection of I/O ports Tasks interact by sending messages through channels
More informationMiddle East Technical University Mechanical Engineering Department ME 413 Introduction to Finite Element Analysis Spring 2015 (Dr.
Middle East Technical University Mechanical Engineering Department ME 413 Introduction to Finite Element Analysis Spring 2015 (Dr. Sert) COMSOL 1 Tutorial 2 Problem Definition Hot combustion gases of a
More informationSpatial Hydrologic Modeling HEC-HMS Distributed Parameter Modeling with the MODClark Transform
v. 9.0 WMS 9.0 Tutorial Spatial Hydrologic Modeling HEC-HMS Distributed Parameter Modeling with the MODClark Transform Setup a basic distributed MODClark model using the WMS interface Objectives In this
More informationMULTIRESOLUTION. APPROACHES in TURBULENCE. MULHSCALf and. Applications. LES, DES and Hybrid. 2nd Edition. RANS/LES Methods and Guidelines
2nd Edition MULHSCALf and MULTIRESOLUTION APPROACHES in TURBULENCE LES, DES and Hybrid Applications RANS/LES Methods and Guidelines Pierre Sagaut Uniuersite Pierre et Marie Curie-Paris 6, France Sebastien
More informationThree dimensional meshless point generation technique for complex geometry
Three dimensional meshless point generation technique for complex geometry *Jae-Sang Rhee 1), Jinyoung Huh 2), Kyu Hong Kim 3), Suk Young Jung 4) 1),2) Department of Mechanical & Aerospace Engineering,
More informationFluent User Services Center
Solver Settings 5-1 Using the Solver Setting Solver Parameters Convergence Definition Monitoring Stability Accelerating Convergence Accuracy Grid Independence Adaption Appendix: Background Finite Volume
More informationSemester Final Report
CSUMS SemesterFinalReport InLaTex AnnKimball 5/20/2009 ThisreportisageneralsummaryoftheaccumulationofknowledgethatIhavegatheredthroughoutthis semester. I was able to get a birds eye view of many different
More informationParameterization of orographic effects on surface radiation in AROME
Parameterization of orographic effects on surface radiation in AROME Christoph Wittmann on behalf of Alexandre Mary, Laura Rontu, Yann Seity and Clemens Wastl partly financed by Content Motivation Method
More informationLab 9: FLUENT: Transient Natural Convection Between Concentric Cylinders
Lab 9: FLUENT: Transient Natural Convection Between Concentric Cylinders Objective: The objective of this laboratory is to introduce how to use FLUENT to solve both transient and natural convection problems.
More informationA Direct Simulation-Based Study of Radiance in a Dynamic Ocean
A Direct Simulation-Based Study of Radiance in a Dynamic Ocean Dick K.P. Yue Center for Ocean Engineering Massachusetts Institute of Technology Room 5-321, 77 Massachusetts Ave, Cambridge, MA 02139 phone:
More informationEFFICIENT METHODS FOR ENCODING REGIONS OF INTEREST IN THE UPCOMING JPEG2000 STILL IMAGE CODING STANDARD
EFFICIENT METHODS FOR ENCODING REGIONS OF INTEREST IN THE UPCOMING JPEG2000 STILL IMAGE CODING STANDARD Charilaos Christopoulos, Joel Askelöf and Mathias Larsson Ericsson Research Corporate Unit Ericsson
More informationApplication of the Volume-of-Fluid Method to the Advection Condensation Problem
SEPTEMBER 997 MARGOLN ET AL. 2265 Application of the Volume-of-Fluid Method to the Advection Condensation Problem LEN MARGOLN AND JON M. RESNER Los Alamos National Laboratory, Los Alamos, New Mexico* POTR
More informationA Direct Simulation-Based Study of Radiance in a Dynamic Ocean
1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. A Direct Simulation-Based Study of Radiance in a Dynamic Ocean LONG-TERM GOALS Dick K.P. Yue Center for Ocean Engineering
More informationPARAMETERIZATION OF DRAG FORCES IN URBAN CANOPY MODELS USING MICROSCALE-CFD MODELS FOR DIFFERENT WIND DIRECTIONS
PARAMETERIZATION OF DRAG FORCES IN URBAN CANOPY MODELS USING MICROSCALE-CFD MODELS FOR DIFFERENT WIND DIRECTIONS J. L. Santiago 1, O. Coceal 2 and A. Martilli 1 1 Atmospheric Pollution Division, Environmental
More informationScale Dependency of Total Water Variance and Its Implication for Cloud Parameterizations
NOVEMBER 2013 S C H E M A N N E T A L. 3615 Scale Dependency of Total Water Variance and Its Implication for Cloud Parameterizations VERA SCHEMANN, BJORN STEVENS, AND VERENA GRÜTZUN Max Planck Institute
More informationExample 13 - Shock Tube
Example 13 - Shock Tube Summary This famous experiment is interesting for observing the shock-wave propagation. Moreover, this case uses the representation of perfect gas and compares the different formulations:
More informationScalability Improvement of the NASA Multiscale Modeling Framework for Tropical Cyclone Climate Study
Scalability Improvement of the NASA Multiscale Modeling Framework for Tropical Cyclone Climate Study Bo-Wen Shen 1,2, Bron Nelson 3, Samson Cheung 3, and Wei-Kuo Tao 2 Dr. Bo-Wen Shen, Earth System Science
More informationMIKE SHE WQ User Manual Particle Tracking Module
MIKE SHE WQ User Manual Particle Tracking Module CONTENTS 1 INTRODUCTION... 1 2 ACTIVATING THE MIKE SHE PARTICLE TRACKING MODULE... 1 3 RUNNING THE PARTICLE TRACKING MODULE... 2 4 CREATING INPUT FOR THE
More informationGEOPHYS 242: Near Surface Geophysical Imaging. Class 8: Joint Geophysical Inversions Wed, April 20, 2011
GEOPHYS 4: Near Surface Geophysical Imaging Class 8: Joint Geophysical Inversions Wed, April, 11 Invert multiple types of data residuals simultaneously Apply soft mutual constraints: empirical, physical,
More informationAtmospheric distortions of spaceborne SAR polarimetric signatures at X and Ka-band
Atmospheric distortions of spaceborne SAR polarimetric signatures at X and Ka-band S. Mori 1,2, Frank. S. Marzano 1,2 and N. Pierdicca 1 1. Sapienza University of Rome, Italy 2. CETEMPS University of L
More informationIMAGE PROCESSING USING DISCRETE WAVELET TRANSFORM
IMAGE PROCESSING USING DISCRETE WAVELET TRANSFORM Prabhjot kour Pursuing M.Tech in vlsi design from Audisankara College of Engineering ABSTRACT The quality and the size of image data is constantly increasing.
More informationHYDRUS (2D/3D) Computer Session
HYDRUS (2D/3D) Computer Session Three-Dimensional Water Flow and Solute Transport This tutorial considers water flow and solute transport in a simple three-dimensional transport domain. The transport domain
More informationVariability in Annual Temperature Profiles
Variability in Annual Temperature Profiles A Multivariate Spatial Analysis of Regional Climate Model Output Tamara Greasby, Stephan Sain Institute for Mathematics Applied to Geosciences, National Center
More information