Multi-Resolution Homogenization of Multi-Scale Laminates: Scale Dependent Parameterization or: Homogenization procedure that retains FINITE-scale-related.

Slides:



Advertisements
Similar presentations
Trend evaluation and comparison of the use and value of GL in core demography and computer science journals Rosa Di Cesare, Roberta Ruggieri, CNR-IRPPS.
Advertisements

A Tailorable Environment for Assessing the Quality of Deployment Architectures in Highly Distributed Settings Sam Malek and Marija Mikic-Rakic Nels Beckman.
UML and WSDL for JISC e-Learning Projects Major Practical Richard Hopkins NeSC Training Team Member
RCUK, Octiber Archiving research data and research publications. Dr Leslie Carr, Intelligence, Agents Multimedia, University of Southampton Dr Simon.
NATO ASI Conference, Kyiv Pollutant Dispersion Investigation of buoyancy effects on distribution of mean concentration field in the turbulent circulation.
17 May Multiple Sites. 17 May Multiple Sites This presentation assumes you are already familiar with Doors and all its standard commands It.
An Advanced Shell Theory Based Tire Model by D. Bozdog, W. W. Olson Department of Mechanical, Industrial and Manufacturing Engineering The 23 rd Annual.
Fitzkilism Production, Putting the Fun in Function By Mrs. Kiley Sandymount Elementary.
© Pearson Education Limited, Chapter 8 Normalization Transparencies.
COAT -TRIBUNALS' MODEL PRACTICE GUIDE - AIJA COAT TRIBUNALS MODEL PRACTICE MANUAL Livingston Armytage Centre for Judicial Studies
Søren Poulsen, Ørsted·DTU, Automation Technical University of Denmark NORPIE Integrating switch mode audio power amplifiers and.
Tim Richards, Tim Green, Simo Varis EFIS Information Resource Discovery - Demonstrator (a.k.a EFIS-RD/ Metadata) 28 June 2005.
Processing of multiple frequency test data of Traction Auto Transformer Helen Di Yu Power Systems Research Group University of Strathclyde.
Two-dimensional Effects on the CSR Interaction Forces for an Energy-Chirped Bunch Rui Li, J. Bisognano, R. Legg, and R. Bosch.
Web Services Choreography Description Language (WS-CDL) Jacek Kopecký June 2004.
12/6/20041 TITLE: Basic Multicarrier EVDV operation SOURCE: Srinivasan
NYSDOT – M. IveyAASTHO SCOE – June 9, Maintaining Project Commitments New York State DOT Perspective Mary E. Ivey, Director Environmental Analysis.
NEW ANALYTIC DC MODELS FOR TUNNEL DIODE AND RESONANT TUNNELING DIODE Chien M. Ta (SMA) Fujiang Lin (IME) Subhash R. Chander (IME) SYMPOSIUM ON ELECTRONICS.
What Is the Council’s Role in Program Implementation? County Extension Council Training Module Missouri Council Leadership Development — a partnership.
Søren Poulsen, Ørsted·DTU, Automation Technical University of Denmark NORPIE Hysteresis Controller with constant switching frequency.
Søren Poulsen, Ørsted·DTU, Automation Technical University of Denmark NORPIE Integrating switch mode audio power amplifiers and.
8 April Doors TM Set System Options. 8 April Set System Options Allows you to set certain standard Doors operating parameters and enable certain.
ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete Objectives: Response to a Sinusoidal Input Frequency Analysis of an RC Circuit.
Lect.3 Modeling in The Time Domain Basil Hamed
Principal Component Analysis Based on L1-Norm Maximization Nojun Kwak IEEE Transactions on Pattern Analysis and Machine Intelligence, 2008.
Point-wise Discretization Errors in Boundary Element Method for Elasticity Problem Bart F. Zalewski Case Western Reserve University Robert L. Mullen Case.
EEE 498/598 Overview of Electrical Engineering
PERTURBATION THEORY Time Independent Theory. A Necessity: Exactly solvable problems are very few and do not really represent a real physical system completely.
Time-domain Crosstalk The equations that describe crosstalk in time-domain are derived from those obtained in the frequency-domain under the following.
Adnan Khan Lahore University of Management Sciences Peter Kramer Rensselaer Polytechnic Institute.
Adnan Khan Department of Mathematics Lahore University of Management Sciences.
Basic Concepts and Definitions Vector and Function Space. A finite or an infinite dimensional linear vector/function space described with set of non-unique.
Completeness of the Coulomb eigenfunctions Myles Akin Cyclotron Institute, Texas A&M University, College Station, Texas University of Georgia, Athens,
EMLAB 1 Power Flow and PML Placement in FDTD. EMLAB 2 Lecture Outline Review Total Power by Integrating the Poynting Vector Total Power by Plane Wave.
Ch 8.1 Numerical Methods: The Euler or Tangent Line Method
1 Numerical and Analytical models for various effects in models for various effects inEDFAs Inna Nusinsky-Shmuilov Supervisor:Prof. Amos Hardy TEL AVIV.
Emergent Universe Scenario
Lecture 20: More on the deuteron 18/11/ Analysis so far: (N.B., see Krane, Chapter 4) Quantum numbers: (J , T) = (1 +, 0) favor a 3 S 1 configuration.
1 Sagnac Effect in Rotating Photonic Crystal Micro-Cavities and Miniature Optical Gyroscopes Tel Aviv University Ben Z. Steinberg Ady Shamir Amir Boag.
Laboratoire Environnement, Géomécanique & Ouvrages Comparison of Theory and Experiment for Solute Transport in Bimodal Heterogeneous Porous Medium Fabrice.
ON MULTISCALE THEORY OF TURBULENCE IN WAVELET REPRESENTATION M.V.Altaisky
Propagation in Photonic Crystal Coupled Cavity Waveguides Possessing Discontinuities Ben Z. Steinberg Amir Boag Orli Hershkoviz Mark Perlson Tel Aviv University.
Eurostat Statistical matching when samples are drawn according to complex survey designs Training Course «Statistical Matching» Rome, 6-8 November 2013.
Stress constrained optimization using X-FEM and Level Set Description
Magnetic Field Issues for Simulation and Reconstruction N. Amapane, N. Neumeister Workshop on LHC Physics with High-p T Muons in CMS Bologna, April 9-12,
Weak Solutions of Kinematic Aggregation Equations Andrea Bertozzi Department of Mathematics UCLA Thanks to Thomas Laurent for contributing to the slides.
On Describing Mean Flow Dynamics in Wall Turbulence J. Klewicki Department of Mechanical Engineering University of New Hampshire Durham, NH
Modeling Electromagnetic Fields in Strongly Inhomogeneous Media
Generalized Finite Element Methods
1 LES of Turbulent Flows: Lecture 7 (ME EN ) Prof. Rob Stoll Department of Mechanical Engineering University of Utah Fall 2014.
Project Background My project goal was to accurately model a dipole in the presence of the lossy Earth. I used exact image theory developed previously.
Materials Process Design and Control Laboratory Sibley School of Mechanical and Aerospace Engineering 169 Frank H. T. Rhodes Hall Cornell University Ithaca,
1 VARIOUS ISSUES IN THE LARGE STRAIN THEORY OF TRUSSES STAMM 2006 Symposium on Trends in Applications of Mathematics to Mechanics Vienna, Austria, 10–14.
Neutrino Oscillation in Dense Matter Speaker: Law Zhiyang, National University of Singapore.
Prof. David R. Jackson Dept. of ECE Fall 2015 Notes 8 ECE 6340 Intermediate EM Waves 1.
Bounded Solutions of Kinematic Aggregation Equations Andrea Bertozzi Department of Mathematics, UCLA Thanks to support from ARO, NSF, and ONR and to contributions.
Math for CS Fourier Transforms
Hanyang University Antennas & RF Devices Lab. ANTENNA THEORY ANALYSIS AND DESIGN Prof. Jaehoon Choi Dept. of Electronics and Computer Engineering
Linear systems: University of Illinois at Chicago ECE 427, Dr. D. Erricolo University of Illinois at Chicago ECE 427, Dr. D. Erricolo Consider two complex.
Four wave mixing in submicron waveguides
Sven Reiche UCLA ICFA-Workshop - Sardinia 07/02
Quantum One.
Chapter 3 – Combinational Logic Design
Microwave Engineering
A first step towards the P wave only modeling plan
Notes 8 ECE 6340 Intermediate EM Waves Fall 2016
Optics 430/530, week II Plane wave solution of Maxwell’s equations
Unfolding with system identification
The Method of Moments Lf = g where L is a linear operator
Chapter 3 Modeling in the Time Domain
Presentation transcript:

Multi-Resolution Homogenization of Multi-Scale Laminates: Scale Dependent Parameterization or: Homogenization procedure that retains FINITE-scale-related physics Ben Z. Steinberg School of Electrical Engineering Tel-Aviv University

URSI EMT Symp.,May Overview Multi-Resolution Homogenization – MRH –Basic Properties –Formulation Outline Extending the Role of Homogenization (use a specific example) –Keeping more Micro-Scale Information: In a Macro-scale formulation Scale-related physics (vanishes in the limit of vanishing micro-scale?) –Achieved by: Global Effective Operator Study/Correction Higher order collective effects (Back Scattering) Feynman diagrams interpretation Length-Scale Related Dispersion – Analytic results Numerical Simulation

URSI EMT Symp.,May MRH Theory Use Multi Resolution analysis and wavelets to achieve an exact decomposition of the governing formulation into a hierarchy of scales. –Define your scales (Medium properties and field observables) –Galerkin-type projection Derive exact self consistent formulation –governing only the Macro-Scale field. –Effects of Micro-Scale heterogeneity on the Macro-Scale field are expressed via the EMO. Study (neglect?) the EMO. Norm bounds and properties w/respect to: –Greens function properties origin, wavelength) –Heterogeneity properties (regularity, scale-content, size) Turn back the crank; identify structure similarity w/respect to original formulation Associate: identify new heterogeneity functions as the effective ones

URSI EMT Symp.,May An Experiment Pulse bandwidth: Micro-Scale: Initially: the filed is described on macro-scale only Micro-Scale Laminate

URSI EMT Symp.,May Later…. Micro-Scale Field Macro-Scale Fields While passing through the laminate: Undergoes distortion (slight? Negligible?) Transfers energy to small scales After it traverses the laminate: Transfers energy from small scales back to large scale Observed on Macro-Scale: Distortion + Delay (micro-scale related) Hence: Effective Dispersion, observed on Macro-Scale

URSI EMT Symp.,May Major Technical Steps The field is governed by Choose homogenization scale - the scale on which the solution is to be smoothed. Usually Cast the problem into an integral equation formulation –Bounded operator –BC are inherent in the formulation structure (kernel) Decompose into scales via MRD (i.e. Galerkin) of the integral operator:

URSI EMT Symp.,May Major Technical Steps (Cont.) The result is: Where: Formulation governing macro-scale field component: Main analytical effort: study the EMO (e.g. structure & norm bounds w/respect to physical parameters)

URSI EMT Symp.,May Scaling functions, wavelets, and their fields…

URSI EMT Symp.,May Major Results Previous MRD homogenization results are contained in [Steinberg et. al, SIAM J. Appl. Math., 60(3) 2000 pp ] Valid for periodic and non-periodic structures Allows for a continuum of scales Classical homogenization results reconstructed as special cases –EMO has been neglected (approved by norm bounds) New study: –Decompose the EMO into a hierarchy of multiple interactions –Scale-related analysis of the leading term New physics not contained in classical results: scale dependent dispersion

URSI EMT Symp.,May Decomposition of the EMO We have Invoke Neumann series representation of the EMO The leading term

URSI EMT Symp.,May For the general term: Location Scale Feynman Diagram in Location-Scale space: Scattering by h (multiplication) Propagation Interaction + Propagation

URSI EMT Symp.,May Contribution of the leading term Assume micro-scale heterogeneity Then It is known that But we want

URSI EMT Symp.,May Finally we get: However, recall the original formulation: dependencies of and combined (!):

URSI EMT Symp.,May Scale dependent dispersion: The new expression for the effective LARGE SCALE heterogeneity: Scale-related dispersion via

URSI EMT Symp.,May Numerical example Scale-dependent phase (Delay) as a signal traverses a laminate: Bragg regime Theory

URSI EMT Symp.,May Conclusions Scales = Fun ! MRH provides micro-scale-dependent parameterization of effective macro-scale formulation Effective dispersion that depends on micro-scale has been derived Micro-Scale dependent effective description of the medium is materialized on LARGE SCALES only.