Construction of Green's functions for the Boltzmann equations Shih-Hsien Yu Department of Mathematics National University of Singapore.

Slides:



Advertisements
Similar presentations
Response of shear flows to external disturbances Contents: 1. Acoustic receptivity of laminar separating boundary layer 2. Acoustic receptivity of laminar.
Advertisements

Finite Difference Discretization of Hyperbolic Equations: Linear Problems Lectures 8, 9 and 10.
P.W. Terry K.W. Smith University of Wisconsin-Madison Outline
Method of Generalized Separation of Variables
Waves and Solitons in Multi-component Self-gravitating Systems
Signal Processing in the Discrete Time Domain Microprocessor Applications (MEE4033) Sogang University Department of Mechanical Engineering.
5/4/2015rew Accuracy increase in FDTD using two sets of staggered grids E. Shcherbakov May 9, 2006.
MULTISCALE COMPUTATIONAL METHODS Achi Brandt The Weizmann Institute of Science UCLA
Dynamics of nonlinear parabolic equations with cosymmetry Vyacheslav G. Tsybulin Southern Federal University Russia Joint work with: Kurt Frischmuth Department.
Aspects of Conditional Simulation and estimation of hydraulic conductivity in coastal aquifers" Luit Jan Slooten.
LMS Durham Symposium Dynamical Systems and Statistical Mechanics 3 – 13 July 2006 Locating periodic orbits in high-dimensional systems by stabilising transformations.
Landscape Erosion Kirsten Meeker
A Concept of Environmental Forecasting and Variational Organization of Modeling Technology Vladimir Penenko Institute of Computational Mathematics and.
Network and Grid Computing –Modeling, Algorithms, and Software Mo Mu Joint work with Xiao Hong Zhu, Falcon Siu.
Coarse Bifurcation Studies of Alternative Microscopic/Hybrid Simulators C. Theodoropoulos and I.G. Kevrekidis in collaboration with K. Sankaranarayanan.
Computations of Fluid Dynamics using the Interface Tracking Method Zhiliang Xu Department of Mathematics University of Notre.
Analysis of Blade Performance in Compressible Flows P M V Subbarao Professor Mechanical Engineering Department Enhanced Effects due to Flow with Snestive.
Duffing Oscillator.
Multiscale transforms : wavelets, ridgelets, curvelets, etc.
Ring Car Following Models by Sharon Gibson and Mark McCartney School of Computing & Mathematics, University of Ulster at Jordanstown.
Hybrid WENO-FD and RKDG Method for Hyperbolic Conservation Laws
August, 1999A.J. Devaney Stanford Lectures-- Lecture I 1 Introduction to Inverse Scattering Theory Anthony J. Devaney Department of Electrical and Computer.
Wave-Particle Interaction in Collisionless Plasmas: Resonance and Trapping Zhihong Lin Department of Physics & Astronomy University of California, Irvine.
Australian Journal of Basic and Applied Sciences, 5(11): , 2011 ISSN Monte Carlo Optimization to Solve a Two-Dimensional Inverse Heat.
60th Annual Meeting Division of Fluid Dynamics A multiscale approach to study the stability of long waves in near-parallel flows S. Scarsoglio #, D.Tordella.
Supergranulation Waves in the Subsurface Shear Layer Cristina Green Alexander Kosovichev Stanford University.
Simon Weber PhD student of Martin Hairer Warwick Mathematics Institute
AMS 691 Special Topics in Applied Mathematics Lecture 3 James Glimm Department of Applied Mathematics and Statistics, Stony Brook University Brookhaven.
1 Linear Stability of Detonations with Reversible Chemical Reactions Shannon Browne Graduate Aeronautical Laboratories California Institute of Technology.
Chapter 3 mathematical Modeling of Dynamic Systems
LBM: Approximate Invariant Manifolds and Stability Alexander Gorban (Leicester) Tuesday 07 September 2010, 16:50-17:30 Seminar Room 1, Newton Institute.
1 Heat Conduction in One- Dimensional Systems: molecular dynamics and mode-coupling theory Jian-Sheng Wang National University of Singapore.
Numerical Investigation into Potential Flow Around High-speed Hydrofoil Assisted Craft ZHONGYU YANG supervised by Prof G.E HEARN and.
7. Introduction to the numerical integration of PDE. As an example, we consider the following PDE with one variable; Finite difference method is one of.
Prabhakar.G.Vaidya and Swarnali Majumder A preliminary investigation of the feasibility of using SVD and algebraic topology to study dynamics on a manifold.
The Stability of Laminar Flows - 2
Numerical methods 1 An Introduction to Numerical Methods For Weather Prediction by Mariano Hortal office 122.
Feedback Stabilization of Nonlinear Singularly Perturbed Systems MENG Bo JING Yuanwei SHEN Chao College of Information Science and Engineering, Northeastern.
Stokes fluid dynamics for a vapor-gas mixture derived from kinetic theory Kazuo Aoki Department of Mechanical Engineering and Science Kyoto University,
AMS 691 Special Topics in Applied Mathematics Lecture 3
Math 445: Applied PDEs: models, problems, methods D. Gurarie.
Arrival time variations of pulses in shallow water and low frequency acoustical underwater positioning B.Katsnelson (Voronezh Uni, Russia) M.Badiey (Uni.
Family of Functions, review Which functions are nonlinear? Select all that apply.
11/22/2013PHY 711 Fall Lecture 341 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 34: Chapter 11.
10//3015PHY 711 Fall Lecture 261 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 26: Chap. 9 of.
Stability Investigation of a Difference Scheme for Incompressible Navier—Stokes Equations D. Chibisov, V. Ganzha, E.W. Mayr, E.V. Vorozhtsov.
CLASSIFICATION OF ECG SIGNAL USING WAVELET ANALYSIS
Non-local Transport of Strongly Coupled Plasmas Satoshi Hamaguchi, Tomoyasu Saigo, and August Wierling Department of Fundamental Energy Science, Kyoto.
Response of an Elastic Half Space to an Arbitrary 3-D Vector Body Force Smith and Sandwell, JGR 2003 Develop the three differential equations relating.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
Int’l Workshop on SDE TT
I- Computational Fluid Dynamics (CFD-I)
Dynamics & Mass transfer modelling Application Observations
PHY 711 Classical Mechanics and Mathematical Methods
Convergence in Computational Science
Introduction to Partial Differential Equations
Introduction to Multigrid Method
ESS 154/200C Lecture 19 Waves in Plasmas 2
Numerical Model of a PDRE
Modeling in the Time Domain
Adaptive Perturbation Theory: QM and Field Theory
Announcements 3/23/12 Prayer
Shock wave structure for polyatomic gas with large bulk viscosity
PHY 711 Classical Mechanics and Mathematical Methods
SPACE TIME Fourier transform in time Fourier transform in space.
PHY 711 Classical Mechanics and Mathematical Methods
Wave Propagation Over a Boltzmann Shock Profile
Partial Differential Equations and Applied Mathematics Seminar
Andrey Il’ichev Steklov Mathematical Institute, Moscow George Tsypkin
AC modeling of converters containing resonant switches
Presentation transcript:

Construction of Green's functions for the Boltzmann equations Shih-Hsien Yu Department of Mathematics National University of Singapore

Motivation to investigate Green’s function for Boltzmann equation before 2003 Nonlinear time-asymptotic stability of a Boltzmann shock profile Zero total macroscopic perturbations Nonlinear time-asymptotic stability of a Knudsen layer for the Boltzmann Equation Mach number <-1

Green’s function of linearized equation around a global Maxwellian, Fourier transformation The inverse transformation

Initial value problem Particle-like wave-like decomposition

Pointwise of structure of the Green’s function Space dimension=3 Space dimension=1

Macroscopic wave structure of 1-D Green’s function Application: Pointwise time-asymptotic stability of a global Maxwellian state in 1-D.

Green’s function of linearized equation around a global Maxwellian M,, in a half-space problem x>0. Green identity: Boundary value estimates ( a priori estimate):

Approximate boundary data for case |Mach(M)|<1 Upwind damping approximation to the boundary data

An approximation to the full boundary data.

Green’s function of linearized equation around a stationary shock profile.

Separation of wave structures Transversal wave Compressive wave

1. Shift data

2. Hyperbolic Decomposition Transversal wave Compressive wave 3. Transverse Operator and Local Wave Front tracing

4. Coupling of T and D operators 5. Respond to Coupling

6. Approximation to Respond, Compressive Operator

6. T-C scheme for An estimates

A Diagram for A Diagram for general pattern + extra time decaying rate in microscopic component nonlinear stability of Boltzmann shock profile

Applications of the Green’s functions Nonlinear invariant manifolds for steady Boltzmann flow

Applications of the Green’s functions Milne’s problme

Sone’s Diagram for Condensation-Evaporation