
Numerical Analysis of Multiscale Computations
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This book is a snapshot of current research in multiscale modeling, computations and applications. It covers fundamental mathematical theory, numerical algorithms as well as practical computational advice for analysing single and multiphysics models containing a variety of scales in time and space. Complex fluids, porous media flow and oscillatory dynamical systems are treated in some extra depth, as well as tools like analytical and numerical homogenization, and fast multipole method.
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Content
- Intro
- Numerical Analysis of Multiscale Computations
- Preface
- Acknowledgements
- Contents
- Explicit Methods for Stiff Stochastic Differential Equations
- 1 Introduction
- 2 Stiff Stochastic Systems and Stability
- 3 Chebyshev Methods
- 4 The S-ROCK Methods
- 4.1 Construction of the S-ROCK Methods
- 4.2 Accuracy of the S-ROCK Methods
- 5 Extended Mean-Square Stability and Damping
- 6 Numerical Illustrations
- References
- Oscillatory Systems with Three Separated Time Scales:Analysis and Computation
- 1 Introduction
- 2 Effective Behavior Across Different Time Scales
- 2.1 Slowly Changing Quantities
- 2.2 Multiscale Charts
- 3 A Homogenization Approach
- 3.1 A Two Scales Example
- 3.2 Three Scales: Example 1
- 3.3 Three Scales: Example 2
- 3.4 Observations
- 4 Numerical Algorithms
- 4.1 Accuracy and Efficiency
- 5 Examples
- 5.1 Harmonic Oscillators
- 5.2 An Example Motivated by the Fermi-Pasta-Ulam (FPU) Problem
- 6 Summary
- References
- Variance Reduction in Stochastic Homogenization: The Technique of Antithetic Variables
- 1 Introduction
- 1.1 Homogenization Theoretical Setting
- 1.2 Numerical Approach
- 1.3 The Technique of Antithetic Variables
- 1.4 A Brief Summary of Our Former Results
- 2 Variance Reduction for Problems Involving Correlations or Anisotropy
- 2.1 Correlated Cases
- 2.1.1 Influence of Correlation: Identical Local Behaviour
- 2.1.2 Centered vs Equidistributed Correlation Structure
- 2.1.3 Longer Correlation Lengths
- 2.2 Anisotropic Cases
- 2.2.1 Test Cases
- 2.2.2 Numerical Results
- 3 Variance Reduction for Eigenproblems
- References
- A Stroboscopic Numerical Method for HighlyOscillatory Problems
- 1 Introduction
- 2 A Modified Equation Approach to Averaging
- 3 A Numerical Method
- 4 Examples
- 5 Numerical Experiments
- 5.1 Constant Step-Sizes
- 5.2 Variable Step-Sizes
- References
- The Microscopic Origin of the Macroscopic Dielectric Permittivity of Crystals: A Mathematical Viewpoint
- 1 Introduction
- 2 Electronic Structure Models for Finite Systems
- 2.1 The N-Body Schrödinger Model
- 2.2 The N-Body Schrödinger Model for Non-interacting Electrons
- 2.3 Density Operators
- 2.4 The Hartree Model and Other Density Operator Models of Electronic Structures
- 3 The Hartree Model for Crystals
- 3.1 Basics of Fourier and Bloch-Floquet Theories
- 3.2 Perfect Crystals
- 3.3 Crystals with Local Defects
- 4 Dielectric Response of a Crystal
- 4.1 Series Expansion of the Time-Independent Response
- 4.2 Properties of Qm,0F and m,0F for Small Amplitude Defects
- 4.3 Dielectric Operator and Macroscopic DielectricPermittivity
- 4.4 Time-Dependent Response
- References
- Fast Multipole Method Using the Cauchy Integral Formula
- 1 Introduction
- 2 Cauchy's Integral Formula and Low-Rank Approximations
- 3 Connection with Fourier and Laplace Transforms
- 4 Construction of Fast Methods
- 5 Interpolation and Anterpolation
- 6 Error Analysis
- 7 Detailed Error Analysis
- 8 Preliminary Numerical Results
- 9 Conclusion
- References
- Tools for Multiscale Simulation of Liquids Using Open Molecular Dynamics
- 1 Introduction
- 2 Open MD: Molecular Dynamics for Open Systems
- 2.1 Open MD Setup
- 2.2 Imposition of the Macro-State
- 2.2.1 State-Coupling Based on Constrained Dynamics
- 2.2.2 The Flux-Based Scheme
- 2.3 Mass and Density Profile at the Buffer
- 2.3.1 Distribution of the External Force
- 2.3.2 The Buffer Mass: Particle Insertion and Deletion
- 3 Using Adaptive Resolution: The Mesoscopic Interface
- 4 HybridMD: Particle-Continuum Hybrid Scheme
- 4.1 Time Coupling
- 4.2 Hybrids Based on State Coupling
- 4.3 Hybrids Based on Flux Exchange
- 4.4 Mass Transfer and Continuity in Flux Based Schemes
- 5 Conclusions and Perspectives
- References
- Multiscale Methods for Wave Propagation in Heterogeneous Media Over Long Time
- 1 Introduction
- 2 HMM for the Wave Equation and Finite Time
- 2.1 One Numerical Example
- 3 HMM for the Wave Equation over Long Time
- 3.1 The HMM Algorithm for Long Time
- 3.2 A Long Time Computation with HMM
- 3.3 Non-periodic Material
- 3.4 Theory
- 3.5 Stability Analysis of the Macro Scheme for the Long Time Effective Equation
- 4 Conclusions
- References
- Numerical Homogenization via Approximation of the SolutionOperator
- 1 Introduction
- 1.1 Background
- 1.2 Mathematical Problem Formulation
- 1.3 Coarse-Graining of the Differential Operator (Homogenization)
- 1.4 Coarse-Graining of the Solution Operator
- 2 Data-Sparse Matrices
- 3 Case Study: A Discrete Laplace Equation on a Square
- 3.1 Problem Formulation
- 3.2 Model Problems
- 3.3 Compressibility of the Solution Operator
- 3.4 Techniques for Computing the Solution OperatorThat Fully Resolve the Micro-Structure
- 3.5 Techniques Accelerated by Collecting Statisticsfrom a Representative Volume Element
- 3.6 Fusing a Homogenized Model to a Locally FullyResolved Region
- 4 Case Study: Two-Phase Media
- 5 Generalizations
- 6 Conclusions
- References
- Adaptive Multilevel Monte Carlo Simulation
- 1 Introduction
- 1.1 A Single Level Posteriori Error Expansion
- 2 Adaptive Algorithms and MultilevelVariance Reduction
- 3 A Stopped Diffusion Example
- References
- Coupled Coarse Graining and Markov Chain Monte Carlofor Lattice Systems
- 1 Introduction
- 2 MCMC Methods
- 2.1 Mixing Times and Speed of Convergence
- 3 The Coupled CGMC Method
- 3.1 The Algorithm
- 3.2 The Rate of Convergence
- 4 Extended Lattice Systems
- 4.1 Coarse-Graining of Microscopic Systems
- 4.2 Multiscale Decomposition and Splitting Methods for MCMC
- 4.3 Microscopic Reconstruction
- 5 Example: Short and Long-Range Interactions
- 6 Conclusions
- References
- Calibration of a Jump-Diffusion Process Using Optimal Control
- 1 Introduction
- 2 The Forward Equation
- 3 The Optimal Control Problem
- 4 Reconstructing the Volatility Surface and Jump Intensity
- 4.1 The Hamiltonian System
- 4.2 Discretization
- 4.3 The Newton Method
- 5 Numerical Examples
- 5.1 Artificial Data No Jumps
- 5.2 Artificial Data with Jumps
- 5.3 Real Data
- References
- Some Remarks on Free Energy and Coarse-Graining
- 1 Motivation
- 1.1 Coarse-Graining of Thermodynamic Quantities
- 1.2 Coarse-Graining of Dynamical Quantities
- 1.3 Outline of the Article
- 1.4 Notation
- 2 Computing Macroscopic Stress-Strain Relationsfor One-Dimensional Chains of Atoms
- 2.1 The Nearest Neighbour (NN) Case
- 2.1.1 Computing the Strain for a Given Stress
- 2.1.2 Computing the Stress for a Given Strain
- 2.1.3 Equivalence of Stress-Strain Relations in the Thermodynamic Limit
- 2.2 The Next-to-Nearest Neighbour (NNN) Case
- 2.2.1 Computing the Strain for a Given Stress
- 2.2.2 Computing the Stress for a Given Strain
- 2.2.3 Equivalence of Stress-Strain Relations in the Thermodynamic Limit
- 2.2.4 Numerical Computation of F' and Comparison with the Zero Temperature Model
- 3 A Coarse-Graining Procedure in the Dynamical Setting
- 3.1 Measuring Distances Between Probability Measures
- 3.2 Effective Dynamics
- 3.3 The Proof in a Simple Two-Dimensional Case
- 3.4 Numerical Results
- 3.4.1 A Three Atom Molecule
- 3.4.2 The Butane Molecule Case
- References
- Linear Stationary Iterative Methods for the Force-Based Quasicontinuum Approximation
- 1 Introduction
- 2 The QC Approximations and Their Stability
- 2.1 Function Spaces and Norms
- 2.2 The Atomistic Model
- 2.2.1 The Critical Strain F*
- 2.3 The Local QC Approximation (QCL)
- 2.4 The Force-Based QC Approximation (QCF)
- 2.5 The Original Energy-Based QCApproximation (QCE)
- 2.6 The Quasi-Nonlocal QC Approximation (QNL)
- 3 Stability and Spectrum of the QCF operator
- 3.1 Spectral Properties of LqcfF in U0,2=l2e
- 3.2 Spectral Properties of LqcfF in U1,2
- 4 Linear Stationary Iterative Methods
- 5 The Richardson Iteration (P=I)
- 5.1 Numerical Example for the Richardson Iteration
- 6 Preconditioning with QCL (P=LqclF=AF L)
- 6.1 Analysis of the QCL Preconditioner in U2,8
- 6.2 Analysis of the QCL Preconditioner in U1,8
- 6.3 Analysis of the QCL Preconditioner in U1,2
- 6.4 Numerical Example for QCL-Preconditioning
- 7 Preconditioning with QCE (P=LqceF): Ghost-ForceCorrection
- References
- Analysis of an Averaging Operator for Atomic-to-ContinuumCoupling Methods by the Arlequin Approach
- 1 Introduction
- 2 Particle and Continuum Model Problems
- 2.1 Particle Model
- 2.2 Continuum Model
- 2.3 Calibration of Continuum Model
- 3 Coupling Method with Averaging Operator
- 3.1 Energy of the Coupled System
- 3.2 Averaging Coupling Operator
- 3.3 Formulation of the Coupled Problem
- 4 Mathematical Analysis of the Coupling Method
- 5 Finite Element Formulation
- 6 Numerical Results
- 6.1 One-Dimensional Numerical Results
- 6.1.1 Overlap Region Composed of One RVE
- 6.1.2 Overlap Region Composed of Several RVE's
- 6.1.3 An Example with a Large Number of Particles
- 6.1.4 Simulation of a Defect
- 6.2 Two-Dimensional Numerical Results
- 7 Conclusion
- References
- A Coupled Finite Difference - Gaussian Beam Method for High Frequency Wave Propagation
- 1 Introduction
- 2 Gaussian Beams
- 3 Motivating Examples
- 4 Local Finite Difference Method
- 5 Hybrid Method
- 5.1 Example: Double Slit Experiment
- 5.2 Example: Sound Speed with Inclusion
- 6 Conclusion
- References
- Editorial Policy
- Lecture Notes in Computational Science and Engineering
- Monographs in Computational Science and Engineering
- Texts in Computational Science and Engineering
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