Decay of an oscillating disk in a gas: Case of a collision-less gas and a special Lorentz gas Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University.

Slides:



Advertisements
Similar presentations
Pressure and Kinetic Energy
Advertisements

Lecture 4 – Kinetic Theory of Ideal Gases
Kinetic Molecular Theory 1.pertaining to motion. 2. caused by motion. 3. characterized by movement: Running and dancing are kinetic activities. ki ⋅ net.
Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University
U N C L A S S I F I E D Operated by the Los Alamos National Security, LLC for the DOE/NNSA IMPACT Project Drag coefficients of Low Earth Orbit satellites.
1 MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 7.
Thermo & Stat Mech - Spring 2006 Class 14 1 Thermodynamics and Statistical Mechanics Kinetic Theory of Gases.
1 A. Derivation of GL equations macroscopic magnetic field Several standard definitions: -Field of “external” currents -magnetization -free energy II.
2-1 Problem Solving 1. Physics  2. Approach methods
Broadwell Model in a Thin Channel Peter Smereka Collaborators:Andrew Christlieb James Rossmanith Affiliation:University of Michigan Mathematics Department.
Introduction to Convection: Flow and Thermal Considerations
Thermo & Stat Mech - Spring 2006 Class 15 1 Thermodynamics and Statistical Mechanics Transport Processes.
Slip to No-slip in Viscous Fluid Flows
5. Simplified Transport Equations We want to derive two fundamental transport properties, diffusion and viscosity. Unable to handle the 13-moment system.
Viscosity. Average Speed The Maxwell-Boltzmann distribution is a function of the particle speed. The average speed follows from integration.  Spherical.
CHAPTER 8 APPROXIMATE SOLUTIONS THE INTEGRAL METHOD
Introduction to Convection: Flow and Thermal Considerations
CHAPTER 7 NON-LINEAR CONDUCTION PROBLEMS
Chapter 13: Temperature and Ideal Gas
Chapter 5 Diffusion and resistivity
Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras Advanced Transport Phenomena Module 2 Lecture 4 Conservation Principles: Mass Conservation.
Boundary-value problems of the Boltzmann equation: Asymptotic and numerical analyses (Part 1) Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University.
KINETIC THEORY AND MICRO/NANOFLUDICS
Kemerovo State University(Russia) Mathematical Modeling of Large Forest Fires Valeriy A. Perminov
Anharmonic Effects. Any real crystal resists compression to a smaller volume than its equilibrium value more strongly than expansion to a larger volume.
Chapter 21: Molecules in motion
Chapter 21: Molecules in motion Diffusion: the migration of matter down a concentration gradient. Thermal conduction: the migration of energy down a temperature.
Prof. dr. A. Achterberg, Astronomical Dept., IMAPP, Radboud Universiteit.
Yoon kichul Department of Mechanical Engineering Seoul National University Multi-scale Heat Conduction.
Gas-kinetic schemes for flow computations Kun Xu Mathematics Department Hong Kong University of Science and Technology.
CHAPTER 3 EXACT ONE-DIMENSIONAL SOLUTIONS 3.1 Introduction  Temperature solution depends on velocity  Velocity is governed by non-linear Navier-Stokes.
2. Brownian Motion 1.Historical Background 2.Characteristic Scales Of Brownian Motion 3.Random Walk 4.Brownian Motion, Random Force And Friction: The Langevin.
Convection - Heat transfer in a gas or liquid by the circulation of currents from one region to another. Can be forced or spontaneous (natural). Hot and.
ELECTRON THEORY OF METALS 1.Introduction: The electron theory has been developed in three stages: Stage 1.:- The Classical Free Electron Theory : Drude.
Chapter 8. FILTRATION PART II. Filtration variables, filtration mechanisms.
FREE CONVECTION 7.1 Introduction Solar collectors Pipes Ducts Electronic packages Walls and windows 7.2 Features and Parameters of Free Convection (1)
Convection in Flat Plate Boundary Layers P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A Universal Similarity Law ……
Free electron theory of Metals
Quantification of the Infection & its Effect on Mean Fow.... P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Modeling of Turbulent.
Chapter 16 Kinetic Theory of Gases. Ideal gas model 2 1. Large number of molecules moving in random directions with random speeds. 2. The average separation.
Stokes fluid dynamics for a vapor-gas mixture derived from kinetic theory Kazuo Aoki Department of Mechanical Engineering and Science Kyoto University,
Compressible Frictional Flow Past Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Small and Significant Region of Curse.
INTRODUCTION TO CONVECTION
Lecture 3. Full statistical description of the system of N particles is given by the many particle distribution function: in the phase space of 6N dimensions.
Tutorial/HW Week #7 WRF Chapters 22-23; WWWR Chapters ID Chapter 14
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2
Boundary-value problems of the Boltzmann equation: Asymptotic and numerical analyses (Part 2) Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University.
Kinetic Molecular Theory 1.pertaining to motion. 2. caused by motion. 3. characterized by movement: Running and dancing are kinetic activities. ki ⋅ net.
Nuclear Reactors, BAU, 1st Semester, (Saed Dababneh).
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2 Tutorial #1 WRF#14.12, WWWR #15.26, WRF#14.1, WWWR#15.2, WWWR#15.3, WRF#15.1, WWWR.
Fundamental (First) Principles of Fluid Mechanics
An Unified Analysis of Macro & Micro Flow Systems… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Wall Bound Flows.
An Unified Analysis of Macro & Micro Flow Systems… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Slip to No-slip in Viscous Fluid.
Equilibrium and Stability
Equation of Continuity
Diffusion over potential barriers with colored noise
Chapter 2: Introduction to Conduction
HW/Tutorial # 1 WRF Chapters 14-15; WWWR Chapters ID Chapters 1-2
Maxwell-Boltzmann velocity distribution
Kinetic Theory PHYS 4315 R. S. Rubins, Fall 2009.
5. Conductors and dielectrics
Extended Surface Heat Transfer
Kinetic Theory PHYS 4315 R. S. Rubins, Fall 2009.
Fundamentals of Heat Transfer
Maxwell-Boltzmann velocity distribution
Theory and numerical approach in kinetic theory of gases (Part 1)
Theory and numerical approach in kinetic theory of gases (Part 3)
Shock wave structure for polyatomic gas with large bulk viscosity
COMBUSTION TA : Donggi Lee PROF. SEUNG WOOK BAEK
Fundamentals of Heat Transfer
Presentation transcript:

Decay of an oscillating disk in a gas: Case of a collision-less gas and a special Lorentz gas Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University (in collaboration with Tetsuro Tsuji) Conference on Kinetic Theory and Related Fields (Department of Mathematics, POSTECH June 22-24, 2011)

Decay of an oscillating disk If, then Equation of motion of the disk : Exponential decay Collisionless gas (Free-molecular gas, Knudsen gas) Other types of gas External force Drag (Hookes law) Gas Decay rate ???

Decay rate Mathematical study Caprino, Cavallaro, & Marchioro, M 3 AS (07) Monotonic decay BC: specular reflection Collisionless gas

Time-independent case parameter Collisionless gas Boltzmann equation Highly rarefied gas Effect of collisions: Neglected Molecular velocity Mean free path

Velocity distribution function time position molecular velocity Macroscopic quantities Molecular mass in at time gas const. Equation for : Boltzmann equation

collision integral Boltzmann equation Nonlinear integro-differential equation [ : omitted ] Dimensionless form: : Knudsen number

Time-independent case parameter Collisionless gas Boltzmann equation Highly rarefied gas Effect of collisions: Neglected Molecular velocity Mean free path

Initial-value problem (Infinite domain) Initial condition: Solution: (Steady) boundary-value problem Single convex body given from BC BC : Solved!

General boundary BC Integral equation for Diffuse reflection: Maxwell type: Integral equation for Exact solution! Sone, J. Mec. Theor. Appl. (84,85) General situation, effect of boundary temperature Y. Sone, Molecular Gas Dynamics: Theory, Techniques, and Applications (Birkhäuser, 2007)

[ : omitted ] Conventional boundary condition Specular reflection Diffuse reflection No net mass flux across the boundary

Maxwell type Accommodation coefficient Cercignani-Lampis model Cercignani, Lampis, TTSP (72) Initial and boundary-value problem

Decay rate Mathematical study Caprino, Cavallaro, & Marchioro, M 3 AS (07) Monotonic decay BC: specular reflection Guess BC: diffuse reflection, oscillatory case Numerical study Collisionless gas

Gas: EQ: IC: BC: Diffuse reflection on body surface Body: EQ: IC:

Gas: EQ: IC: BC: Diffuse reflection on plate Plate: EQ: IC: gas (unit area) left surface right surface 1D case: Decay of oscillating plate

Numerical results (decay rate) Parameters Double logarithmic plot

Parameters Numerical results (decay rate) Double logarithmic plot Power-law decay Diffuse ref. Specular ref.

LONG MEMORY effect (recollision) Single logarithmic plot If the effect of recollision is neglected… Parameters Exponential decay no oscillation around origin

Impinging molecules Reflected molecules (diffuse reflection ) Impinging molecules Initial distribution LEFT SIDERIGHT SIDE TRAJECTORY OF THE PLATE Reflected molecules (diffuse reflection) Velocity of the plate Velocity of the plate recollision enlarged for a large time (Marginal) VDF on the plate

Power-law decay enlarged figure Long memory effect (Marginal) VDF on the plate

Power-law decay Decay rate of kinetic energy is faster than potential energy No possibility of infinitely many oscillations around origin Decay of the plate velocity

Power-law decay

Density

2D & 3D cases Disk (diameter, without thickness) [Axisymmetric]

Numerical evidence for ( BC: diffuse reflection, non small )

Special Lorentz gas(Toy model for gas) Gas molecules: Interaction with background Destruction of long-memory effect EQ: IC: (Dimensionless) BC: Diffuse reflection EQ for the disk, … Knudsen number mean free path characteristic length

Randomly distributed obstacles at rest Re-emitted Absorbed Evaporating droplets No collision between gas molecules Gas molecule Mean free path Number density Saturated state

Collisionless gas Toy model Independent of Algebraic decay!

Collisionless gas Toy model Independent of Algebraic decay!

Special Lorentz gas(Toy model for gas) Gas molecules: Interaction with background Destruction of long-memory effect EQ: IC: (Dimensionless) BC: Diffuse reflection EQ for the disk, … Knudsen number mean free path characteristic length long-memory effect

Very special Lorentz gas(Very toy model for gas) EQ: IC: (Dimensionless) BC: Diffuse reflection EQ for the disk, … Knudsen number mean free path characteristic length Previous model

Randomly distributed moving obstacles Re-emitted Absorbed Evaporating droplets No collision between gas molecules Gas molecule (velocity ) Obstacles: Maxwellian

Collisionless gas Toy model 1 Toy model 2 Exponential decay!!

Collisionless gas Toy model 1 Toy model 2 Exponential decay!!

Collisionless gas Toy model 1 Toy model 2 Exponential decay!!