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Conference on Kinetic Theory and Related Fields (Department of Mathematics, POSTECH June 22-24, 2011). 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
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Conference on Kinetic Theory and Related Fields (Department of Mathematics, POSTECH June 22-24, 2011) Decay of an oscillating disk in a gas:Case of a collision-less gas anda special Lorentz gas Kazuo Aoki Dept. of Mech. Eng. and Sci. Kyoto University (in collaboration with Tetsuro Tsuji)
Decay of an oscillating disk Gas Equation of motion of the disk : External force Drag (Hooke’s law) If , then Exponential decay Collisionless gas (Free-molecular gas, Knudsen gas) Other types of gas Decay rate ???
Collisionless gas Collisionless gas Mathematical study Decay rate Caprino, Cavallaro, & Marchioro, M3AS (07) BC:specular reflection Monotonic decay
Highly rarefied gas Collisionless gas Effect of collisions: Neglected Molecular velocity Mean free path Boltzmann equation Time-independent case parameter
Velocity distribution function position time molecular velocity Molecular mass in at time Macroscopic quantities gas const. Equation for : Boltzmann equation
Nonlinear integro-differential equation Boltzmann equation collision integral [ : omitted ] Dimensionless form: : Knudsen number
Highly rarefied gas Collisionless gas Effect of collisions: Neglected Molecular velocity Mean free path Boltzmann equation Time-independent case parameter
(Infinite domain) Initial-value problem Initial condition: Solution: (Steady) boundary-value problem Single convex body given from BC Solved! BC :
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)
Conventional boundary condition [ : omitted ] 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
Collisionless gas Mathematical study Decay rate Caprino, Cavallaro, & Marchioro, M3AS (07) BC:specular reflection Monotonic decay Guess BC:diffuse reflection, oscillatory case Numerical study
Gas: EQ: IC: BC:Diffuse reflection on body surface Body: EQ: IC:
1D case: Decay of oscillating plate gas Gas: EQ: IC: BC:Diffuse reflection on plate Plate: (unit area) EQ: left surface IC: right surface
Numerical results (decay rate) Parameters Double logarithmic plot
Numerical results (decay rate) Parameters Diffuse ref. Specular ref. Double logarithmic plot Power-law decay
Parameters If the effect of recollision is neglected… no oscillation around origin Exponential decay LONG MEMORY effect (recollision) Single logarithmic plot
(Marginal) VDF on the plate LEFT SIDE TRAJECTORY OF THE PLATE RIGHT SIDE Velocity of the plate Velocity of the plate Reflected molecules (diffuse reflection) Impinging molecules Reflected molecules (diffuse reflection) Impinging molecules recollision enlarged for a large time Initial distribution
(Marginal) VDF on the plate enlarged figure Power-law decay Long memory effect
Decay of the plate velocity Power-law decay • Decay rate of kinetic energy • is faster than potential energy • No possibility of infinitely • manyoscillations around • origin
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 (Dimensionless) EQ: IC: Knudsen number BC: Diffuse reflection mean free path EQ for the disk, … characteristic length
Randomly distributed obstacles at rest Evaporating droplets No collision between gas molecules Re-emitted Gas molecule Absorbed 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 (Dimensionless) long-memory effect EQ: IC: Knudsen number BC: Diffuse reflection mean free path EQ for the disk, … characteristic length
Very special Lorentz gas (Very toy model for gas) (Dimensionless) EQ: Previous model IC: Knudsen number BC: Diffuse reflection mean free path EQ for the disk, … characteristic length
(velocity ) Randomly distributed moving obstacles Evaporating droplets No collision between gas molecules Re-emitted Gas molecule Absorbed 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!!