GAČR Grant no. 102/08/H081 “Nonstandard application of physical fields” Arindam SARKAR Jiří Chvojka A David LUKÁŠ.

Slides:



Advertisements
Similar presentations
Stellar Structure Section 2: Dynamical Structure Lecture 2 – Hydrostatic equilibrium Mass conservation Dynamical timescale Is a star solid, liquid or gas?
Advertisements

Technical University of Liberec
Colloid Stability ?.
WAVES.
Enclosure Fire Dynamics
Mechanical Waves.
Chapter 15 - Waves Traveling Waves –Types –Classification –Harmonic Waves –Definitions –Direction of Travel Speed of Waves Energy of a Wave Standing Waves.
Torsion  Introduction -- Analyzing the stresses and strains in machine parts which are subjected to torque T Circular -- Cross-section Non-circular.
Seismic Wave Demonstrations and Animations L. Braile, Purdue University  Copyright L. Braile. Permission.
Seismic Wave Demonstrations and Animations L. Braile, Purdue University  Copyright L. Braile. Permission.
6.2C Volumes by Slicing with Known Cross-Sections.
Chapter 3 Torsion Introduction -- Analyzing the stresses and strains in machine parts which are subjected to torque T Circular -- Cross-section Non-circular.
1 Wave turbulence in resonators Elena Kartashova, RISC , Physical Colloquium.
Two-particle Distribution and Correlation in Hot QGP Hui Liu (刘绘) Phys. Dep., JiNan University Jiarong Li (李家荣) IOPP, CCNU Outline: Brief review on distribution.
Copyright 2005 by Nelson, a division of Thomson Canada Limited FIGURES FOR CHAPTER 3 TORSION Click the mouse or use the arrow keys to move to the next.
1 3D Simulations for the Elliptic Jet W. Bo (Aug 12, 2009) Parameters: Length = 8cm Elliptic jet: Major radius = 0.8cm, Minor radius = 0.3cm Striganov’s.
PHYS 218 sec Review Chap. 15 Mechanical Waves.
Internal Flow: Mass Transfer Chapter 8 Section 8.9.
Waves Traveling Waves –Types –Classification –Harmonic Waves –Definitions –Direction of Travel Speed of Waves Energy of a Wave.
Physical principles of nanofiber production 7
ChE 452 Lecture 24 Reactions As Collisions 1. According To Collision Theory 2 (Equation 7.10)
Physical principles of nanofiber production Theoretical background (3) Electrical bi-layer D. Lukáš
Scattering by particles
DISLOCATION DYNAMICS STUDIES OF DISLOCATION INTERACTION IN MULTILAYERS UROP 03 – STAGE II PRESENTATION by Rajlakshmi Purkayastha ( ) under the.
Instabilities of Electrically Forced Jets Moses Hohman (Univ. of Chicago Thoughtworks) Michael Shin (Materials Science, MIT) Greg Rutledge (Chemical Engineering,
Mechanics of Materials – MAE 243 (Section 002) Spring 2008
Specific Heat of Solids Quantum Size Effect on the Specific Heat Electrical and Thermal Conductivities of Solids Thermoelectricity Classical Size Effect.
Matter & Energy pg Today’s LO: I can convert temperatures between different temperature scales.
Warm Up. Volume of Solids - 8.3A Big Idea Just like we estimate area by drawing rectangles, we can estimate volume by cutting the shape into slices,
Free Electron Lasers (I)
Practical Statistics for Particle Physicists Lecture 3 Harrison B. Prosper Florida State University European School of High-Energy Physics Anjou, France.
Simulation of Muon Collider Target Experiments Yarema Prykarpatskyy Center for Data Intensive Computing Brookhaven National Laboratory U.S. Department.
LATTICE BOLTZMANN SIMULATIONS OF COMPLEX FLUIDS Julia Yeomans Rudolph Peierls Centre for Theoretical Physics University of Oxford.
Chapter 7 Atomic Structure & Periodicity. Electromagnetic Radiation O Waves (wavelength, frequency & speed) O  c (page 342: #39) O Hertz O Max Planck.
Physical principles of nanofiber production 1
© Crown copyright Met Office Radiation scheme for Earth’s atmosphere …and what might not work for exoplanets James Manners 6/12/11.
1 PHY Lecture 5 Interaction of solar radiation and the atmosphere.
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
IE 300, Fall 2012 Richard Sowers IESE. 8/30/2012 Goals: Rules of Probability Counting Equally likely Some examples.
1 Physical principles of nanofiber production 6. Electric pressure and liquid body disintegration D.Lukáš 2010.
Get a computer then answer the following question. What is the difference between a convergent, divergent, and transform plate movements.
Rayleigh-Plateau Instability Rachel and Jenna. Overview Introduction to Problem Introduction to Problem Experiment and Data Experiment and Data Theories.
Applications of Ampere’s Law
Computational Mechanics JASS 2006 Survey of Wave Types and Characteristics Longitudinal Waves (For reminding only)  Pure longitudinal waves  Quasi-longitudinal.
Modelling Spray Impingement
Waves 1 Wave Basics. WAVE Disturbance that transfers energy from one place to another. Medium: __________________________________ __________________________________________.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2004, BNL Target Simulations Roman Samulyak in collaboration with Y.
Melting Solid  Liquid Energy is added, particles speed up (endothermic) Melting Point: Temp. at which a substance melts Freezing Liquid  Solid Energy.
CHAPTER 9 Velocity Profiles for Circular Sections and Flow in Noncircular Sections.
Introduction The objective of simulation – Analysis the system (Model) Analytically the model – a description of some system intended to predict the behavior.
Simulation of High-Power Mercury Jet Targets for Neutrino Factory and Muon Collider R. Samulyak, 1,2 H.C. Chen, 1 H.G. Kirk, 2 K.T. McDonald 3 1 Stony.
Date of download: 6/21/2016 Copyright © ASME. All rights reserved. From: Mechanics of Random Discontinuous Long-Fiber Thermoplastics—Part I: Generation.
Mathematics to Innovate Blade Profile P M V Subbarao Professor Mechanical Engineering Department Also a Fluid Device, Which abridged the Globe into Global.
Coherent THz radiation source driven by pre-bunched electron beam
Lecture 8: Stellar Atmosphere
Date of download: 7/7/2016 Copyright © ASME. All rights reserved. From: Energy Conservative Dissipative Particle Dynamics Simulation of Natural Convection.
The Tayler instability in stably-stratified stars and a differential- rotation-driven dynamo Jon Braithwaite CITA, Toronto.
Fyzikální principy tvorby nanovláken 1. Hladinové zvlákňování
11.1 Polar Coordinates.
Date of download: 11/4/2017 Copyright © ASME. All rights reserved.
Psychology 202a Advanced Psychological Statistics
Production of an S(α,β) Covariance Matrix with a Monte Carlo-Generated
Hamiltonian formalism, seismic waves, and seismic barriers
Light Waves and Polarization
CURVE SKETCHING PRECALC1 (Analytical Geometry).
Invention of Geometries to Generate Lift
Water and Backbone Dynamics in a Hydrated Protein
Section 2.3 Pictures of Data
Unit 3: The Dynamic Earth
Cross Cutting Concepts
Presentation transcript:

GAČR Grant no. 102/08/H081 “Nonstandard application of physical fields” Arindam SARKAR Jiří Chvojka A David LUKÁŠ

Journal of Statistical Physics Auto-model based computer simulation of Rayleigh Instability (A.S.) has been supported by GACR Grant no. 102/08/H081 “Nonstandard application of physical fields”.

Dispersion relation Dispersion law for the Rayleigh instability plots dimensionless angular frequency against the dimensionless wave-number.

Auto-model (a) The original longitudinal and cross sectional configurations of the liquid coated fibre. (b) Detailed cross-sectional shape of the original liquid layer on a fibre and the liquid nodes distribution along the fibre axis after the detachment into individual unduloids at the time of MCSPS=20,000.

Dynamics of Rayleigh instability The time versus the droplet numbers for (a) the liquid coating the fibre; (b) the pure liquid jet. Unduloids on the fibre merge and those, which disappeared, are marked in grey.

Time versus the droplet numbers The time versus the droplet numbers for the system of liquid coating fibre with the original cross-section sketched. (a) the droplet numbers n ~ MCSPS; (b) ln(n) versus MCSPS with a regression result.

Outputs The Rayleigh wavelength l versus the original radius r o as predicted by the analytical theory (solid line) and by the computer simulations (points). (a) is for pure liquid jet and (b) for liquid coating a fibre.

Hammersley and Clifford theorem Markov random field

Clans and clan functions g Bayes’ rule

Clan functions and marginal pobabilitioes

Energy function, Hamiltonian and exchange energies Interaction energies E(x i,x j ) in [e.u.] Gas x i = 0Liquid x i = 1Fiber x i = 2 Gas x j = Liquid x j = Fiber x j =

ELECTROHYDRODYNAMICS OF FREE LIQUID SURFACE IN A CIRCULAR CLEFT; AN APPLICATION TO ELECTROSPRAYING AND ELECTROSPINNING Journal: Acta Materialia A. Sarkar, Jiří Chvojka a D.Lukáš

Journal: Textile Progress Arindam+Jiří+David