Smoothed Particle Hydrodynamics

Slides:



Advertisements
Similar presentations
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 18 – Mass-radius relation for black dwarfs Chandrasekhar limiting mass Comparison.
Advertisements

H6: Relativistic momentum and energy
AMS 691 Special Topics in Applied Mathematics Review of Fluid Equations James Glimm Department of Applied Mathematics and Statistics, Stony Brook University.
Workshop on Numerical Methods for Multi-material Fluid Flows, Prague, Czech Republic, September 10-14, 2007 Sandia is a multiprogram laboratory operated.
Chapter 16 Dark Matter And The Fate Of The Universe.
Error Analysis for Material Point Method and a case study from Gas Dynamics Le-Thuy Tran and Martin Berzins Thanks to DOE for funding from
Stellar Interior. Solar Facts Radius: –R  = 7  10 5 km = 109 R E Mass : –M  = 2  kg –M  = 333,000 M E Density: –   = 1.4 g/cm 3 –(water is.
Particle-based fluid simulation for interactive applications
Universe in a box: simulating formation of cosmic structures Andrey Kravtsov Department of Astronomy & Astrophysics Center for Cosmological Physics (CfCP)
PRE-SUSY Karlsruhe July 2007 Rocky Kolb The University of Chicago Cosmology 101 Rocky I : The Universe Observed Rocky II :Dark Matter Rocky III :Dark Energy.
Prof. Reinisch, EEAS / Simple Collision Parameters (1) There are many different types of collisions taking place in a gas. They can be grouped.
By: Giuseppe Tormen. Heating Processes Adiabatic Compression Viscous Heating – Due to internal friction of the gas. Photoionization.
Module on Computational Astrophysics Jim Stone Department of Astrophysical Sciences 125 Peyton Hall : ph :
Modeling Fluid Phenomena -Vinay Bondhugula (25 th & 27 th April 2006)
PRESIDENCY UNIVERSITY
The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences Cracow, Poland Based on paper M.Ch., W. Florkowski nucl-th/ Characteristic.
Non-Newtonian nature of Causal Hydrodynamics T. Koide ( Universidade Federal do Rio de Janeiro ) G.S. Denicol (UFRJ),T. Kodama (UFRJ),Ph. Mota (UFRJ) Because.
Conservation Laws for Continua
Slug flow and fluid-structure interaction in industrial pipe systems
Conservation of Momentum. Conserved Total momentum of a system before and after an interaction remains constant Momentum before = Momentum After Two balls.
Relativistic Smoothed Particle Hydrodynamics
The Dual Origin of a Simulated Milky Way Halo Adi Zolotov (N.Y.U.), Beth Willman (Haverford), Fabio Governato, Chris Brook (University of Washington, Seattle),
(MNRAS 327, 610, 2001 & 347, 1234, 2004) David Churches, Mike Edmunds, Alistair Nelson - Physics & Astronomy, Cardiff University - Physics & Astronomy,
Nonequilibrium Dynamics in Astrophysics and Material Science YITP, Kyoto, Japan, Oct. 31-Nov. 3, 2011 Tetsufumi Hirano Sophia Univ./the Univ. of Tokyo.
Connecting the Galactic and Cosmological Length Scales: Dark Energy and The Cuspy-Core Problem By Achilles D. Speliotopoulos Talk Given at the Academia.
Physics 311 Classical Mechanics Welcome! Syllabus. Discussion of Classical Mechanics. Topics to be Covered. The Role of Classical Mechanics in Physics.
Effects of Compressibility, Turbulent Viscosity and Mass-Transfer-Rate on Accretion Discs in Close Binaries: Timescales of Outburst Events G. Lanzafame.
Aerodynamics Linear Motion (Moving Air ).
Csörgő, T. 1 Observables and initial conditions from exact rotational hydro solutions T. Csörgő 1, I. Barna 1 and M.I. Nagy 1,3 1 MTA Wigner Research Center.
Massive star evolution convection semiconvection overshoot angular momentum transport with and without B-field torques nucleosynthesis presupernova models.
Lecture 6 Momentum, Relativity, Energy and Civilization Chapter 3.8  3.15 Outline Linear Momentum Angular Momentum Relativity and Rest Energy Energy and.
Equal- and unequal-mass mergers of disk and elliptical galaxies with black holes Peter Johansson University Observatory Munich 8 th Sino-German workshop.
Energy momentum tensor of macroscopic bodies Section 35.
Modeling the Hadronization of Quark Matter G. Toledo Sánchez Instituto de Fisica UNAM, Mexico A. Ayala, G. Paic, M. Martinez ICN-UNAM, México Strangeness.
Method To run the simulations of our impacts with Pluto, we used a method known as “Smoothed Particle Hydrodynamics”. SPH is used to model the flow of.
It’s all Relativity. March, 1905: Twenty six year old Albert Einstein demonstrates the particle nature of light by explaining the photoelectric effect.
Software for the Games Industry 9 November 2004 Fluid Gaming: Particle Methods for Fluid Mechanics and Visualisation Graham Wynn James Gray Richard West.
Csörgő, T. 1 Observables and initial conditions from exact rotational hydro solutions T. Csörgő 1, I. Barna 1 and M.I. Nagy 1,3 1 MTA Wigner Research Center.
Origin of solar systems 30 June - 2 July 2009 by Klaus Jockers Max-Planck-Institut of Solar System Science Katlenburg-Lindau.
Conical Flow induced by Quenched QCD Jets Jorge Casalderrey-Solana, Edward Shuryak and Derek Teaney, hep- ph/ SUNY Stony Brook.
Моделирование магниторотационных процессов в коллапсирующих сверхновых и развитие Магнито-Дифференциально- Ротационной неустойчивости Сергей Моисеенко,
Simplified Smoothed Particle Hydrodynamics for Interactive Applications Zakiya Tamimi Richard McDaniel Based on work done at Siemens Corporate.
Relativistic Hydrodynamics T. Csörgő (KFKI RMKI Budapest) new solutions with ellipsoidal symmetry Fireball hydrodynamics: Simple models work well at SPS.
Multi-material simulation of laser-produced plasmas by Smoothed Particle Hydrodynamics A. Sunahara France /5-11. Institute.
A car of mass 1000 kg moves with a speed of 60 m/s on a circular track of radius 110 m. What is the magnitude of its angular momentum (in kg·m 2 /s) relative.
General Relativistic MHD Simulations with Finite Conductivity Shinji Koide (Kumamoto University) Kazunari Shibata (Kyoto University) Takahiro Kudoh (NAOJ)
Zagreb, Croatia, 2015/04/20 Csörgő, T. 1 New exact solutions of hydrodynamcs and search for the QCD Critical Point T. Csörgő 1,2 with I.Barna 1 and M.
2+1 Relativistic hydrodynamics for heavy-ion collisions Mikołaj Chojnacki IFJ PAN NZ41.
Lecture_06: Outline Special Theory of Relativity  Principles of relativity: length contraction, Lorentz transformations, relativistic velocity  Relativistic.
Does HBT interferometry probe thermalization? Clément Gombeaud, Tuomas Lappi and J-Y Ollitrault IPhT Saclay WPCF 2009, CERN, October 16, 2009.
M. Omang, S. Børve, and J. Trulsen
Low-Mass Star Formation, Triggered by Supernova in Primordial Clouds Masahiro N. Machida (Chiba University) Kohji Tomisaka (NAOJ) Fumitaka Nakamura (Niigata.
Momentum & Angular Momentum. Momentum Example on pg 178 in chapter 9 packet.
Relativistic Theory of Hydrodynamic Fluctuations Joe Kapusta University of Minnesota Nuclear Physics Seminar October 21, 2011 Collaborators: Berndt Muller.
Capture of Stars by Supermassive Black Holes J.A. de Freitas Pacheco T. Regimbau C. Filloux Observatoire de la Côte d’Azur.
PhD student at the International PhD Studies Institute of Nuclear Physics PAN Institute of Nuclear Physics PAN Department of Theory of Structure of Matter.
LISA double BHs Dynamics in gaseous nuclear disk.
Formation of BH-Disk system via PopIII core collapse in full GR National Astronomical Observatory of Japan Yuichiro Sekiguchi.
Hydrodynamics Continuity equation Notation: Lagrangian derivative
Cheng Zhao Supervisor: Charling Tao
Cosmology Scale factor Cosmology à la Newton Cosmology à la Einstein
T HE VORTICAL MECHANISM OF GENERATION & COLLIMATION OF THE ASTROPHYSICAL JETS M.G. A BRAHAMYAN Yerevan State University, Armenia.
Dynamics of a System of Particles Prof. Claude A Pruneau Notes compiled by L. Tarini Physics and Astronomy Department Wayne State University PHY 6200 Theoretical.
WPCF 2015, Warsaw, 2015/11/06 Csörgő, T. for Nagy, M 1 Observables and initial conditions for rotating and expanding fireballs T. Csörgő 1,2, I.Barna 1.
Application of smooth particle hydrodynamics on biomass burning
From: Numerical aspects of giant impact simulations
Le-Thuy Tran and Martin Berzins
Guido Ala, Elisa Francomano, Antonino Spagnuolo
Elastic Collisions.
Introduction to Accretion Discs
Presentation transcript:

Smoothed Particle Hydrodynamics Carlos Eduardo Aguiar Instituto de Física - UFRJ Outline Non-relativistic hydrodynamics. SPH equations. Applications. Relativistic hydrodynamics. Relativistic SPH. High energy nuclear physics.

Fluid Dynamics

Hydrodynamic Equations Continuity equation Ideal fluid Euler’s equation

Entropy Equation no viscosity no thermal conduction

Energy Equation

Ideal Gas

Conservation Laws

SPH Developed to study gas dynamics in astrophysical systems. Lagrangian method. No grids. Arbitrary geometries. Equally applicable in 1, 2 and 3 space dimensions. - L.Lucy, Astron.J. 82, 1013 (1977) - R.Gingold, J.Monaghan, MNRAS 181, 378 (1977) Reviews: - J. Monaghan, Annu. Rev. Astron. Astrophys. 30, 543 (1992) - L. Hernquist, N. Katz, Ap. J. Suppl. 70, 419 (1989)

Smoothing h x Error:

Particles "Monte-Carlo" sampling

Different ways of writing SP estimates (we omit the SP subscript from now on):

Derivatives No need for finite differences and grids: D D i-1 i i+1

More than one way of calculating derivatives: Exact Galilean invariance

Moving the Particles

Euler's Equation Exact momentum conservation

Entropy

Energy

Alternatively:

SPH Equations

Smoothing Kernels Gaussian: Spline:

Shock Waves shock wave x numerical calculation

Artificial Viscosity Galilean invariant. Vanishes for rotations. Conserves linear and angular momentum.

Local Resolution Length

SPH Simulation of the Hubble Volume Mass density in a thin slice (100x100x20Mpc/h) at the present epoch. This is a view one would observe if the speed of light were infinite.

SPH Simulation of Galaxy Formation Gas Dark Matter Density of gas and dark matter in a group of galaxies.

SPH Simulation of Supernova Explosion 75 ms after bounce z (km) x (km) Herant et al., Ap.J. 435, 339 (1994)

SPH Simulation of Supernova Explosion Herant et al., Ap.J. 435, 339 (1994)

SPH Simulation of Stellar Collision Disruption of a main sequence star by a close encounter with a high velocity neutron star. Colors represent log (density).

SPH Simulation of Colliding Asteroids An 8 m radius rock strikes the 1.6 km long asteroid Castalia at 5 km/s. Red is totally fractured rock, blue is intermediate fractured rock, and white particles represent the impactor.

SPH Simulation of Projectile Impact on Sand Projectile: Aluminum cylinder 30x10 cm (2d). Initial velocity: 3 km/sec Particles Temperature

Relativistic Hydrodynamics Energy-momentum conservation Baryon-number conservation

Continuity equation: Entropy equation: s = entropy density (rest frame)

Relativistic Euler equation: w = enthalpy per baryon Momentum equation:

Energy equation:

Relativistic SPH

Momentum (per baryon number) Energy (per baryon number)

Particle Velocity ?

RSPH Equations

Baryon-Free System entropy density: (Rest frame) (Lab frame)

Baryon-Free RSPH

Ultrarelativistic Pion Gas

Ultrarelativistic Pions Rarefaction Wave

SHASTA et al.

Ultrarelativistic Pions Landau Solution

Artificial Viscosity E.Chow and J.Monaghan, Journal of Computational Physics 134, 296 (1997) See also: S.Siegler and H.Riffert, astro-ph/9904070

Shock Tube Ideal nucleon gas

SHASTA et al.

Shock Tube Ideal nucleon gas

SHASTA et al.