Outline Dynamo: theoretical General considerations and plans Progress report Dynamo action associated with astrophysical jets Progress report Dynamo: experiment.

Slides:



Advertisements
Similar presentations
Statistical Properties of Broadband Magnetic Turbulence in the Reversed Field Pinch John Sarff D. Craig, L. Frassinetti 1, L. Marrelli 1, P. Martin 1,
Advertisements

Dynamo Effects in Laboratory Plasmas S.C. Prager University of Wisconsin October, 2003.
P.W. Terry K.W. Smith University of Wisconsin-Madison Outline
Magnetic Relaxation in MST S. Prager University of Wisconsin and CMSO.
Turbulent transport of magnetic fields Fausto Cattaneo Center for Magnetic Self-Organization in Laboratory and Astrophysical.
Pulsar radio wave dispersion, intermittency, and kinetic Alfvén wave turbulence Paul Terry Stas Boldyrev.
Control of Magnetic Chaos & Self-Organization John Sarff for MST Group CMSO General Meeting Madison, WI August 4-6, 2004.
Plans for Dynamo Research Presented by F. Cattaneo, S. Prager.
Progress and Plans on Magnetic Reconnection for CMSO For NSF Site-Visit for CMSO May1-2, Experimental progress [M. Yamada] -Findings on two-fluid.
Madison 2006 Dynamo Fausto Cattaneo ANL - University of Chicago Stewart Prager University of Wisconsin.
Collaborators: Jungyeon Cho --- Chungnam U.
CMSO 2005 Mean field dynamos: analytical and numerical results Fausto Cattaneo Center for Magnetic-Self Organization and Department.
The solar dynamo(s) Fausto Cattaneo Center for Magnetic Self-Organization in Laboratory and Astrophysical Plasmas Chicago 2003.
Chicago, October 2003 David Hughes Department of Applied Mathematics University of Leeds Nonlinear Effects in Mean Field Dynamo Theory.
Reconnection: Theory and Computation Programs and Plans C. C. Hegna Presented for E. Zweibel University of Wisconsin CMSO Meeting Madison, WI August 4,
Magnetic Chaos and Transport Paul Terry and Leonid Malyshkin, group leaders with active participation from MST group, Chicago group, MRX, Wisconsin astrophysics.
CMSO 2005 Simulation of Gallium experiment * § Aleksandr Obabko Center for Magnetic-Self Organization Department of Astronomy and Astrophysics.
General Meeting Madison, August 4-6, 2004 Plans and Progress of Magnetic Helicity Conservation and Transport H. Ji for participants of the Center for Magnetic.
INI 2004 Astrophysical dynamos Fausto Cattaneo Center for Magnetic Self-Organization Computations Institute Department of Mathematics.
September 2005 Magnetic field excitation in galaxies.
“Physics at the End of the Galactic Cosmic-Ray Spectrum” Aspen, CO 4/28/05 Diffusive Shock Acceleration of High-Energy Cosmic Rays The origin of the very-highest-energy.
Mario A. Riquelme, Anatoly Spitkovsky Department of Astrophysical Sciences, Princeton University Generation of magnetic field upstream of shocks: the cosmic.
Magnetization of Galactic Disks and Beyond Collaborators: Dmitry Shapovalov (Johns Hopkins) Alex Lazarian (U. Wisconsin) Jungyeon Cho (Chungnam) Kracow.
Flux emergence: An overview of thin flux tube models George Fisher, SSL/UC Berkeley.
New Mechanism of Generation of Large-Scale Magnetic Field in Turbulence with Large-Scale Velocity Shear I. ROGACHEVSKII, N. KLEEORIN, E. LIVERTS Ben-Gurion.
Influence of turbulence on the dynamo threshold B. Dubrulle, GIT/SPEC N. Leprovost, R. Dolganov, P. Blaineau J-P. Laval and F. Daviaud.
CHE/ME 109 Heat Transfer in Electronics
Krakow 2010 Galactic magnetic fields: MRI or SN-driven dynamo? Detlef Elstner Oliver Gressel Natali Dziourkevich Alfio Bonanno Günther Rüdiger.
Statistics of Lorenz force in kinematic stage of magnetic dynamo at large Prandtle number S.S.Vergeles Landau Institute for Theoretical Physics in collaboration.
Transport Equations for Turbulent Quantities
Different Limiting Mechanisms for Nonlinear Dynamos Robert Cameron Max-Planck-Institut für Sonnensystemforschung D Katlenburg-Lindau, Germany David.
Converging Ideas!!.  Great discussion led by the 4 invited speakers  Chuck Smith – Observational challenges  Ben Chandran – Theoretical questions &
Kinetic Effects on the Linear and Nonlinear Stability Properties of Field- Reversed Configurations E. V. Belova PPPL 2003 APS DPP Meeting, October 2003.
Enhancement of Heat Transfer P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Invention of Compact Heat Transfer Devices……
Physics of Convection " Motivation: Convection is the engine that turns heat into motion. " Examples from Meteorology, Oceanography and Solid Earth Geophysics.
Making Magnetic Fields: Dynamos in the Nonlinear Regime Collaborators: Alex Lazarian --- U. Wisconsin Jungyeon Cho --- Chungnam U. Dmitry Shapovalov ---
Effect of Magnetic Helicity on Non-Helical Turbulent Dynamos N. KLEEORIN and I. ROGACHEVSKII Ben-Gurion University of the Negev, Beer Sheva, ISRAEL.
Large scale magnetic fields and Dynamo theory Roman Shcherbakov, Turbulence Discussion Group 14 Apr 2008.
TerascaleSimulation Tools and Technologies Spectral Elements for Anisotropic Diffusion and Incompressible MHD Paul Fischer Argonne National Laboratory.
Decay of a simulated bipolar field in the solar surface layers Alexander Vögler Robert H. Cameron Christoph U. Keller Manfred Schüssler Max-Planck-Institute.
BGU WISAP Spectral and Algebraic Instabilities in Thin Keplerian Disks: I – Linear Theory Edward Liverts Michael Mond Yuri Shtemler.
MHD Turbulence driven by low frequency waves and reflection from inhomogeneities: Theory, simulation and application to coronal heating W H Matthaeus Bartol.
Dynamo theory and magneto-rotational instability Axel Brandenburg (Nordita) seed field primordial (decay) diagnostic interest (CMB) AGN outflows MRI driven.
Turbulent Dynamo Stanislav Boldyrev (Wisconsin-Madison) Fausto Cattaneo (Chicago) Center for Magnetic Self-Organization in Laboratory and Astrophysical.
3 March 2005ICTP Trieste David Hughes Department of Applied Mathematics University of Leeds Some Aspects of Mean Field Dynamo Theory.
1 Turbulent Generation of Large Scale Magnetic Fields in Unmagnetized Plasma Vladimir P.Pavlenko Uppsala University, Uppsala, Sweden.
Turbulent Dynamos: How I learned to ignore kinematic dynamo theory MFUV 2015 With Amir Jafari and Ben Jackel.
Box Model: Core Evolution ~ 700 Myr T(r,t) C(r,t) r ICB (t) 3D Model: Numerical Dynamo ~ 5 Myr intervals T(x,t) C(x,t) B(x,t) T(x,t) C(x,t) B(x,t) Thermodynamic.
MHD Dynamo Simulation by GeoFEM Hiroaki Matsui Research Organization for Informatuion Science & Technology(RIST), JAPAN 3rd ACES Workshop May, 5, 2002.
The Magneto-Rotational Instability and turbulent angular momentum transport Fausto Cattaneo Paul Fischer Aleksandr Obabko.
Numerical simulations of astrophysical dynamos Axel Brandenburg (Nordita, Stockholm) Dynamos: numerical issues Alpha dynamos do exist: linear and nonlinear.
ITP 2008 MRI Driven turbulence and dynamo action Fausto Cattaneo University of Chicago Argonne National Laboratory.
Convection in Flat Plate Boundary Layers P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi A Universal Similarity Law ……
Gas-kineitc MHD Numerical Scheme and Its Applications to Solar Magneto-convection Tian Chunlin Beijing 2010.Dec.3.
ENS MHD induction & dynamo LYON Laboratoire de Physique
Physics 681: Solar Physics and Instrumentation – Lecture 22 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Magnetic field transport in turbulent compressible convection Nic Brummell (303) JILA, University of Colorado Steve.
Turbulent Convection and Anomalous Cross-Field Transport in Mirror Plasmas V.P. Pastukhov and N.V. Chudin.
Gary A Glatzmaier University of California, Santa Cruz Direct simulation of planetary and stellar dynamos I. Methods and results.
ANGULAR MOMENTUM TRANSPORT BY MAGNETOHYDRODYNAMIC TURBULENCE Gordon Ogilvie University of Cambridge TACHOCLINE DYNAMICS
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Sun: Magnetic Structure Feb. 16, 2012.
May 23, 2006SINS meeting Structure Formation and Particle Mixing in a Shear Flow Boundary Layer Matthew Palotti University of Wisconsin.
H. Isobe Plasma seminar 2004/06/16 1. Explaining the latitudinal distribution of sunspots with deep meridional flow D. Nandy and A.R. Choudhhuri 2002,
INI 2004 Small-scale dynamos Fausto Cattaneo Department of Mathematics University of Chicago.
THE DYNAMIC EVOLUTION OF TWISTED MAGNETIC FLUX TUBES IN A THREE-DIMENSIONALCONVECTING FLOW. II. TURBULENT PUMPING AND THE COHESION OF Ω-LOOPS.
Magneto-rotational instability in the solar core and Ap star envelopes Rainer Arlt Astrophysikalisches Institut Potsdam and Günther Rüdiger, Rainer Hollerbach.
Spectral and Algebraic Instabilities in Thin Keplerian Disks: I – Linear Theory Edward Liverts Michael Mond Yuri Shtemler.
Dynamo action & MHD turbulence (in the ISM, hopefully…)
The Effects of Magnetic Prandtl Number On MHD Turbulence
Magnetic acceleration of relativistic jets
Presentation transcript:

Outline Dynamo: theoretical General considerations and plans Progress report Dynamo action associated with astrophysical jets Progress report Dynamo: experiment General considerations and plans Progress report

Dynamo action in astrophysics Liquid metal experiments Geodynamo Solar/stellar dynamos Galactic dynamos IGM Dynamo action present in many different physical systems Range of scales from meters to hundred of Kpc Basic mechanism very robust

Linear and nonlinear dynamos Kinematic regime Weak initial field Lorentz force negligible Seek exponentially growing solutions of the induction equation Linear eigenvalue problem Nonlinear regime Lorentz force dynamically important Dynamo saturation and stationary MHD (turbulence) state Self consistent solution of velocity and magnetic field Nonlinear initial value problem

Large and small scale dynamos Assume that velocity is characterized by typical scale o Small scale dynamo Generation on scales o Competition between line stretching and enhanced diffusion Dynamo generates B 2 but not B 2 Large scale dynamo Generation on scales o Lack of reflectional symmetry important (helicity) Inverse cascades (magnetic helicity, energy, etc.) Mean field theory and transport Average induction α-effect Average diffusion β-effect Average advection γ-effect

From kinematic to nonlinear dynamos Most astrophysical situations: Dynamos operate in nonlinear regime Magnetic fields are in equipartition with velocity on integral scales Rotation is often present and important Pm (= ) is either Hugeinterstellar medium Hugely small---stars and liquid metals What are the dynamo saturation mechanisms that leads to observed field stregths? /o/o 1 B 2 kinematic models nonlinear models Large-scale dynamos Small-scale dynamos

Research Plan Research to target three areas: Understand generic properties of nonlinear MHD dynamos. What determines the nonlinear saturation? What is the structure of dynamo fields at small magnetic Prandtl number? How are large scale fields generated by inverse cascades? Why is the alpha effect strong in the RFP and weak in numerical simulations aimed at astrophysics?

Research Plan Develop a self-consistent computational model for the solar dynamo. Build a code that integrates multiple physical processes in spherical and cylindrical geometry. Focus understanding origin of the large-scale magnetic field. Compare with solar observations, and with available liquid metal experiments.

Research Plan Understand the dynamics of dynamo effects beyond MHD, and their relevance to astrophysics and experiments. Under what conditions are different dynamo effect large? What is the relation of reconnection layer physics to dynamos? Which dynamo effects dominates in experiment? Are there important astrophysical situations for which non-MHD dynamo effects are significant?

Research Plan Detailed description of Research tasks Approximate timeline People involved Can be found at the CMSO web-page

Helical dynamos and inverse cascades Computations Hughes & Cattaneo Dynamo action in rotating convecting layer Rotating convection with Ra>>1, and strong rotation (Ta Ra) (Kinetic) helicity distribution anti-symmetric about the midplane anti- symmetric -effect System is a turbulent small-scale dynamo No evidence for large-scale field generation Results consistent with a laminar -effect What is going on?

Dynamo action in rough velocities Computations Tobias & Cattaneo Kinematic dynamo action in rough velocities Extend analytical results (see Boldyrevs presentation) to more general cases 1.Finite correlation time flows 2.Non Gaussian statistics 3.Presence of coherent structure Preliminary results show For many systems impact of 1 and 2 is relatively weak For certain classes of dynamos (quick dynamos) presence of coherent structures very important What is important in practice? streamfunction B-field streamfunctionB-field

Computational MRI: preliminary results Computations Fischer, Obabko & Cattaneo Nonlinear development of Magneto-Rotational Instability Cylindrical geometry similar to Goodman-Ji experiment Hydrodynamically stable rotation profile Weak vertical field Use newly developed spectral finite-elements MHD code Try to understand differences between experiments and simulations Simulations Re Rm (moderate). Experiments Re>>Rm (Rm smallish) Potentially great opportunity to develop turbulence models Get back to solar dynamo problem---continue with MRIdo both