MHD Department Institute of Safety Research 2 nd Sino-German Workshop on EPM (Dresden) Experimental studies of bubble-driven liquid metal flows in a static.

Slides:



Advertisements
Similar presentations
INSTABILITY OF ROTATING MAGNETIC FIELD DRIVEN FLOW IN A COUNTER-ROTATING CYLINDER Alexander Pedchenko and Ilmars Grants Institute of Physics, University.
Advertisements

Proto-Planetary Disk and Planetary Formation
Particle’s Dynamics in Dusty Plasma with Gradients of Dust Charges
AS 4002 Star Formation & Plasma Astrophysics BACKGROUND: Maxwell’s Equations (mks) H (the magnetic field) and D (the electric displacement) to eliminate.
Continuous casting - comparison between numerical simulation and experimental measurement EPM-MADYLAM Y.Delannoy, O.Widlund, J.Etay Presented by Y.Fautrelle.
Design Constraints for Liquid-Protected Divertors S. Shin, S. I. Abdel-Khalik, M. Yoda and ARIES Team G. W. Woodruff School of Mechanical Engineering Atlanta,
Electro-Hydro-Dynamics Enhancement of Multi-phase Heat Transfer
DIFFUSION MODELS OF A FLUIDIZED BED REACTOR Chr. Bojadjiev Bulgarian Academy of Sciences, Institute of Chemical Engineering, “Acad. G.Bontchev” str.,
On-Set of EHD Turbulence for Cylinder in Cross Flow Under Corona Discharges J.S. Chang, D. Brocilo, K. Urashima Dept. of Engineering Physics, McMaster.
MUTAC Review April 6-7, 2009, FNAL, Batavia, IL Mercury Jet Target Simulations Roman Samulyak, Wurigen Bo Applied Mathematics Department, Stony Brook University.
POSTER TEMPLATE BY: Presentations.com POSTER TEMPLATE BY: Presentations.com Outlet Inlet n’=375 n=150 n φ =75 (dφ=1.2 ⁰ ) Extra Terms.
NUMERICAL INVESTIGATION OF WAVE EFFECTS IN HIGH-FREQUENCY CAPACITIVELY COUPLED PLASMAS* Yang Yang and Mark J. Kushner Department of Electrical and Computer.
Brookhaven Science Associates U.S. Department of Energy Muon Collider/Neutrino Factory Collaboration Meeting May 26 – 28, CERN, Geneva Target Simulations.
Chapter 1: Introduction and Basic Concepts
A Study of Fluid Flow and Heat Transfer in a Liquid Metal in a Backward-Facing Step under Combined Electric and Magnetic Fields E. Gutierrez-Miravete and.
University of South Carolina FCR Laboratory Dept. of Chemical Engineering By W. K. Lee, S. Shimpalee, J. Glandt and J. W. Van Zee Fuel Cell Research Laboratory.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review March 16-17, 2006, FNAL, Batavia, IL Target Simulations Roman Samulyak Computational.
Data Fitting A Development of Dynamic Wind Tunnel Testing Technique with Magnetic Suspension and Balance System Workshop on Next Generation Transport Aircraft.
Viscosity. Average Speed The Maxwell-Boltzmann distribution is a function of the particle speed. The average speed follows from integration.  Spherical.
Computational Modelling of Unsteady Rotor Effects Duncan McNae – PhD candidate Professor J Michael R Graham.
Development of Synthetic Air Jet Technology for Applications in Electronics Cooling Dr. Tadhg S. O’Donovan School of Engineering and Physical Sciences.
Usually a diluted salt solution chemical decomposition
Sino-German Workshop on Electromagnetic Processing of Materials, – Shanghai, PR China Use of magnetic fields during solidification under.
Sino-German Workshop on EPM, Shanghai, Oct , 2004 Stiller, Frana, Grundmann, Cramer, Varshney, Gerbeth Numerical and Experimental Studies on Electromagnetic.
NUMERICAL STUDY OF THE INFLUENCE OF AN APPLIED ELECTRICAL POTENTIAL ON THE SOLIDIIFCATION OF A BINARY METAL ALLOY P.A. Nikrityuk, K. Eckert, R. Grundmann.
Numerical Simulation of Physical Foaming Processes
Institute of Safety Research MHD department Experiments on the magnetic field influence on gas-liquid metal two-phase flows Chaojie Zhang, Sven Eckert,
Sino-German-Workshop, Oct , Shanghai, China 1 New possibilities for velocity measurements in metallic melts S. Eckert, G. Gerbeth, F. Stefani.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2004, LBNL Target Simulation Roman Samulyak, in collaboration with.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review January 14-15, 2003, FNAL Target Simulations Roman Samulyak Center for Data Intensive.
Control of liquid metal by AC magnetic fields : examples of free surfaces and solidification Y. Fautrelle EPM lab./CNRS/Grenoble Polytechnic Institute.
2 nd Sino-German Workshop on EPM, Dresden, Oct , 2005 Frana, Stiller, Cramer Simulations on Stirring with Magnetic Fields 1 Simulations on Stirring.
Cavitation Models Roman Samulyak, Yarema Prykarpatskyy Center for Data Intensive Computing Brookhaven National Laboratory U.S. Department of Energy
1 LES of Turbulent Flows: Lecture 16 (ME EN ) Prof. Rob Stoll Department of Mechanical Engineering University of Utah Fall 2014.
Lesson 13 CONVECTION HEAT TRANSFER Given the formula for heat transfer and the operating conditions of the system, CALCULATE the rate of heat transfer.
Modeling Acoustic Modes in a Continuous Loop Piping System E. Marderness 1 and E. Gutierrez-Miravete 2 1 General Dynamics-Electric Boat, Groton, CT 2 Department.
Electromagnetic Waves and Their Propagation Through the Atmosphere
Convective Heat Transfer in Porous Media filled with Compressible Fluid subjected to Magnetic Field Watit Pakdee* and Bawonsak Yuwaganit Center R & D on.
Forschungszentrum Rossendorf Sino-German Workshop on EPM Shanghai, Oct , 2004 Flow Control by Tailored Magnetic Fields Context, Basic Ideas, Some.
Effect of HSMF on Electrodeposited Ni-Fe Membrane-- Crystal Morphology and Magnetism Performance Yunbo Zhong, Yanling Wen, Zhongming Ren, Kang Deng, Kuangdi.
Center for MHD Studies Turbulent MHD flow in a cylindrical vessel excited by a misaligned magnetic field A. Kapusta and B. Mikhailovich Center for MHD.
Walter Schostak Center for Materials Under eXtreme Environment
Forschungszentrum Rossendorf SFB 609FLOWCOMAG Flow Control by Tailored Magnetic Fields (FLOWCOMAG) April 1-2, 2004 Jointly organized by: Forschungszentrum.
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
Chapter 16 MECHANISMS OF HEAT TRANSFER Copyright © 2012 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Fundamentals of.
Enhanced heat transfer in confined pool boiling
Problem 14 Magnetic Spring Reporter: Hsieh, Tsung-Lin.
1 Linear Wave Equation The maximum values of the transverse speed and transverse acceleration are v y, max =  A a y, max =  2 A The transverse speed.
Some slides on UCLA LM-MHD capabilities and Preliminary Incompressible LM Jet Simulations in Muon Collider Fields Neil Morley and Manmeet Narula Fusion.
Transition to Tubulence in the Hartmann Layer A. Thess 1, D.Krasnov 1, E. Zienicke 1, O. Zikanov 2, T. Boeck 3 1-Ilmenau University of Technology 2-University.
Chapter 7 Natural convection systems. 7-1 Introduction  natural or free convection: the motion of the fluid due to density changes arising from heating.
MULTI-COMPONENT FUEL VAPORIZATION IN A SIMULATED AIRCRAFT FUEL TANK C. E. Polymeropoulos Department of Mechanical and Aerospace Engineering, Rutgers University.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2004, BNL Target Simulations Roman Samulyak in collaboration with Y.
Investigation of Thin Film Evaporation Limit in Single Screen Mesh Layers Presented to IMECE 2002 Nov. 19, 2002, New Orleans, LA Yaxiong Wang & G.P. “Bud”
Heat Transfer Su Yongkang School of Mechanical Engineering # 1 HEAT TRANSFER CHAPTER 6 Introduction to convection.
4TH ESO Chemistry and Physics IES AMES WORK HEAT WAVES.
FEASIBILITY ANALYS OF AN MHD INDUCTIVE GENERATOR COUPLED WITH A THERMO - ACOUSTIC ENERGY CONVERSION SYSTEM S. Carcangiu 1, R. Forcinetti 1, A. Montisci.
The rate of change of velocity.
Identifying the “wavemaker” of fluid/structure instabilities
Extended Surface Heat Transfer
UNIT - 4 HEAT TRANSFER.
Lecture 14 : Electromagnetic Waves
V. Galindo1, G. Gerbeth1, S. Eckert1, W. Witke1,
Liquid metal free surfaces under AC magnetic fields
S. Eckert1, V. Galindo1, G. Gerbeth1, W. Witke1,
Introduction to Space Weather
S. Eckert1, V. Galindo1, G. Gerbeth1, W. Witke1,
I. What? ~ II. Why? ~ III. How? Modelling volcanic plumes with WRF
Experimental and Numerical Investigation of Controlled, Small-Scale Motions in a Turbulent Shear Layer Bojan Vukasinovic, Ari Glezer Woodruff School of.
Magnetic field influences on electrochemical processes
Presentation transcript:

MHD Department Institute of Safety Research 2 nd Sino-German Workshop on EPM (Dresden) Experimental studies of bubble-driven liquid metal flows in a static magnetic field C. Zhang, S. Eckert, G. Gerbeth Forschungszentrum Rossendorf, Dresden - Germany

MHD Department Institute of Safety Research Background & Motivation Numerous applications of bubble-driven flows and magnetic fields in metallurgical engineering Combination of gas bubble injections and magnetic fields Comprehensive understandings of such MHD two-phase flows

MHD Department Institute of Safety Research Scalar quantity transportations in MHD flows A static magnetic field might both increase and decrease the heat transfer rate in enclosed thermal convections –T. Tagawa & H.Ozoe, J. Heat Transfer 120, –U. Burr & Mueller, J. Fluid Mech 453, –G. Authie, et al., 2003, Eur. J. Mech. B/Fluids 22, Flow field information are highly desirable How about bubble-driven flow in a magnetic field? Single bubble motion; bubble plume flow

MHD Department Institute of Safety Research Bubble-driven flow: experimental setup Cylindrical container aspect ratio=2.5 Liquid metal – GaInSn Single Ar bubble or bubble plume Q max =8cm 3 /s A vertical longitudinal magnetic field or a horizontal transverse magnetic field, B= T UDV measurements of the vertical and radial component velocity

MHD Department Institute of Safety Research Single bubble rising in a longitudinal magnetic field Rising bubble Bubble wake US transducer

MHD Department Institute of Safety Research Bubble wake modified by the longitudinal magnetic field B=0 B0B0

MHD Department Institute of Safety Research Bubble drag coefficient modified by the longitudinal magnetic field Magnetic interaction number: ratio between electromagnetic and inertial force (N = ) Bubble Eötvös number

MHD Department Institute of Safety Research Bubble velocity oscillation frequency and amplitude modified by the longitudinal magnetic field St = f  d e /u T

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Spatial properties (Q=0.37cm 3 /s) B=0 B=0.06T

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Spatial properties (Q=0.37cm 3 /s) B=0.11TB=0.17T

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Spatial properties (Q=3.7cm 3 /s) B=0B=0.06T

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Spatial properties (Q=3.7cm 3 /s) B=0.11TB=0.17T

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field -Radial component void fraction distribution measurements B Container cross-section view Q=7cm 3 /s

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Temporal properties (Q=4.0cm 3 /s) Q=5cm 3 /s R=0.87

MHD Department Institute of Safety Research Bubble plume-driven flow in the transverse magnetic field - Temporal properties (Q=4.0cm 3 /s) Q=5cm 3 /s R=0.87

MHD Department Institute of Safety Research Summary The non-intrusive UDV measuring technique allows us to look into the opaque liquid metal flows A DC transverse magnetic field modifies both the spatial and temporal properties of the ordinary bubble-driven flow DC magnetic field may enforce flow instabilities! (Continuous casting + EMBR) Potential tools for controlling liquid metal flows in metallurgical engineering

MHD Department Institute of Safety Research Perspectives for future research projects Potential topics of interest: –Liquid metal mixing enhancement (control of heat and mass transfer in bubble plumes) –Gas phase distributions –Free surface stabilization –Continuous casting –… FZR: Capacity of EPM model experiments in metallurgical engineering –Liquid metal model experiments –Magnetic fields (tailored fields  MULTIMAG facility) –Measuring techniques

MHD Department Institute of Safety Research Acknowledgement The research is supported by the Deutsche Forschungsgemeinschaft (DFG) in the form of the SFB 609 “Electromagnetic Flow Control in Metallurgy, Crystal Growth and Electrochemistry”. This support is gratefully acknowledged by the authors.

MHD Department Institute of Safety Research Magnetic field influence on the liquid velocity distribution in the container meridional plane Q=20sccm

MHD Department Institute of Safety Research Vortex structure evolution in a static magnetic field P. Davidson. 1995, JFM, 299,

MHD Department Institute of Safety Research when the velocity is uniform in the direction of the magnetic field, then current density is a potential, namely so there is no Joule dissipation in such case. Accordingly, the Joule dissipation can be reduced by forming the two-dimensional vortical structures along the magnetic field line direction. D. Lee & H. Choi, JFM, 2001, by taking the curl of both sides and using the equation

MHD Department Institute of Safety Research Bubble drag coefficient modified by the longitudinal magnetic field

MHD Department Institute of Safety Research Bubble velocity oscillation frequency and amplitude modified by the longitudinal magnetic field