Survey of experimental results

Size: px
Start display at page:

Download "Survey of experimental results"

Transcription

1 Survey of experimental results Philippe CARDIN, Observatoire de Grenoble, France Caramulo, September 5, 2003

2 Do we need experiments? Proofs of theory Checks of numerical simulations. Studies in different regimes Real models of natural objects Inputs for theories or simulations Improvement in technology Discoveries September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 2

3 Outline 1. Introduction : some physical properties 2. Historical approach to experimental dynamos : Two successful experiments 4. A new generation of experimental dynamos... September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 3

4 Outline 1. Introduction : some physical properties 2. Historical approach to experimental dynamos : Two successful experiments 4. A new generation of experimental dynamos... September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 4

5 The magnetic Reynolds number UL Re m = = η µσul Necessary condition for dynamo action : Re m >~50 µ is difficult to change (Martin et al, 2000; Frick et al, 2002) σ Na = 3 σ Ga = 10 σ Hg σ Na decreases with T At T 100 C, µσ Na 10 For L = 1m, τ diff 0.1 s Size L and velocity U should be as large as possible September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 5

6 The magnetic Reynolds number UL UL ν Re = = = η ν η Re m P m For liquid metals, P m 10-6 Liquid metal dynamo occurs for large Re (>10 6 ) Turbulent dynamos β effect (effective η increases with turbulence). (Reighart and Brown, 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 6

7 Velocity / Size Velocity is limited by the available power. Po 3 ρη R L 3 m For liquid sodium: ρη 3 = 1 Pour Rm = 50, L = 1 m, Po 100 kw (Nataf, 2003) The problem is to cool down the experiment (O.1K/s) Large L is necessary. Sodium is cheap (< 10 /l) and light (r < 1000). Sodium is dangerous (reductor, water => explosion H2). Large experiments are expansive. September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 7

8 Experiments ; necessary conditions Rm> 50 imposes the use of sodium U > 5m/s, which means a power of a few hundreds KW (cooling unit too) L > 1m, which means a few tons of liquid sodium An adequate velocity field (in space and time) to start and maintain a dynamo September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 8

9 Outline 1. Introduction : some physical properties 2. Historical approach to experimental dynamos : Two successful experiments 4. A new generation of experimental dynamos... September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 9

10 (Lehnert,1958) Na b t /B <0.25 b pr /B < cm 58 litres of sodium. Ω< 500 rpm Rm < 5 «ω effect» September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 10

11 (Lowes and Wilkinson,1963; 1968) (Herzenberg, 1958) 2 * 100 W 7 cm Ferromagnetic materials (µ > µ 0 ) + Mercury September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 11

12 (Lowes and Wilkinson,1963; 1968) µ r ~ 200 Re m ~ 200 September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 12

13 (Steenbeck et al.,1967) 15 cm 51 cm U = 0-11 m/s «α effect» September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 13

14 U (mv) (Steenbeck et al.,1967) 40 - U (mv) 40 - U α v 2 B v 2 B (T) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 14

15 (Steenbeck et al.,1967) U/U theo U theo α µ 0 σv 2 Bl 2 N = σlb 2 /ρv September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 15

16 50 rpm (Gans,1970) Rem 20 Na 25 cm 3600 rpm Megater, Léorat September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 16

17 Outline 1. Introduction : some physical properties 2. Historical approach to experimental dynamos : Two successful experiments 4. A new generation of experimental dynamos... September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 17

18 The Riga dynamo (Ponomarenko,1973) dynamo z translation helicoidal flow At rest Kinematic approach, With infinite geometry. B exp(ikz) exp(iωt) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 18

19 First attempt Imposed magnetic field Induced magnetic field Leningrad, 1987 (Gailitis et al., 1987, 1989); (Gailitis 1992). September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 19

20 First attempt; results. (Gailitis et al., 1987, 1989); (Gailitis 1992). Improvements: (Gailitis, 1996); (Christen et al., 1998) (Stefani et al.,1999) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 20

21 Riga Dynamo (120 kw, 1500 litres Na, 2200 rpm) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 21

22 Riga; growth of the magnetic field (Gailitis et al., 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 22

23 Riga; comparison Num./Exp. (Gailitis et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 23

24 Riga: Motor power measurements 10 KW (Gailitis et al., 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 24

25 Riga: Saturation (Gailitis et al., 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 25

26 The Karlsruhe dynamo (G.O.Roberts,1972) dynamo (Busse,1992): r 0,d,a/r 0 <<1 Re m, H Rem, C > 8 π 2 Re m, H Re m, C > 16a πr d 1 + πr0 2 September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 26

27 Karlsruhe: the set up (1600 litres Na, 630 kw) m 52 cylindres 0.21 m 1.7 m 0.19 m V C or V H up to 120 m 3 /h September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 27

28 Dynamo modulus in Karlruhe September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 28

29 Pr Müller and the dynamo modulus September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 29

30 View of the building in Karlsruhe September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 30

31 Dynamo effect in Karlsruhe experiment (Müller and Stieglitz, 2000) (Stieglitz and Müller, 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 31

32 Stability diagram in Karlsruhe dynamo (Stieglitz and Müller, 2001) (Rädler et al, 1998) (Tilgner, 1997) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 32

33 B-spectra in Karlsruhe f -1 spectra f -3 f F (Hz) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 33

34 Two succesful experimental dynamos Good prediction of the onset with laminar (average) flow and ideal boundary conditions. Kinematic and mean field approaches. Saturation mechanism? (Tilgner et Busse, 2002) Motions of the liquid sodium initially at rest. (Pétrélis et Fauve, 2001) claim that a turbulent scaling is in agreement with the experiment whereas a laminar scaling predict a field orders of magnitude too small. September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 34

35 Outline 1. Introduction : some physical properties 2. Historical approach to experimental dynamos : Two successful experiments 4. A new generation of experimental dynamos... September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 35

36 The Maryland group A convective dynamo? 20.3 cm (Shew et al.,2002) 6000 rpm, E ~ 10-8, Λ ~ 1, Rm < cm 1.5 litres 6000 rpm Rm<8 (Lathrop et al., 2001) 90 litres 61 cm (Aubert el al.,2001) predict if R=1 m and 100kW of heat, Re m = 1 September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 36

37 Mechanically forced motions S2T2 kinematic model (Dudley and James, 1989) R mc = 55 2 * 7.4 kw 15 litres D = 31.2 cm (Lathrop et al., 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 37

38 Decay rates m=0 m=1 (Peffley et al., 2001) R mc ~ 200? September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 38

39 Hunting for dynamos 1 Cu plate 3 Cu rings 5 Cu plates + baffles Different propellers BEST Herzenberg type (Shew et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 39

40 MHD Turbulence 15 litres 31.2 cm N = σlb 2 /ρv Re m = rpm var B (Sisan et al., 2003) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 40

41 The maryland project Ω 2 Ω 1 D=3m, 15 tonnes Sodium. 260 kw * 3= 780 kw. Rem < 400. Ω sphère (Lathrop, 2003) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 41

42 Van Karman experiments : VKG 5 litres gallium R = 10cm 2*11 kw Rm<16 Magnetic expulsion (Odier et al., 1998;2000) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 42

43 Van Karman Sodoium 70 litres sodium, 2*75 kw, 1500 rpm, Rm<50 R=20 cm, H=2R September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 43

44 View of the Cadarache experiment September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 44

45 VKS: optimisation of the flow Poloidal / Toroïdal cm of cupper R mc ~ 70 or R mmax ~ 55 (Marié et al., 2001) (Bourgoin et al., 2002) LDV et UDV September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 45

46 VKS: MHD effects ω effect α effect N << 1 B o passive Expulsion (Bourgoin et al., 2002) (Marié et al, 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 46

47 VKS : spectra (Bourgoin et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 47

48 Madison Experiment Optimisation of S2T2 kinematic model (Dudley and James, 1989) R mc = 47 2* 50 kw 1750 rpm 1 m (Forest et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 48

49 Madison: Onset of the average flow (Forest et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 49

50 Diameter=1m 150 kw V~20m/s C 35 kw cooling 120G axial R m ~250 > 100 View of the Madison experiment September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 50

51 Ponomarenko type The Perm project Water: 2 kw, 3000 rpm 0.2 à 0.5 s breaking τ=1-2 s. (Frick et al, 2002) Sodium experiment: R=0.4 m, r=0.12 m 115 litres Na 3000 rpm Vmax=140 m/s Rm=40 Breaking 0.1 s September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 51

52 Perm: Optimisation of the flow Amplification factor of 3 0.1s Increase of µ 0.2 s. Dependent of the initial magnetic field (Dobler et al., 2003) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 52

53 Socorro group: α ω type dynamo (Colgate et al., 2002) Taylor-Couette flow (ω effect ) + Sodium plumes (α effect ) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 53

54 Socorro: design of the experiment 30.5cm Na 30.5cm <8000 tpm <2000 tpm 61cm 100 kw Rem~120 Water experiment Sodium tank (Colgate et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 54

55 The Grenoble project. 1 litre de gallium, 3000 rpm. (Brito et al., 1995; 1996) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 55

56 An Ω quenching effect? (Brito et al., 1995) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 56

57 Convective study Temperature T2 Temperature T1 September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 57

58 Thermal convection in rapidly rotating shell (Aubert et al., 2001) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 58 5 litres of gallium, up to 1000 tpm. With toroidal magnetic field Without magnetic field Nicolas. Gillet

59 Ultrasonic velocity measurements (Aubert et al, 2001; Aubert et al., 2003) U ΩD conv = αgf ρc Ω D p September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 59

60 Viscosity measurement Spin-up experiment At t=0, Ω =300 rpm --> Ω=340 tpm Brito et al, 2003 September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 60

61 (Greenspan, 1968) theory u φ ( s, t) = s Ω exp 1/ 2 E Ω t (1 s R / 4 ) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 61

62 Turbulent viscosity measurement September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 62

63 The DTS experiment 45 litres of Na, 2*10 kw Rm < 30 Spherical Couette experiment (Cardin et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 63

64 A magnetostrophic experimental dynamo: A planetary dynamo model R m = 100 a = 1 m Power = 600 kw Ω = 450 rpm Ω = 150 rpm B = 0.3 T (Cardin et al., 2002) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 64

65 Conclusion? (Nataf,2003) September 5, 2003 Caramulo, Survey of experimental results - P. Cardin 65

Dynamo theory and its experimental validation

Dynamo theory and its experimental validation Dynamo theory and its experimental validation Karl-Heinz Rädler Astrophysical Institute Potsdam Stockholm February 2009 Outline The idea of the self-exciting dynamo and elements of dynamo theory The Riga

More information

Laboratory Dynamo Experiments

Laboratory Dynamo Experiments Space Sci Rev (2010) 152: 543 564 DOI 10.1007/s11214-009-9546-1 Laboratory Dynamo Experiments Gautier Verhille Nicolas Plihon Mickael Bourgoin Philippe Odier Jean-François Pinton Received: 22 March 2009

More information

Magnetic field reversals in turbulent dynamos

Magnetic field reversals in turbulent dynamos Magnetic field reversals in turbulent dynamos Stéphan Fauve LPS-ENS-Paris APS, San Antonio, november 23, 2008 Cosmic magnetic fields Earth 0.5 G Sun 1 G (Hale, 1908) 10 3 G Neutrons stars 10 10-10 13 G

More information

Chaotic dynamics of the magnetic field generated by a turbulent flow in the VKS experiment

Chaotic dynamics of the magnetic field generated by a turbulent flow in the VKS experiment Chaotic dynamics of the magnetic field generated by a turbulent flow in the VKS experiment Stéphan Fauve LPS - ENS-Paris Wolfgang Pauli Institute, Vienna, february 14 th 2008 MHD equations and dimensionless

More information

Laboratory Dynamo Experiments

Laboratory Dynamo Experiments Laboratory Dynamo Experiments Gautier Verhille, Nicolas Plihon, Mickaël Bourgoin, Philippe Odier, Jean-François Pinton To cite this version: Gautier Verhille, Nicolas Plihon, Mickaël Bourgoin, Philippe

More information

Liquid metal dynamo experiments

Liquid metal dynamo experiments Liquid metal dynamo experiments Sébastien Aumaître CEA-Saclay and VKS team Dynamics and turbulent transport in plasmas and conducting fluids Les Houche-2011 Bibliography H. K. Moffatt : Magnetic field

More information

Measurements of the magnetic field induced by a turbulent flow of liquid metal a

Measurements of the magnetic field induced by a turbulent flow of liquid metal a PHYSICS OF PLASMAS 13, 055901 006 Measurements of the magnetic field induced by a turbulent flow of liquid metal a M. D. Nornberg, E. J. Spence, R. D. Kendrick, C. M. Jacobson, and C. B. Forest b Department

More information

Lorentz force effects in magneto-turbulence

Lorentz force effects in magneto-turbulence Physics of the Earth and Planetary Interiors 135 (2003) 137 159 Lorentz force effects in magneto-turbulence Daniel R. Sisan, Woodrow L. Shew, Daniel P. Lathrop Department of Physics, IREAP and IPST, University

More information

THE RIGA DYNAMO EXPERIMENTS

THE RIGA DYNAMO EXPERIMENTS THE RIGA DYNAMO EXPERIMENTS Frank Stefani, Thomas Gundrum, Gunter Gerbeth, Agris Gailitis, Olgerts Lielausis, and Ernests Platacis. Introduction Cosmic magnetic fields, including the magnetic fields of

More information

RESULTS OF THE FIRST RIGA DYNAMO EXPERIMENT

RESULTS OF THE FIRST RIGA DYNAMO EXPERIMENT RESULTS OF THE FIRST RIGA DYNAMO EXPERIMENT Frank Stefani, Gunter Gerbeth and Thomas Gundrum. Introduction The investigation of homogeneous fluid dynamos where a magnetic field B is created solely out

More information

Large-scale field and small scale dynamo

Large-scale field and small scale dynamo Large-scale field and small scale dynamo Franck Plunian & Yannick Ponty Université de Grenoble, LGIT Observatoire de la Côte d'azur Large scale magnetic fields are ubiquitous in planetary and stellar objects

More information

The Madison Dynamo Experiment: magnetic instabilities driven by sheared flow in a sphere. Cary Forest Department of Physics University of Wisconsin

The Madison Dynamo Experiment: magnetic instabilities driven by sheared flow in a sphere. Cary Forest Department of Physics University of Wisconsin The Madison Dynamo Experiment: magnetic instabilities driven by sheared flow in a sphere Cary Forest Department of Physics University of Wisconsin February 28, 2001 Planets, stars and perhaps the galaxy

More information

Influence of time dependent flows on the threshold of the kinematic dynamo action

Influence of time dependent flows on the threshold of the kinematic dynamo action Eur. Phys. J. Special Topics 146, 313 32 (27) c EDP Sciences, Springer-Verlag 27 DOI: 1.114/epjst/e27-189-4 THE EUROPEAN PHYSICAL JOURNAL SPECIAL TOPICS Influence of time dependent flows on the threshold

More information

TOPICAL PROBLEMS OF FLUID MECHANICS 195 STABILTY OF A CONDUCTING FLUID CONTAINED BETWEEN TWO ROTATING SPHERES SUBJECTED TO A DIPOLAR MAGNETIC FIELD

TOPICAL PROBLEMS OF FLUID MECHANICS 195 STABILTY OF A CONDUCTING FLUID CONTAINED BETWEEN TWO ROTATING SPHERES SUBJECTED TO A DIPOLAR MAGNETIC FIELD TOPICAL PROBLEMS OF FLUID MECHANICS 95 DOI: https://doi.org/0.43/tpfm.207.025 STABILTY OF A CONDUCTING FLUID CONTAINED BETWEEN TWO ROTATING SPHERES SUBJECTED TO A DIPOLAR MAGNETIC FIELD A. Lalaoua,2, F.

More information

NIMROD simulations of dynamo experiments in cylindrical and spherical geometries. Dalton Schnack, Ivan Khalzov, Fatima Ebrahimi, Cary Forest,

NIMROD simulations of dynamo experiments in cylindrical and spherical geometries. Dalton Schnack, Ivan Khalzov, Fatima Ebrahimi, Cary Forest, NIMROD simulations of dynamo experiments in cylindrical and spherical geometries Dalton Schnack, Ivan Khalzov, Fatima Ebrahimi, Cary Forest, 1 Introduction Two experiments, Madison Plasma Couette Experiment

More information

Numerical Study of Dynamo Action at Low Magnetic Prandtl Numbers

Numerical Study of Dynamo Action at Low Magnetic Prandtl Numbers Numerical Study of Dynamo Action at Low Magnetic Prandtl Numbers Yannick Ponty, Pablo Mininni, David Montgomery, Jean-François Pinton, Hélène Politano, Annick Pouquet To cite this version: Yannick Ponty,

More information

An iterative study of time independent induction effects in magnetohydrodynamics.. March 16, Abstract

An iterative study of time independent induction effects in magnetohydrodynamics.. March 16, Abstract An iterative study of time independent induction effects in magnetohydrodynamics.. March 16, 24 M. Bourgoin 1, P. Odier 1, J.-F. Pinton 1, Y. Ricard 2 (1) Laboratoire de Physique, CNRS UMR#5672, (2) Laboratoire

More information

Creation and destruction of magnetic fields

Creation and destruction of magnetic fields HAO/NCAR July 30 2007 Magnetic fields in the Universe Earth Magnetic field present for 3.5 10 9 years, much longer than Ohmic decay time ( 10 4 years) Strong variability on shorter time scales (10 3 years)

More information

arxiv: v1 [physics.flu-dyn] 9 Mar 2018

arxiv: v1 [physics.flu-dyn] 9 Mar 2018 Laboratory experiments on dynamo action and magnetically triggered flow instabilities F. STEFANI, A. GAILITIS, G. GERBETH, A. GIESECKE, Th. GUNDRUM, G. RÜDIGER, M. SEILMAYER, T. VOGT arxiv:1803.03421v1

More information

Colloquium: Laboratory experiments on hydromagnetic dynamos

Colloquium: Laboratory experiments on hydromagnetic dynamos Colloquium: Laboratory experiments on hydromagnetic dynamos Agris Gailitis, Olgerts Lielausis, and Ernests Platacis Institute of Physics, University of Latvia, LV-2169 Salaspils 1, Latvia Gunter Gerbeth

More information

Kinematic dynamo onset and magnetic field saturation in rotating spherical Couette and periodic box simulations

Kinematic dynamo onset and magnetic field saturation in rotating spherical Couette and periodic box simulations Kinematic dynamo onset and magnetic field saturation in rotating spherical Couette and periodic box simulations Dissertation zur Erlangung des mathematisch-naturwissenschaftlichen Doktorgrades Doctor rerum

More information

Large scale fluctuations and dynamics of the Bullard - von. Abstract

Large scale fluctuations and dynamics of the Bullard - von. Abstract Large scale fluctuations and dynamics of the Bullard - von Kármán dynamo Gautier Verhille, Nicolas Plihon, Grégory Fanjat, Romain Volk, Mickael Bourgoin, and Jean-François Pinton arxiv:0906.2719v1 [physics.flu-dyn]

More information

Magnetic field reversals in an experimental turbulent dynamo

Magnetic field reversals in an experimental turbulent dynamo March 27 EPL, 77 (27) 591 doi: 1.129/295-575/77/591 www.epljournal.org Magnetic field reversals in an experimental turbulent dynamo M. Berhanu 1,R.Monchaux 2,S.Fauve 1,N.Mordant 1,F.Pétrélis 1,A.Chiffaudel

More information

Bifurcations and multistability in turbulence

Bifurcations and multistability in turbulence Bifurcations and multistability in turbulence VKS team A. Chiffaudel L. Marié F. Ravelet F.Daviaud CEA/Saclay, France O. Dauchot A. Prigent Conceptual Aspects of turbulence, Vienna, February 28 1 Bifurcations

More information

Convection-driven dynamos in the limit of rapid rotation

Convection-driven dynamos in the limit of rapid rotation Convection-driven dynamos in the limit of rapid rotation Michael A. Calkins Jonathan M. Aurnou (UCLA), Keith Julien (CU), Louie Long (CU), Philippe Marti (CU), Steven M. Tobias (Leeds) *Department of Physics,

More information

Planetary dynamos: Dipole-multipole transition and dipole reversals

Planetary dynamos: Dipole-multipole transition and dipole reversals Planetary dynamos: Dipole-multipole transition and dipole reversals Ulrich Christensen Max-Planck-Institute for Solar System Research Katlenburg-Lindau, Germany in collaboration with Hagay Amit, Julien

More information

Bistability between a stationary and an oscillatory dynamo in a turbulent flow of liquid sodium

Bistability between a stationary and an oscillatory dynamo in a turbulent flow of liquid sodium J. Fluid Mech. (29), vol. 641, pp. 217 226. c Cambridge University Press 29 doi:1.117/s221129991996 217 Bistability between a stationary and an oscillatory dynamo in a turbulent flow of liquid sodium M.

More information

Profile SFR-27 VKS2 FRANCE. Von Karman Sodium Saint Paul Lez Durance FRANCE

Profile SFR-27 VKS2 FRANCE. Von Karman Sodium Saint Paul Lez Durance FRANCE Profile SFR-27 VKS2 FRANCE GENERAL INFORMATION NAME OF THE ACRONYM COOLANT(S) OF THE LOCATION (address): OPERATOR CONTACT PERSON (name, address, institute, function, telephone, email): Von Karman Sodium

More information

Magnetohydrodynamic experiments on cosmic magnetic fields

Magnetohydrodynamic experiments on cosmic magnetic fields ZAMM Z. Angew. Math. Mech. 88, No. 12, 930 954 (2008) / DOI 10.1002/zamm.2008002 Magnetohydrodynamic experiments on cosmic magnetic fields Plenary lecture presented at the 79th Annual GAMM Conference,

More information

Anisotropic turbulence in rotating magnetoconvection

Anisotropic turbulence in rotating magnetoconvection Anisotropic turbulence in rotating magnetoconvection André Giesecke Astrophysikalisches Institut Potsdam An der Sternwarte 16 14482 Potsdam MHD-Group seminar, 2006 André Giesecke (AIP) Anisotropic turbulence

More information

Effects of conductivity jumps in the envelope of a kinematic dynamo flow

Effects of conductivity jumps in the envelope of a kinematic dynamo flow C. R. Mecanique 334 (2006) 593 598 http://france.elsevier.com/direct/cras2b/ Effects of conductivity jumps in the envelope of a kinematic dynamo flow Raphael Laguerre a,d,, Caroline Nore a,b,jacquesléorat

More information

arxiv: v1 [physics.flu-dyn] 30 Oct 2014

arxiv: v1 [physics.flu-dyn] 30 Oct 2014 MAGNETOHYDRODYNAMICS Vol. 40 (2004), No. 1, pp. 1 9 TOWARDS A PRECESSION DRIVEN DYNAMO EXPERIMENT arxiv:1410.8373v1 [physics.flu-dyn] 30 Oct 2014 F. Stefani 1, T. Albrecht 2, G. Gerbeth 1, A. Giesecke

More information

Simulation Study on the Generation and Distortion Process of the Geomagnetic Field in Earth-like Conditions

Simulation Study on the Generation and Distortion Process of the Geomagnetic Field in Earth-like Conditions Chapter 1 Earth Science Simulation Study on the Generation and Distortion Process of the Geomagnetic Field in Earth-like Conditions Project Representative Yozo Hamano Authors Ataru Sakuraba Yusuke Oishi

More information

Numerical study of dynamo action at low magnetic Prandtl numbers

Numerical study of dynamo action at low magnetic Prandtl numbers Numerical study of dynamo action at low magnetic Prandtl numbers Y. Ponty 1, P.D. ininni 2, D.C. ontgomery 3, J.-F. Pinton 4, H. Politano 1 and A. Pouquet 2 1 CNRS UR6202, Laboratoire Cassiopée, Observatoire

More information

Dynamo action at low magnetic Prandtl numbers: mean flow vs. fully turbulent motion

Dynamo action at low magnetic Prandtl numbers: mean flow vs. fully turbulent motion Dynamo action at low magnetic Prandtl numbers: mean flow vs. fully turbulent motion Yannick Ponty, Pablo Mininni, Jean-François Pinton, Hélène Politano, Annick Pouquet To cite this version: Yannick Ponty,

More information

Q: Why do the Sun and planets have magnetic fields?

Q: Why do the Sun and planets have magnetic fields? Q: Why do the Sun and planets have magnetic fields? Dana Longcope Montana State University w/ liberal borrowing from Bagenal, Stanley, Christensen, Schrijver, Charbonneau, Q: Why do the Sun and planets

More information

Fluctuation dynamo amplified by intermittent shear bursts

Fluctuation dynamo amplified by intermittent shear bursts by intermittent Thanks to my collaborators: A. Busse (U. Glasgow), W.-C. Müller (TU Berlin) Dynamics Days Europe 8-12 September 2014 Mini-symposium on Nonlinear Problems in Plasma Astrophysics Introduction

More information

Generation of magnetic fields by large-scale vortices in rotating convection

Generation of magnetic fields by large-scale vortices in rotating convection Generation of magnetic fields by large-scale vortices in rotating convection Céline Guervilly, David Hughes & Chris Jones School of Mathematics, University of Leeds, UK Generation of the geomagnetic field

More information

arxiv: v1 [physics.flu-dyn] 19 Apr 2007

arxiv: v1 [physics.flu-dyn] 19 Apr 2007 Magnetic induction in a turbulent flow of liquid sodium: mean behaviour and slow fluctuations arxiv:7.6v [physics.flu-dyn] 9 Apr 7 F. Ravelet,, R. Volk, A. Chiffaudel, F. Daviaud, B. Dubrulle, R. Monchaux,

More information

Rotating dynamo turbulence: theoretical and numerical insights

Rotating dynamo turbulence: theoretical and numerical insights Rotating dynamo turbulence: theoretical and numerical insights Nathanaël Schaeffer 1, H.-C. Nataf 1, A. Fournier 2, J. Aubert 2, D. Jault 1, F. Plunian 1, P. Zitzke 1 1: ISTerre / CNRS /Université Joseph

More information

Magnetic field topologies of M dwarfs

Magnetic field topologies of M dwarfs LATT CNRS / Université de Toulouse J. F. Donati, P. Petit, B. Dintrans LATT CNRS / Université de Toulouse X. Delfosse, T. Forveille LAOG CNRS / Université de Grenoble M. M. Jardine University of St Andrews

More information

Dynamics in the Earth s core. Philippe Cardin, ISTerre, Université Grenoble Alpes et CNRS

Dynamics in the Earth s core. Philippe Cardin, ISTerre, Université Grenoble Alpes et CNRS Dynamics in the Earth s core Philippe Cardin, ISTerre, Université Grenoble Alpes et CNRS Doctoral training on internal Earth, Barcelonnette, oct 2016 Sources of motions inside the core Core cooling and

More information

Emmanuel DORMY (CNRS / ENS)

Emmanuel DORMY (CNRS / ENS) Emmanuel DORMY (CNRS / ENS) dormy@phys.ens.fr The Earth s internal structure Mantle Fluid outer core ICB 3480 km 6366 km 1221 km Inner core CMB Roberts & King 2013 Governing Equations Governing Equations

More information

Scaling properties of convection-driven dynamos in rotating spherical shells and application to planetary magnetic fields

Scaling properties of convection-driven dynamos in rotating spherical shells and application to planetary magnetic fields Geophys. J. Int. (006) 66, 97 4 doi: 0./j.365-46X.006.03009.x Scaling properties of convection-driven dynamos in rotating spherical shells and application to planetary magnetic fields U. R. Christensen

More information

Wave-driven dynamo action in spherical MHD systems

Wave-driven dynamo action in spherical MHD systems Wave-driven dynamo action in spherical MHD systems K. Reuter, F. Jenko, A. Tilgner, 2 and C. B. Forest 3 Max-Planck-Institut für Plasmaphysik, EURATOM Association, Boltzmannstraße 2, D-85748 Garching,

More information

Vortex Dynamos. Steve Tobias (University of Leeds) Stefan Llewellyn Smith (UCSD)

Vortex Dynamos. Steve Tobias (University of Leeds) Stefan Llewellyn Smith (UCSD) Vortex Dynamos Steve Tobias (University of Leeds) Stefan Llewellyn Smith (UCSD) An introduction to vortices Vortices are ubiquitous in geophysical and astrophysical fluid mechanics (stratification & rotation).

More information

Creation and destruction of magnetic fields

Creation and destruction of magnetic fields HAO/NCAR July 20 2011 Magnetic fields in the Universe Earth Magnetic field present for 3.5 10 9 years, much longer than Ohmic decay time ( 10 4 years) Strong variability on shorter time scales (10 3 years)

More information

Astronomical Notes. Astronomische Nachrichten Founded by H. C. Schumacher in 1821

Astronomical Notes. Astronomische Nachrichten Founded by H. C. Schumacher in 1821 Astronomical Notes Astronomische Nachrichten Founded by H. C. Schumacher in 1821 Editors K. G. Strassmeier (Potsdam/Editor-in-Chief), G. Hasinger (Garching), R.-P. Kudritzki (Honolulu), T. Montmerle (Grenoble),

More information

arxiv: v1 [physics.flu-dyn] 26 Aug 2009

arxiv: v1 [physics.flu-dyn] 26 Aug 2009 Influence of an external magnetic field on forced turbulence in a swirling flow of liquid metal Basile Gallet, Michael Berhanu, and Nicolas Mordant arxiv:0908.3821v1 [physics.flu-dyn] 26 Aug 2009 Laboratoire

More information

ABSTRACT. Dr. Daniel P. Lathrop, Department of Physics. Background and theory for the geodynamo is presented, along with a review of

ABSTRACT. Dr. Daniel P. Lathrop, Department of Physics. Background and theory for the geodynamo is presented, along with a review of ABSTRACT Title of Document: DYNAMO THEORY AND EXPERIMENT Damon L. Ellingston, M.S., 2006 Directed By: Dr. Daniel P. Lathrop, Department of Physics Background and theory for the geodynamo is presented,

More information

Amplification of magnetic fields in core collapse

Amplification of magnetic fields in core collapse Amplification of magnetic fields in core collapse Miguel Àngel Aloy Torás, Pablo Cerdá-Durán, Thomas Janka, Ewald Müller, Martin Obergaulinger, Tomasz Rembiasz Universitat de València; Max-Planck-Institut

More information

The VKS experiment: turbulent dynamical dynamos

The VKS experiment: turbulent dynamical dynamos The VKS experiment: turbulent dynamical dynamos Sébastien Aumaître, Michaël Berhanu, Mickaël Bourgoin, Arnaud Chiffaudel, François Daviaud, Bérengère Dubrulle, Stéphan Fauve, Louis Marié, Romain Monchaux,

More information

Energy transfers and magnetic energy growth in small-scale dynamo

Energy transfers and magnetic energy growth in small-scale dynamo Decemer 3 EPL, (3) doi:.9/9-7// www.epljournal.org Energy transfers and magnetic energy growth in small-scale dynamo Rohit Kumar (a), Mahendra K. Verma () and Ravi Samtaney (c) Department of Physics, Indian

More information

Passive, Active and Feedback Stabilization of Thick, Flowing Liquid Metal Walls

Passive, Active and Feedback Stabilization of Thick, Flowing Liquid Metal Walls 21 st MHD Control Workshop, San Diego, CA, November 7-9, 2016 Passive, Active and Feedback Stabilization of Thick, Flowing Liquid Metal Walls Francesco A. Volpe, S.M.H. (Taha) Mirhoseini Dept. Applied

More information

Profile SFR-57 RIGADYN LATVIA. Riga MHD Dynamo test facility. Institute of Physics University of Latvia (IPUL)

Profile SFR-57 RIGADYN LATVIA. Riga MHD Dynamo test facility. Institute of Physics University of Latvia (IPUL) Profile SFR-57 RIGADYN LATVIA GENERAL INFORMATION NAME OF THE ACRONYM COOLANT(S) OF THE LOCATION (address): OPERATOR CONTACT PERSON (name, address, institute, function, telephone, email): Riga MHD Dynamo

More information

Asymptotic theory for torsional convection in rotating fluid spheres

Asymptotic theory for torsional convection in rotating fluid spheres Under consideration for publication in J. Fluid Mech. 1 Asymptotic theory for torsional convection in rotating fluid spheres By KEKE Z H A N G 1, KAMENG L A M A N D DALI K O N G 3 1,3 College of Engineering,

More information

DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL

DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL DYNAMO THEORY: THE PROBLEM OF THE GEODYNAMO PRESENTED BY: RAMANDEEP GILL MAGNETIC FIELD OF THE EARTH DIPOLE Field Structure Permanent magnetization of Core? 80% of field is dipole 20 % is non dipole 2)

More information

Morphology of field reversals in turbulent dynamos

Morphology of field reversals in turbulent dynamos May EPL, 9 () 49 doi:.9/95-575/9/49 www.epljournal.org C. Gissinger,, E. Dormy and S. Fauve Laboratoire de Physique Statistique, Ecole Normale Supérieure, UPMC Université Paris 6, Université Paris Diderot,

More information

FDEPS Kyoto: Bibliography for the lecture notes. Planetary interiors: Magnetic fields, Convection and Dynamo Theory

FDEPS Kyoto: Bibliography for the lecture notes. Planetary interiors: Magnetic fields, Convection and Dynamo Theory FDEPS Kyoto: Bibliography for the lecture notes Planetary interiors: Magnetic fields, Convection and Dynamo Theory Chris Jones, University of Leeds, UK November 2017 1. Observational background to planetary

More information

Scope of this lecture ASTR 7500: Solar & Stellar Magnetism. Lecture 9 Tues 19 Feb Magnetic fields in the Universe. Geomagnetism.

Scope of this lecture ASTR 7500: Solar & Stellar Magnetism. Lecture 9 Tues 19 Feb Magnetic fields in the Universe. Geomagnetism. Scope of this lecture ASTR 7500: Solar & Stellar Magnetism Hale CGEG Solar & Space Physics Processes of magnetic field generation and destruction in turbulent plasma flows Introduction to general concepts

More information

ELEC9712 High Voltage Systems. 1.2 Heat transfer from electrical equipment

ELEC9712 High Voltage Systems. 1.2 Heat transfer from electrical equipment ELEC9712 High Voltage Systems 1.2 Heat transfer from electrical equipment The basic equation governing heat transfer in an item of electrical equipment is the following incremental balance equation, with

More information

Fluctuations of electrical conductivity: a new source for astrophysical magnetic fields

Fluctuations of electrical conductivity: a new source for astrophysical magnetic fields Fluctuations of electrical conductivity: a new source for astrophysical magnetic fields F. Pétrélis, A. Alexakis, C. Gissinger 1 1 Laboratoire de Physique Statistique, Ecole Normale Supérieure, CNRS, Université

More information

Lagrangian Statistics. of 3D MHD Convection. J. Pratt, W.-C. Müller. Boussinesq Simulation. Lagrangian. simulation. March 1, 2011

Lagrangian Statistics. of 3D MHD Convection. J. Pratt, W.-C. Müller. Boussinesq Simulation. Lagrangian. simulation. March 1, 2011 March 1, 2011 Our approach to the Dynamo Problem dynamo action: amplification of magnetic fields by turbulent flows, generation of large scale structures collaboration with the group of Schüssler et al.

More information

MAGNETOHYDRODYNAMICS Vol. 38 (2002), No. 1-2, pp

MAGNETOHYDRODYNAMICS Vol. 38 (2002), No. 1-2, pp MAGNETOHYDRODYNAMICS Vol. 38 (22), No. 1-2, pp. 143 162 NON-STATIONARY SCREW FLOW IN A TOROIDAL CHANNEL: WAY TO A LABORATORY DYNAMO EXPERIMENT P. Frick, V. Noskov, S. Denisov, S. Khripchenko, D. Sokoloff,

More information

NONLINEAR BEHAVIOR OF A NON-HELICAL DYNAMO

NONLINEAR BEHAVIOR OF A NON-HELICAL DYNAMO NONLINEAR BEHAVIOR OF A NON-HELICAL DYNAMO Pablo D. Mininni 1, Yannick Ponty 2, David C. Montgomery 3, Jean-Francois Pinton 4, Helene Politano 2, and Annick Pouquet 1 ABSTRACT A three-dimensional numerical

More information

Numerical simulation of the Gailitis dynamo David Moss 1 School of Mathematics University of Manchester Oxford Rd Manchester M13 9PL UK

Numerical simulation of the Gailitis dynamo David Moss 1 School of Mathematics University of Manchester Oxford Rd Manchester M13 9PL UK Abstract Numerical simulation of the Gailitis dynamo David Moss 1 School of Mathematics University of Manchester Oxford Rd Manchester M13 9PL UK The linear magnetohydrodynamic equations are solved with

More information

Suppression of Temperature Fluctuations by Rotating Magnetic Field in a Large Scale Rayleigh-Bénard Cell

Suppression of Temperature Fluctuations by Rotating Magnetic Field in a Large Scale Rayleigh-Bénard Cell International Scientific Colloquium Modelling for Material Processing Riga, September 16-17, 2010 Suppression of Temperature Fluctuations by Rotating Magnetic Field in a Large Scale Rayleigh-Bénard Cell

More information

Convective Mass Transfer

Convective Mass Transfer Convective Mass Transfer Definition of convective mass transfer: The transport of material between a boundary surface and a moving fluid or between two immiscible moving fluids separated by a mobile interface

More information

The azimuthal MRI in experiment: confirmations and surprises

The azimuthal MRI in experiment: confirmations and surprises Max-Planck-Princeton Center for Plasma Physics General Meeting, Berlin, June 28 July 1, 2014 The azimuthal MRI in experiment: confirmations and surprises Frank Stefani with thanks to V. Galindo, O. Kirillov,

More information

Dynamo regimes and transitions in the VKS experiment

Dynamo regimes and transitions in the VKS experiment EPJ manuscript No. (will be inserted by the editor) Dynamo regimes and transitions in the VKS experiment M. Berhanu 1, G. Verhille 2, J. Boisson 4, B. Gallet 1, C. Gissinger 1, S. Fauve 1, N. Mordant 1,

More information

Turbulence in geodynamo simulations

Turbulence in geodynamo simulations Turbulence in geodynamo simulations Nathanaël Schaeffer, A. Fournier, D. Jault, J. Aubert, H-C. Nataf,... ISTerre / CNRS / Université Grenoble Alpes Journée des utilisateurs CIMENT, Grenoble, 23 June 2016

More information

Dynamo regimes and transitions in the VKS experiment

Dynamo regimes and transitions in the VKS experiment EPJ manuscript No. (will be inserted by the editor) Dynamo regimes and transitions in the VKS experiment M. Berhanu 1, G. Verhille 2, J. Boisson 4, B. Gallet 1, C. Gissinger 1, S. Fauve 1, N. Mordant 1,

More information

BAE 820 Physical Principles of Environmental Systems

BAE 820 Physical Principles of Environmental Systems BAE 820 Physical Principles of Environmental Systems Stokes' law and Reynold number Dr. Zifei Liu The motion of a particle in a fluid environment, such as air or water m dv =F(t) - F dt d - 1 4 2 3 πr3

More information

Scaling laws for dynamos in rotating spheres: from planets to stars

Scaling laws for dynamos in rotating spheres: from planets to stars Scaling laws for dynamos in rotating spheres: from planets to stars Ulrich Christensen Max Planck Institute for Solar System Research, Katlenburg- Lindau, Germany In collaboration with: Julien Aubert,

More information

FORMULA SHEET. General formulas:

FORMULA SHEET. General formulas: FORMULA SHEET You may use this formula sheet during the Advanced Transport Phenomena course and it should contain all formulas you need during this course. Note that the weeks are numbered from 1.1 to

More information

ON VARIABLE LAMINAR CONVECTIVE FLOW PROPERTIES DUE TO A POROUS ROTATING DISK IN A MAGNETIC FIELD

ON VARIABLE LAMINAR CONVECTIVE FLOW PROPERTIES DUE TO A POROUS ROTATING DISK IN A MAGNETIC FIELD ON VARIABLE LAMINAR CONVECTIVE FLOW PROPERTIES DUE TO A POROUS ROTATING DISK IN A MAGNETIC FIELD EMMANUEL OSALUSI, PRECIOUS SIBANDA School of Mathematics, University of KwaZulu-Natal Private Bag X0, Scottsville

More information

ES265 Order of Magnitude Phys & Chem Convection

ES265 Order of Magnitude Phys & Chem Convection ES265 Order of Magnitude Phys & Chem Convection Convection deals with moving fluids in which there are spatial variations in temperature or chemical concentration. In forced convection, these variations

More information

Geomagnetic Dynamo Theory

Geomagnetic Dynamo Theory Max Planck Institute for Solar System Research Katlenburg-Lindau, Germany International School of Space Science Geomagnetism and Ionosphere L Aquila, Italy 7-11 April 2008 Outline Introduction 1 Introduction

More information

The Lorentz force effect on the On-Off dynamo intermittency

The Lorentz force effect on the On-Off dynamo intermittency The Lorentz force effect on the On-Off dynamo intermittency Alexandros Alexakis, Yannick Ponty To cite this version: Alexandros Alexakis, Yannick Ponty. The Lorentz force effect on the On-Off dynamo intermittency.

More information

Turbulent three-dimensional MHD dynamo model in spherical shells: Regular oscillations of the dipolar field

Turbulent three-dimensional MHD dynamo model in spherical shells: Regular oscillations of the dipolar field Center for Turbulence Research Proceedings of the Summer Program 2010 475 Turbulent three-dimensional MHD dynamo model in spherical shells: Regular oscillations of the dipolar field By R. D. Simitev, F.

More information

HARMONIC AND SUBHARMONIC SOLUTIONS OF THE ROBERTS DYNAMO PROBLEM. APPLICATION TO THE KARLSRUHE EXPERIMENT

HARMONIC AND SUBHARMONIC SOLUTIONS OF THE ROBERTS DYNAMO PROBLEM. APPLICATION TO THE KARLSRUHE EXPERIMENT MAGNETOHYDRODYNAMICS Vol. 38 (2002), No. -2, pp. 95 06 HARMONIC AND SUBHARMONIC SOLUTIONS OF THE ROBERTS DYNAMO PROBLEM. APPLICATION TO THE KARLSRUHE EXPERIMENT F. Plunian, K.-H. Rädler 2 Laboratoires

More information

Numerical simulation of a spherical dynamo excited by a flow of von Kármán type

Numerical simulation of a spherical dynamo excited by a flow of von Kármán type Geophysical and Astrophysical Fluid Dynamics Vol. 104, Nos. 2 3, April June 2010, 207 220 Numerical simulation of a spherical dynamo excited by a flow of von Kármán type PAUL H. ROBERTSy, GARY A. GLATZMAIER*z

More information

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 3 August 2004

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 3 August 2004 ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 3 August 004 Final Examination R. Culham This is a 3 hour, closed-book examination. You are permitted to use one 8.5 in. in. crib sheet (both sides),

More information

On the Generation of Core Dynamo Action

On the Generation of Core Dynamo Action On the Generation of Core Dynamo Action CIDER Meeting, KITP 7/7/16 Jonathan Aurnou UCLA Earth & Space Sciences aurnou@ucla.edu Beyond record players? Treat core dynamics as a rotating magnetoconvection

More information

NUMERICAL SIMULATIONS OF CURRENT GENERATION AND DYNAMO EXCITATION IN A MECHANICALLY-FORCED, TURBULENT FLOW. R. Adam B. Bayliss

NUMERICAL SIMULATIONS OF CURRENT GENERATION AND DYNAMO EXCITATION IN A MECHANICALLY-FORCED, TURBULENT FLOW. R. Adam B. Bayliss NUMERICAL SIMULATIONS OF CURRENT GENERATION AND DYNAMO EXCITATION IN A MECHANICALLY-FORCED, TURBULENT FLOW by R. Adam B. Bayliss A dissertation submitted in partial fulfillment of the requirements for

More information

Planetary interiors: Magnetic fields, Convection and Dynamo Theory 3. How planetary magnetic fields are generated

Planetary interiors: Magnetic fields, Convection and Dynamo Theory 3. How planetary magnetic fields are generated Planetary interiors: Magnetic fields, Convection and Dynamo Theory 3. How planetary magnetic fields are generated Chris Jones, Department of Applied Mathematics University of Leeds UK FDEPS Lecture 3,

More information

Nonlinear Analysis: Modelling and Control, 2008, Vol. 13, No. 4,

Nonlinear Analysis: Modelling and Control, 2008, Vol. 13, No. 4, Nonlinear Analysis: Modelling and Control, 2008, Vol. 13, No. 4, 513 524 Effects of Temperature Dependent Thermal Conductivity on Magnetohydrodynamic (MHD) Free Convection Flow along a Vertical Flat Plate

More information

Zonal shear and super-rotation in a magnetized spherical Couette flow experiment

Zonal shear and super-rotation in a magnetized spherical Couette flow experiment Zonal shear and super-rotation in a magnetized spherical Couette flow experiment Daniel Brito, Thierry Alboussière, Philippe Cardin, Nadège Gagnière, Dominique Jault, Patrick La Rizza, Jean-Paul Masson,

More information

Intermittency in spiral Poiseuille flow

Intermittency in spiral Poiseuille flow Intermittency in spiral Poiseuille flow M. Heise, J. Abshagen, A. Menck, G. Pfister Institute of Experimental and Applied Physics, University of Kiel, 2498 Kiel, Germany E-mail: heise@physik.uni-kiel.de

More information

List of publications cited in the 2018 FDEPS Course

List of publications cited in the 2018 FDEPS Course List of publications cited in the 2018 FDEPS Course Henri-Claude Nataf Univ Grenoble Alpes, Univ Savoie Mont Blanc, CNRS, IRD, IFSTTAR, ISTerre, 38000 Grenoble, France November 27-30, 2018 1 Overview and

More information

Joule Heating Effect on the Coupling of Conduction with Magnetohydrodynamic Free Convection Flow from a Vertical Flat Plate

Joule Heating Effect on the Coupling of Conduction with Magnetohydrodynamic Free Convection Flow from a Vertical Flat Plate Nonlinear Analysis: Modelling and Control, 27, Vol. 12, No. 3, 37 316 Joule Heating Effect on the Coupling of Conduction with Magnetohydrodynamic Free Convection Flow from a Vertical Flat Plate M. A. Alim

More information

EXAMPLE SHEET FOR TOPIC 3 AUTUMN 2013

EXAMPLE SHEET FOR TOPIC 3 AUTUMN 2013 EXAMPLE SHEET FOR TOPIC ATMN 01 Q1. se dimensional analysis to investigate how the capillary rise h of a liquid in a tube varies with tube diameter d, gravity g, fluid density ρ, surface tension σ and

More information

Contributions to the theory of a two-scale homogeneous dynamo experiment

Contributions to the theory of a two-scale homogeneous dynamo experiment Contributions to the theory of a two-scale homogeneous dynamo experiment Karl-Heinz Rädler Astrophysical Institute of Potsdam, An der Sternwarte 16, D-14482 Potsdam, Germany Axel Brandenburg NORDITA, Blegdamsvej

More information

Problem 4.3. Problem 4.4

Problem 4.3. Problem 4.4 Problem 4.3 Problem 4.4 Problem 4.5 Problem 4.6 Problem 4.7 This is forced convection flow over a streamlined body. Viscous (velocity) boundary layer approximations can be made if the Reynolds number Re

More information

Analysis of Turbulent Free Convection in a Rectangular Rayleigh-Bénard Cell

Analysis of Turbulent Free Convection in a Rectangular Rayleigh-Bénard Cell Proceedings of the 8 th International Symposium on Experimental and Computational Aerothermodynamics of Internal Flows Lyon, July 2007 Paper reference : ISAIF8-00130 Analysis of Turbulent Free Convection

More information

Energy transfers during dynamo reversals

Energy transfers during dynamo reversals December 213 EPL, 14 (213) 692 doi: 1.129/295-575/14/692 www.epljournal.org Energy transfers during dynamo reversals Pankaj Mishra 1, Christophe Gissinger 1, Emmanuel Dormy 2 and Stephan Fauve 1 1 Laboratoire

More information

Table of Contents. Foreword... xiii. Preface... xv

Table of Contents. Foreword... xiii. Preface... xv Table of Contents Foreword.... xiii Preface... xv Chapter 1. Fundamental Equations, Dimensionless Numbers... 1 1.1. Fundamental equations... 1 1.1.1. Local equations... 1 1.1.2. Integral conservation equations...

More information

VARYING THE SPHERICAL SHELL GEOMETRY IN ROTATING THERMAL CONVECTION

VARYING THE SPHERICAL SHELL GEOMETRY IN ROTATING THERMAL CONVECTION Geophysical and Astrophysical Fluid Dynamics Vol. 98, No. 2, April 2004, pp. 153 169 VARYING THE SPHERICAL SHELL GEOMETRY IN ROTATING THERMAL CONVECTION F.M. AL-SHAMALI a, *, M.H. HEIMPEL a and J.M. AURNOU

More information

HEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1

HEAT TRANSFER BY CONVECTION. Dr. Şaziye Balku 1 HEAT TRANSFER BY CONVECTION Dr. Şaziye Balku 1 CONDUCTION Mechanism of heat transfer through a solid or fluid in the absence any fluid motion. CONVECTION Mechanism of heat transfer through a fluid in the

More information

Low dimensional turbulence

Low dimensional turbulence Low dimensional turbulence F. Daviaud in collaboration with A. Chiffaudel, B. Dubrulle P.-P. Cortet, P. Diribarne, D. Faranda, E. Herbert, L. Marié, R. Monchaux, F. Ravelet, B. Saint-Michel, C. Wiertel

More information