Spectrum and small-scale structures in MHD turbulence Joanne Mason, CMSO/University of Chicago
CMSO 2005 [email protected] Simulation of Gallium experiment * § Aleksandr Obabko Center for...
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Transcript of CMSO 2005 [email protected] Simulation of Gallium experiment * § Aleksandr Obabko Center for...
CMSO 2005
Simulation of Gallium experiment*§
Aleksandr Obabko
Center for Magnetic-Self OrganizationDepartment of Astronomy and Astrophysics
University of Chicago
*with Fausto Cattaneo (U of C) and Paul Fischer (ANL)§used NERSC resources supported by the Office of Science of the US DOE under Contract No.
DE-AC03-76SF00098 (INCITE 2005)
CMSO 2005
Problem formulation
PmReRmRRRR
Re
Rmt
pRet
,))((
0
1)()(
2
1)()(
122211
2
22
Bu
BuBBuB
BuBBuu
u
• Incompressible viscous resistive MHD equations in cylindrical geometry of MRI experiment at PPPL
• Boundary conditions:
0 ,
,0
,)( ,0
,0
zo,z
z
21
HzRRr
r
r
z
BBB
BB
rrVVV
• Solved numerically by MHD version of ANL spectral element code nek5000
22
214
2
2113
222
111
,
,
,
,
)(
Rrr
rRr
RrR
RrR
r
RR
RR
CMSO 2005
Overview of Results
• Periodic: Stable Couette flow for Bz0→0 & Bz0→∞, otherwise, MRI (for Rm>100…300)
• Rings diminish Ekman circulation (and torque) as compared to cases with lids & exhibit similar growth of torque with increase of Bz0
Rings setup is more suitable for study of MRI & angular momentum transport in laboratory
Torque / TorqueCouette
1.0
2.0
3.0
4.0
5.0
6.0
7.0
0.00 0.05 0.10 0.15 0.20 0.25 0.30
Bz0
Rings Re=6e3 T_i
Rings Re=6e3 T_o
Rings Re=2e3 T_i
Rings Re=2e3 T_o
Periodic Re=2e3
Periodic Re=6e3
Lids Re=2e3 Ti
Lids Re=6e3 Ti
• 2D & 3D hydro & MHD runs with vertical B.C. of periodicity, rings & lids• Re=620 … 6200, Pm=0.5 & Bz0=0 … 0.275
CMSO 2005
2D Steady Hydro Results for Re=620
• Angular momentum transport outward both by outward radial flow of high angular momentum and by inward radial flow of low angular momentum (like convection)
• Rings diminish Ekman circulation and hydro angular momentum transport restored Couette flow profile
zrF
rV
Lids: Rings:
V
Couette flow
Lids
Rings
Lids
Rings
zrF
CMSO 2005
2D Unsteady Results for Re=6200 with rings
• Smaller viscous boundary & shear layers• Oscillating vertical jets • Short radial jet outward at midplane of z=H/2
V
Couette flow
zrFzrF zrF
rV rV
CMSO 2005
2D MHD: Re=6200, Rm=3100, B0=0.05, rings
• The reversal of radial flow (toward the inner cylinder along the plane at z=H/2)• Higher torques compared to hydro case• Hydro angular momentum transport near boundaries, magnetic – near z=H/2
V
Couette flow
zrF
zrFrV zrMzrH
rV
rB
zrH zrMrB zrF
Total
Hydro
Magnetic
CMSO 2005
3D Results for Re=6200
• Initial conditions: 2D flow solutions• Weak 3D dimensionality in hydro cases
Similar angular momentum transport• Smaller structures compared to 2D cases
tzrF zr ,,, tzrF zr ,,
2D
Hydro with rings
3D
tzrF zr ,,, tzrF zr ,,
Periodic MHD, Bz0=0.05
2D 3D
CMSO 2005
Conclusion & Future Work
Conducted 2D & 3D Hydro & 2D MHD computations with vertical B.C. of periodicity, rings & lids in geometrical setup of Princeton MRI experiment
Observed diminished Ekman circulation and angular momentum transport in hydro cases with rings as compared to the cases with lids
Found similar behavior of torque with increase of external axial magnetic field Bz0 for 2D MHD cases with rings as compared to the periodic case with MRI
Suitability of the ring setup for study of MRI and angular momentum transport in laboratory
Angular momentum transport is reminiscent of transport of thermal energy in convection
…Ongoing 3D MHD calculations
…Plans for high-Re (~106) 2D MHD Case