Title: Galactic Dynamos and ISM Turbulence.
1Galactic Dynamos and ISM Turbulence.
- Steve Cowley,UCLA/ Imperial College
- Alex Schekochihin, Imperial
- Jim McWilliams, UCLA
- Greg Hammett, Princeton
- Greg Howes, UCLA/Imperial
- Russell Kulsrud, Princeton
- Ben Chandran, Univ. Iowa
- Jason Maron, Iowa/Rochester
- Sam Taylor, Imperial
2Outline
- Galactic Dynamos can they work? What can we do
to improve our knowledge of this kind of dynamo?
Experiments? Theory? Can we understand
anything if we dont solve everything. - ISM turbulence issues. Experiments? Theory.
3Field in M51.
Polarization of 6cm emission. Indicates
direction of B field.
Large scale coherent Field.
Beck 2000
4Theorists Milky Way
Vertical Field in Center B 1mG
Horizontal Field in Disc B 3?G
V
V
Scale Rotation time
Supernova explosion.
Scale Eddy turnover time
5Observed Density Fluctuations -- Small Scale
Turbulence.
- A spectrum of density fluctuations is inferred
from various radio scattering observations. It
has the classic k-5/3 spectrum from above the
mean free path to gyro-radius scales. This is
more than a whole talk in itself. - It is believed to be evidence of an MHD turbulent
cascade. Goldreich, Shridhar, Maron, Vishniac,
Lithwick, Lazarian,Boldyrev, . Etc.
6Galactic Dynamo -- The Usual Mechanism - Almost
Parker 1956
Coriolis Twist
7The Usual Mechanism - Almost
Parker 1956
Rotation Rate
w
Rotation Rate
8Velocity Spectrum -- with no B field
Kolmogorov 1941.
2
V
14
l
5
10
m
k
?
Viscous scale
-
5
/
3
k
Viscous eddy Turnover.
Helical part of spectrum
Smaller eddies turnover faster.
k
1
1
1
L
l
l
G
0
?
9The Large Prandtl Number Case Galaxies, Clusters
etc.
- Magnetic Prandtl number Pr ??? 1012 in
the ISM. THIS IS VERY DIFFERENT FROM THE SUN AND
EARTH WHERE Pr ltlt 1. - On the turnover time of the viscous eddies the
seed field grows. The field develops structure
below the viscous scale down to the resistive
scale l? Pr -1/2 l?
l
?
10Stage 1. Small Scale Dynamo
æ
k
5
(ln
k
)
3
g
t
ö
3
/
2
2
ç
2
B
(
k
,
t
)
exp
-
2
V
è
ø
1
/
2
t
4
g
t
4
k
Resistive scale Is very small-
6
l
10
m
R
1
1
1
1
L
l
l
l
G
0
D
R
11Large Pr Dynamo Numerical.
Schekochihin, SCC, McWilliams, Maron.
12Energy spectra Simulation and Theory
13Stage 2. The First Inverse Cascade?
Perhaps an approach to equipartition? I like
to think of untangling the small scales and
building the large scale field.
k
14No Numerical evidence for equipartition. No
Goldrich-Sridhar.
Stirring scale still folding Field lines.
Folded field lines - small scale energy.
Alfven waves on folded field lines?
15Folded Field saturated state.
16Stage 3. The Inverse Cascade?
17Helicity Will Save Us?
Coriolis Twist
18Helicity Will Save Us?
19Can the Helical Dynamo work when ltB2gt ltv2gt and
Helicity is small?
- One assumption is yes -- it is common to use the
?-? dynamo equations for the disk even though
there is no kinematic regime for the helical
galactic dynamo. - One old assumption was that the homogeneous
turbulence acts like a turbulent resistivity on
ltBgt and ltB2gt. It doesnt of course at high Pr. - Jason Maron and Eric Blackman looked at this in a
homogeneous box and got growth -- the resolution
was unavoidably low and Pr 1. - This is a significant question. I expect the
dynamo to be suppressed but ??
20Better simulations?
- Need geometry -- Greg Howes is doing disc
simulations. Buoyancy, shear. Galactic MRI? - Extra physics Ambipolar drift, tensor viscosity.
- Inhomogeneous ISM, clouds etc.
- RESOLUTION.
- I would be progress just to get the homogeneous
isotropic Pr1dynamo and steady state field
sorted out. (the MHD Kolmogorov problem)
21Sodium experiments?
- Prlt1 small scale dynamo may not exist -- see
Schekochihin submitted to PRL (see XXX). For
sodium Pr 10-4. - Only the helical dynamo.
- Relevant for the sun and geodynamo.
- Could try to increase sodium viscosity to reduce
Re. (temperature control fillings etc.)
22Plasma Prgt1 Dynamo experiments?
- Is the RFP dynamo relevant -- perhaps it is for
sustainment. - It would be nice to have a flow driven plasma
dynamo experiment. - I dont have a clue how to do that.