Title: The Propagation Distance and Sources of Interstellar Turbulence
1The Propagation Distance and Sources of
Interstellar Turbulence
Steven R. Spangler
University of Iowa
2Entities responsible for Tiny Scale Structures
and Extreme Scattering Events are probably part
of interstellar plasma turbulence---solitary
waves or coherent structures.
The Diffuse Ionized Gas (DIG) is a partially
ionized plasma
3Graduate school courses in plasma physics are
usually restricted to the discussion of fully
ionized plasmas. Practitioners of the subject,
however, are aware of the fact that media of
research interest are not generally fully
ionized. Laboratory physicists know that neutral
gas is present and is a nuisance, in that it can
collisionally damp phenomena of interest.
Astronomers have a Manichean view of ionization
in the universe they assume that their media are
either completely neutral and obedient to the
laws of hydrodynamics, or completely ionized
and describable by single fluid
magnetohydrodynamics.
SRS, Physics of Plasmas 10, 2169, 2003
4An apparently important process in the
thermodynamics of the the DIG Ion-Neutral
Collisional Heating
Spangler 1991, ApJ 376,540 Minter and Spangler
1997, ApJ 485, 182
5Calculation of Collisional Heating Rate
6Calculation assumed spectrum of turbulence as
given, then calculated the heating rate as the
turbulence decays. No attempt to give
self-consistent description of turbulence.
7Implications for ISM Heating
Modification of Figure from Minter and Spangler
(1997), using solar-wind-derived CB2 instead of
Faraday rotation value
8A Gratifying Result
- Calculation suggests turbulent heating might
provide important process in the thermodynamics
of the interstellar medium. - Further discussion and support from data in
Minter and Balser, ApJ 484, L133, 1997
9An odd and undesired consequence of these ideas
the propagation distance of interstellar
turbulence
- Damping rate on neutral helium
S-1
Propagation distance of turbulence
Vastly smaller than typical distance to
hypothesized sources of turbulence
10Possible Explanations
- Unknown, local sources of interstellar turbulence
- Wave Percolation through a lacunose ISM
- Colossal physical misunderstanding
11The microphysics of ion-neutral damping
- Mechanism 1 induced dipole moment in neutral by
ion - Mechanism 2 charge exchange
- Astronomers can benefit from interest in plasma
physics ion-neutral interactions are important
in Tokamak confinement
12The Physics of Ion-Neutral Interactions I
- Interactions due to induced dipole moment of
neutral atoms - Collision frequency
Ion-neutral cross section
Cross sections
cm2
13The Physics of Ion-Neutral Interactions II
charge exchange
- Exchange creates fast neutral and slow ion
14Both processes relevant for conditions in the DIG
- It is probably worthwhile to revisit the
microphysics of MHD wave damping via ion-neutral
interactions
15Future Research Directions
- Detailed study of damping of MHD waves in a
partially ionized plasma, paying attention to
energy flow - Laboratory experiments to test those results
- Astronomical observational tests for anomalous
neutral heating in the DIG and similar ISM phases
16The Diffuse Ionized Gas (DIG) of the Interstellar
Medium
- Density 0.08 cc
- B field 3 microG
- T8000k
- VA23.3 km/sec
- Helium ionization 50-100 neutral
17Estimates of PB(k)
- Radio scintillations measurements sensitive only
to density n, not B or V - Minter and Spangler (1996 ApJ 458, 184) used
Faraday rotation to retrieve CB2 - Approach here use slow solar wind as a model
plasma to determine n-B relation
18Solar Wind Data
- Used Wind spacecraft data from NSSDC
- Analysed 50 intervals of one hour duration.
- All in slow solar wind (V lt 400 km/sec)
- Parameters calculated
19Empirical Compressibility Relation
20Application to Interstellar Medium
New estimate similar, but slightly higher than
MS96