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Title: Interstellar%20and%20Interplanetary%20Material


1
Interstellar and Interplanetary Material
HST Astrobiology Workshop May 5-9, 2002 P.C.
Frisch University of Chicago
2
Outline
  • The solar system is our template for
    understanding interplanetary material
  • Heliosphere, solar wind, ISM
  • Astrospheres
  • Interstellar and interplanetary matter
  • ISM affects planets inner vrs outer planets
  • 3D data visualization of solar motion

3
Heliosphere and ISM
  • About 98 of diffuse material in heliosphere is
    interstellar gas
  • Solar wind and interstellar gas densities are
    equal near Jupiter, or at 6 au

4
Solar Wind
  • Expanding solar corona becomes solar wind
  • At 1 au and solar max n(p)4 /cc, V 350
    km/s, B 2nT (20 mG)
  • SW density decreases by 1/R2 in solar system
  • SW sweeps up charged particles, including ISM

5
Heliosphere today
  • Top Plasma Temp
  • Bottom Interstellar Ho
  • Ho Wall Ho and p couple
  • Properties T29,000 K, N(Ho)3 x 1014 cm-2,
    dV-8 km/s
  • Model 4-fluid model
  • (Figure courtesy Hans Mueller)

6
Heliosphere vrs Planetary System
  • HELIOSPHERE
  • Warm Partially Ionized ISM surrounds Sun
    nHI0.22 /cc, nHeI0.12 /cc, n0.11 /cc, T6500
    K, VHC26 km/s (ionization must be modeled)
  • SW Termination Shock 75-90 au
  • Heliopause 140 au
  • Bow shock 250 au, M1.5 (?)
  • PLANETARY SYSTEM
  • Pluto 39 au
  • NASA Spacecraft
  • Voyager 1 84 au (in nose direction) (3.6
    au/year)
  • Voyager 2 66 au (in nose direction) (3.3
    au/year)
  • Pioneer 10 80 au (in tail direction)
  • ESA/NASA Ulysses 15 au, over poles of Sun
  • Future Spacecraft
  • Interstellar Probe ? 10-20 au/year in nose
    direction (Liewer and Mewaldt 2000)

7
Warm partially ionized diffuse interstellar cloud
around Sun
  • Observations of interstellar Heo in solar system
    give cloud properties (Witte et al. 2002, Flynn
    et al 1998)
  • nHeI0.014 /cc, T6,400 K, VHC26
    km/s
  • ISM radiative transfer models give composition
    and ionization at boundary heliosphere (Slavin
    Frisch 2002, model 18)
  • nHI0.24 /cc , ne0.09 /cc, H/H23,
    He/He45
  • Magnetic field strength lt3 mG (but unknown)
  • Over 1 of cloud mass is in interstellar dust
  • Observed upstream direction towards l5o, b14o.
  • This cloud referred to as Local Interstellar
    Cloud (LIC)

8
Sun in Local Bubble interior 106 Years Ago
  • ? Sun moves towards l28o, b32o, V13.4 km/s
  • (Dehnen Binney 1998)
  • ? Local Bubble densities nHIlt0.0005 cm-3
  • nHII0.005 cm-3
  • T106 K

9
Heliosphere while in Local Bubble Plasma(Figure
courtesy Hans Mueller)
  • Sun in Fully Ionized Local Bubble Plasma
  • Relative V13.4 km/s
  • TInterstellar106.1 oK
  • n(p)IS0.005 cm-3
  • n(Ho)IS0 cm-3
  • No IS neutrals in heliosphere

10
Solar Environment varies with Time
  • ?Sun entered outflow of diffuse ISM from Sco-Cen
    Association (SCA) 103-105 years ago
  • LSR Outflow 17 /- 5 km/s from upstream
    direction
  • l2.3o, b-5.2o
  • ISM surrounding solar system now is warm
    partially ionized gas.
  • Solar path towards l28o, b32o implies Sun
    will be in SCA outflow for million years in
    future.
  • Denser ISM will shrink heliosphere to radius
    ltlt100 au

11
Solar Encounter with Interstellar Clouds
  • Sun predicted to encounter about a dozen giant
    molecular clouds over lifetime,
  • Encounters with n10 cm-3 interstellar clouds
    will be much more frequent.
  • An increase to n10 cm-3 for the cloud around the
    Sun would (Zank and Frisch 1998)
  • Contract heliopause to radius of 14 au
  • Increase density of neutrals at 1 au to 2 cm-3
  • Give a Rayleigh-Taylor unstable heliopause from
    variable mass loading of solar wind by pickup ions

12
Heliosphere and IS cloud densitynHI0.22 /cc
nHI15 /cc
13
Solar Encounter with Interstellar Clouds
  • Sun moves through LSR at 13.4 km/s, or 13.4
    pc/106 years.
  • 96 interstellar absorption components are seen
    towards 60 nearby stars which sample interstellar
    cloudlets within 30 pc of Sun (F02).
  • Nearest stars show 1 interstellar absorption
    component per 1.4-1 .6 pc.
  • Relative Sun-cloud velocities of 0-32 km/s
    suggest variations in the galactic environment of
    the Sun on timescales lt50,000 years.

14
Astrospheres.
  • Cool star mass loss gives astrospheres with
    properties determined by interactions with the
    ISM and sensitive to interstellar pressure
    (Frisch 1993)
  • a Cen mass loss rate of 10-14 MSun/year (Wood et
    al. 2001)
  • Heated interstellar Ho in solar heliosheath
    (25,000 K) see towards a Cen AB and other stars
    (e.g. Linsky, Wood)
  • Astrospheres found around a Cen AB (1.3 pc), e
    Ind (3 pc), l And (?, 23 pc), and other stars
    (Linsky Wood 1996,Gayley et al. 1997, Wood et
    al. 1996)

15
Example Sun a Cen Heliosheath
  • Interstellar Lya absorption shows redward
    shoulder from decelerated Ho
  • Interstellar Ho and p couple by charge exchange
  • Ho heated to 29,000 K, N(Ho)3 x 1014 cm-2, dV
    -8 km/s
  • Gayley et al. 1997

16
Interstellar and Interplanetary Material
Observations of ISM in the Solar System
  • Ho /Heo fluorescence of solar Lya/584A emission
    (1971, many satellites)
  • Heo Ulysses
  • Dust Ulysses, Galileo, Cassini
  • Pickup Ions Ampte, Ulysses
  • Anomalous Cosmic Rays e.g. Ulysses, ACE, many
    other spacecraft

17
Interstellar Ho in Solar System
  • Ho Solar Lya photons fluorescing on
    interstellar Ho at 4 au
  • Discovered 1971 (Thomas, Krassa, Bertaux,
    Blamont)
  • Ho decelerated in solar system (by 5 km/s)
  • Left Interstellar Ho
  • Right Geocorona
  • (Copernicus data, Adams and Frisch 1977)

18
Interstellar Heo in Solar System
  • Heo Solar 584 A fluorescence on interstellar
    Heo at 0.5 au
  • Discovered 1974 (Weller and Meier)
  • Heo atoms measured directly by Ulysses
  • Best data on interstellar gas inside solar system
  • n(Heo)0.014 /cc, T6,400 K, V26 km/s, observed
    upstream at l5o, b14o (Witte 2002)

19
Interstellar Heo in Solar System
  • Interstellar He gravitationally focused
    downstream of the Sun.
  • The Earth passes through the Helium focusing cone
    at the beginning of December.
  • Density enhancement in cone

20
Pickup Ions Gloeckler and Geiss (2002)
21
Pickup ions become Anomalous Cosmic Rays (Figure
from ACE web site)
22
Anomalous Cosmic RaysCummings and Stone (2002)
23
Anomalous Cosmic Rays captured in Earths
magnetosphereFigure from ACE web site
24
Pickup Ions, Anomalous Cosmic Rays,and the
ISM(Cummings and Stone 2002)
25
Pickup Ions, Anomalous Cosmic Rays,and the
ISM(Cummings and Stone 2002)
26
Interstellar Dust
  • Smallest grains filtered in outer heliosphere
    (lt0.1mm)
  • Medium grains filtered by solar wind (0.1-0.2 mm)
  • Large grains constitute 30 of interplanetary
    grain flux with masses gt10-13 gr (or radiusgt0.2
    mm) at 1 au.
  • 1 of the cloud mass in dust
  • Work by Gruen, Landgraf et al.

27
Entry of ISM into Heliosphere
28
ISM effects on planets
  • Inner versus Outer Planets (Ho)
  • Cosmic rays
  • ?Anomalous cosmic rays (require neutral ISM)
  • ?Galactic Cosmic Rays (sensitive to heliosphere
    B)
  • In principle, core samples on inner versus outer
    planets would sort solar variations from
    interstellar variations

29
Inner versus Outer PlanetsHeliosphere in n15
cm-3 cloudT (K) Ho
Density (cm-3)
30
Cosmic Rays and Sunspot numbersClimax, Co. data
0.5-200 GeV/nucleii(figure courtesy Cliff
Lopate)
  • Cosmic ray fluxes at Earth coupled to solar cycle
    (through solar magnetic field)
  • Encounter with dense interstellar cloud decreases
    heliosphere dimensions by order of magnitude and
    will alter cosmic ray flux at Earth

31
Planetary climates and the interplanetary
environment.
  • Galactic Cosmic Ray flux correlated with low
    level (lt3.2 km) cloud cover (Marsh Svensmark
    2002)

32
Instantaneous 3D visualization of Hipparcos
catalog stars and MHD heliosphere model. Credits
  • Data Hipparcos catalog of stars, A. Mellinger
    Milky Way Galaxy photage, Heliosphere MHD model
    of T. Linde (U. Chicago)
  • Video A. Hanson (Indiana U., producer), P.
    Frisch (U. Chicago, scientist)
  • Funding NASA AISRP grant 5-8163 (U. Chicago)

33
ConclusionsKnow your astrosphere
  • A stellar astrosphere and the interplanetary
    environment of an extrasolar planetary system
    depend on both the stellar wind and the
    properties of the interstellar cloud surrounding
    the star.
  • Inner and outer planets see different fluxes of
    ISM over time.
  • Astrospheres change when stars encounter
    different interstellar clouds.
  • Star-planet coupling is function of surrounding
    ISM (and perhaps climate?)
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