Title: Interstellar%20and%20Interplanetary%20Material
1Interstellar and Interplanetary Material
HST Astrobiology Workshop May 5-9, 2002 P.C.
Frisch University of Chicago
2Outline
- 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
3Heliosphere 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
4Solar 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
5Heliosphere 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)
6Heliosphere 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)
7Warm 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)
8Sun 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
9Heliosphere 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
10Solar 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
11Solar 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
12Heliosphere and IS cloud densitynHI0.22 /cc
nHI15 /cc
13Solar 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.
14Astrospheres.
- 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)
15Example 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
16Interstellar 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
17Interstellar 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)
18Interstellar 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)
19Interstellar 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
20Pickup Ions Gloeckler and Geiss (2002)
21Pickup ions become Anomalous Cosmic Rays (Figure
from ACE web site)
22Anomalous Cosmic RaysCummings and Stone (2002)
23Anomalous Cosmic Rays captured in Earths
magnetosphereFigure from ACE web site
24Pickup Ions, Anomalous Cosmic Rays,and the
ISM(Cummings and Stone 2002)
25Pickup Ions, Anomalous Cosmic Rays,and the
ISM(Cummings and Stone 2002)
26Interstellar 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.
27Entry of ISM into Heliosphere
28ISM 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
29Inner versus Outer PlanetsHeliosphere in n15
cm-3 cloudT (K) Ho
Density (cm-3)
30Cosmic 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
31Planetary climates and the interplanetary
environment.
- Galactic Cosmic Ray flux correlated with low
level (lt3.2 km) cloud cover (Marsh Svensmark
2002)
32Instantaneous 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)
33ConclusionsKnow 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?)