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Formation%20of%20the%20Earth%20and%20the%20Terrestrial%20Planets

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Title: Formation%20of%20the%20Earth%20and%20the%20Terrestrial%20Planets


1
Formation of the Earth and the Terrestrial Planets
2
  • Lets start with topics that we wont talk about
    at any great length in this course
  • First, one has to form the universe (the Big
    Bang)
  • Then, one needs to form galaxies
  • Then, one needs to form stars ?

3
Orion Nebula
Photo from HST
  • The Orion nebula is a dense interstellar
  • cloud of gas and dust in which stars are
  • being formed

http//www.greatdreams.com/cosmic/orion852.jpg
4
Eagle Nebula (Pillars of Creation)
From Hubble Space Telescope
5
Horsehead Nebula (also from HST)
http//forums.airbase.ru/cache/sites/a/n/antwrp.gs
fc.nasa.gov/apod/image/0310/468x468/horsehead_cfht
.jpg
6
Cloud collapse/disk formation
  • Then, one needs to form disks (circumstellar
    nebulae)
  • This happens quite naturally if the interstellar
    material was spinning ?

http//www.aerospaceweb.org/question/ astronomy/so
lar-system/formation.jpg
7
Oort Cloud Kuiper Belt
http//www.harmsy.freeuk.com/oimages/oort_cloud.jp
g
  • The Solar System also includes comets, both
    within the Kuiper Belt
  • (within the disk) and the Oort Cloud
    (spherical shell)

8
Early stages of planet formation
  • Dust settles to the midplane of the solar nebula
  • The dust orbits slightly faster than the gas
    because it doesnt feel the effects of pressure
  • Gas drag causes some of the dust to spiral
    inwards
  • Turbulence is generated, lifting some of the
    dust out of the midplane
  • If the dust density is great enough, then
    gravitational instability sets in, forming
    km-size planetesimals

Chambers, EPSL (2004), Fig. 1
9
Bipolar outflows
From The New Solar System, ed. 4, J.K Beatty et
al., eds., p. 16
  • Material falls into the star along the midplane
    of the disk and is
  • ejected towards the poles of the star
  • Mass flows inward, angular momentum outward

10
Runaway growth stage
  • Initially, the planetesimals were small
  • Collisions make them grow if the relative
    velocities are small
  • Dynamical friction keeps orbits circular and
    relative velocities low
  • Gravitational focusing causes the largest bodies
    to grow the fastest
  • Runaway growth of planetary embryos

Chambers, EPSL (2004), Fig. 2
11
Inner Solar System Evolution
Morbidelli et al., Meteoritics Planetary Sci.
(2000), Fig. 1
12
Eccentricity e b/a a 1/2 major axis b 1/2
distance between foci Sun-Earth
distances Aphelion 1 e Perihelion 1 - e
Today e 0.017 Range 0 to 0.06 Cycles
100,000 yrs


b
a
13
Final stage of accretion
Chambers, EPSL (2004), Fig. 3
  • Results of four different simulations. Segments
    in the pie chart show
  • the fraction of material coming from different
    parts of the Solar System.

14
  • Back to generalities. Lets look at the results
    of planetary formation in more detail

15
Titius-Bode Law
Ref. J. K. Beatty et al., The New Solar System
(1999), Ch. 2.
  • The logarithmic, or geometric, spacing is
    probably not an accident! The Solar
  • System is packed, i.e., it holds as many
    planets as it can. If one tries to stick
  • even a small planet inside it (except in the
    asteroid belt), it will be ejected.

16
Different planetary types
  • There is a pattern to the planets in our Solar
    System
  • Small, rocky planets on the inside
  • Gas giant planets in the middle
  • Ice giant planets on the outside
  • Why does this happen this way, and should we
    expect this same pattern to apply elsewhere?

318 ME
95 ME
14.5 ME
17.2 ME
1 ME
17
Solar nebula composition
Ref. J. K. Beatty et al., The New Solar System
(1999), Ch. 14.
  • The solar nebula is assumed to have the same
    elemental composition
  • as the Sun
  • Well talk later about how solar composition is
    obtained
  • Different compounds condense out at different
    temperatures

18
Condensation sequence(high temperatures to low)
  1. Refractory oxides (CaTiO3, Ca2Al2SiO7, MgAl2O4)
  2. Metallic Fe-Ni alloy
  3. MgSiO3 (enstatite)
  4. Alkali aluminosilicates
  5. FeS (troilite)
  6. FeO-silicates
  7. Hydrated silicates (kinetically inhibited)

Ref. Lewis and Prinn, Planets and their
Atmospheres (1984), p. 60
19
Condensation sequence (cont.)
  • 8. H2O
  • 9. NH3
  • 10. CH4
  • 11. H2
  • He
  • Collectively, these last 5 compounds (or
    elements) are referred to as volatiles because
    they are either liquids or gases at room
    temperature
  • Volatiles are important, as they are the
    compounds on which life depends most strongly
  • So, how did planets acquire them?

20
Equilibrium condensation model
  • 1 M? solar nebula (which is
  • too high!)
  • -- Nebula would be unstable if
  • over 0.1 M?
  • -- Minimum mass solar nebula
  • ? 0.03 M?
  • The curve along which the
  • planets lie is an adiabat running
  • along the midplane of the
  • nebula

Venus
Earth
Mars
Ref. J. S. Lewis and R. G. Prinn, Planets and
Their Atmospheres (1984)
21
Problems with the equilibrium condensation model
  • Assumed nebular mass (and thus pressure) was too
    high
  • Formation of hydrated silicates is kinetically
    inhibited
  • Gas-solid reactions are slow
  • Actual planetary accretion problem is
    time-dependent
  • The equilibrium condensation model applies only
    at a given instant in time
  • Planetesimals can move from one part of the solar
    nebula to another
  • This will be the key to understanding the origin
    of Earths volatiles
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