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Terrestrial Planets. II.

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Earth as a planet: interior & tectonics. Dynamics of the mantle Modeling terrestrial planets Earth interior Earth mantle convection simulation Earth interior - mantle ... – PowerPoint PPT presentation

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Title: Terrestrial Planets. II.


1
Terrestrial Planets. II.
  1. Earth as a planet interior tectonics.
  2. Dynamics of the mantle
  3. Modeling terrestrial planets

2
Earth interior
3
Earth mantle convection simulation
Labrosse Sotin (2002)
4
Earth interior - mantle plumes
5
Earth - cooling
6
Earth - cooling
7
Earth - cooling
8
Earth interior - cooling
9
Super-Earths
10
Searching for Small Planets
First Super-Earth discovered GJ 876d -- Mass
7.5 Earths Also HD 69830b -- Mass 10 Earths
NASA Kepler mission Radii in this range
after Gould et al. (2006)
M Mercury V Venus E Earth, etc.
11
What would we look for and could we measure
it ?
Illustrate with an example - planet GJ876d
12
What would we look for and could we measure
it ?
Illustrate with an example - planet GJ876d
  • GJ876 an M-dwarf (1/3 solar) with 3 planets
  • GJ876d - the first Super-Earth (7.5 Earth mass)
    discovered (Rivera et al. 2005)
  • Several possible models of GJ876d s interior -
    could we distinguish among them ?
  • If so, what tolerances in Radius Mass are
    needed ?

13
Interiors of Super-Earths
The models follow the techniques and many
assumptions of Earths model

TWO POINTS - Given a wide range of
cosmic compositions, the mineralogy
and differentiation do not vary - Their mantles
will consist mostly of the newly discovered
high-P phase of perovskite - post-pv
Schematic temperature profile
Tsuchiya et al. (2004) Valencia, Sasselov,
OConnell (2006)
14
Post-Perovskite
15
Interiors of Super-Earths
Valencia, Sasselov, OConnell (2006)
Ocean Planet
Earth-like
16
Interiors of Super-Earths
Mass-Radius relations for 11 different mineral
compositions (Earth-like)

Valencia, OConnell, Sasselov (2005)
1ME 2ME 5ME 10ME
17
Theoretical Error Budget
  • Planet Radius Errors
  • New high-P phases, e.g. ice-XI -0.4
  • EOS extrapolations (V vs. BM) 0.9
  • Iron core alloys (Fe vs. FeS) -0.8
  • Viscosity, f(T ) vs. const. 0.2
  • Overall the uncertainties are below 2
  • (at least, thats what is known now)

18
Interior Structure of GJ 876d
20,000
7.5 ME
DENSITY (kg/m3)
12,000
Valencia, Sasselov, OConnell (2006)
4,000
2,000
6,000
10,000
RADIUS (km)
19
Interior Structure of GJ 876d
Valencia, Sasselov, OConnell (2006)
20
Interior Structure of Super-Earths
Valencia, Sasselov, OConnell (2006)
21
Interior Structure of Super-Earths
Kepler error bar
Valencia, Sasselov, OConnell (2006)
22
Interior Structure of Super-Earths
Valencia, Sasselov, OConnell (2006)
23
What would we look for and could we measure
it ?
Could we measure the difference? - YES
We need at least 5 in Radius, and at
least 10 in Mass.
Work on tables for use with Kepler underway -
masses 0.4 to 15 ME
24
New Earths Facility
Synergy with KEPLER Provide ability to reach
RV amplitudes of about 20 cm /sec. Given Porb
and phase from transit, this can translate to 10
masses in the Super-Earth and Earths regime.
  • HARPS-NEF with Obs.Geneve
  • on a large telescope (WHT)
  • Use to measure masses, hence
  • mean densities, for KEPLERs candidates.

25
New Earths Facility
HARPS-South facts Requires T and P control 1
m/sec 15 nm 10-3 pix 0.01 K
0.01 mbar Obs. Run on a Cen B 52 cm/sec (one
night, 80 of that was p-modes), Obs. Run on
HD 69830d 20 cm/sec (over entire run).
26
HD 69830 b,c, d
Flux
HARPS
significant part of the error bars due to
stellar jitter - 20 to 80 cm/sec for HD 69830d
have residuals of 20 cm/sec over the 3-year run.
Lovis, Mayor, Pepe, et al. (2006)
Wavelength (microns)
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