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Atmospheres of Hot Terrestrial Exoplanets. Laura Schaefer and Bruce Fegley, Jr. Planetary Chemistry Laboratory Department of Earth and Planetary Sciences Washington University, St. Louis, MO http://solarsystem.wustl.edu. What do we expect?.
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Atmospheres of Hot Terrestrial Exoplanets Laura Schaefer and Bruce Fegley, Jr. Planetary Chemistry Laboratory Department of Earth and Planetary Sciences Washington University, St. Louis, MO http://solarsystem.wustl.edu
What do we expect? • Extreme heating over a planet’s lifetime may lead to loss of volatiles • Venus is in a shorter orbit than the Earth and has lost its water content due to stellar heating and runaway greenhouse effect • Mercury: lost all volatiles (if it formed with any) • Jupiter’s moon Io is dominated by S, and may have lost lighter volatiles such as H, C, and N due to intense tidal heating • Expect a range of planets with variable volatile content • Silicate atmospheres (no volatiles!) • Super-Venus (CO2 atmosphere, trace water)
2600 K 50 K R = 1.67R M = 4.8M ρ ~ 5,600 CoRoT-7b • Tidally-locked transiting planet with a = 0.017 AU (0.85 days) • Dayside temperature is hot enough to melt and vaporize rock • Planet may have a partial magma ocean • Volatiles could have been blown away from the atmosphere or condensed on the cold nightside • Results in a net loss of elements from the magma ocean • Atmosphere may be composed of rock-forming elements
Silicate Atmosphere Calculations • MAGMA code calculates composition of silicate atmosphere • vaporization of systems containing Si, Mg, Fe, Ca, Al, Ti, Na, K, and O • As a function of: • temperature (1500 – 3000 K) • mass-loss by isothermal fractional vaporization • Results give composition and total pressure • Fractional vaporization may simulate • removal of material from dayside to nightside on CoRot-7b or • Loss of material from the atmosphere • We also calculate the composition of clouds, which may alter the atmospheric composition
Temperature-dependent results • Graph shows initial results for the BSE (Fvap = 0) • Column density (PiNA/μg) is calculated for a planet the size of CoRoT-7b (g ~16.7 m/s2) • Na is the major gas at all temperatures • O2, O, and SiO are also very abundant
2600 K 1800 K 2200 K Fractional Vaporization • Graph shows atmospheric composition as a function of fraction vaporized at constant temperature • Na is lost from system first, then K and Fe • SiO becomes major gas • Mg becomes more abundant than SiO at higher fractions vaporized • O and O2 maintain fairly constant abundance • Elements are lost less quickly as temperature increases
Silicate Clouds • We calculated cloud condensation temperatures (Tcond) for the atmosphere generated at 2200 K for the BSE model • Assumes dry adiabat and g ~ 36 m/s2 • Mg, Al, Si, Ca, and Fe may fall back to surface and be reincorporated in the magma ocean • Ti, Na, and K remain in atmosphere to high enough altitudes that they may either be transported to nightside or removed from atmosphere by stellar wind
Extended Na cloud • Large clouds of Na exist around Mercury and Jupiter’s moon Io • At Mercury, the Na cloud (~1011 cm-2) extends to ~23RMercury • At Io, the Na cloud (1010 - 1012 cm-2) extends to ~500RJupiter (~19,600RIo) • These clouds are very bright spectral features • An Earth-like exoplanet with a silicate atmosphere may have an extended Na cloud • Na is present in the atmosphere to high altitudes • may interact with stellar wind • A large Na cloud around a transiting planet like CoRoT-7b will occult more of the stellar disk than a closely bound atmosphere • Increases the probability of detection for a super-Earth • Na has already been detected in the atmospheres of several giant exoplanets (HD209458b, HD189733b)
Venus-like Exoplanets • Thick CO2 atmosphere, low H2O abundance • Either lost water, or never accreted water • Greenhouse effect = high surface T • Like Venus, may have surface-atmosphere equilibrium • Mineralogy of surface will buffer the abundances of gases in atmosphere • Abundances of several gases would help us narrow down possible mineralogy of the surface • CO2, H2O, HCl, and HF • CO difficult because of photochemistry • Sulfur-gases difficult due to condensation
Calcite - Quartz - Wollastonite CaCO3 + SiO2 = CaSiO3 + CO2 (g)
758 K 122 bars Eastonite – Spinel – Enstatite - Kalsilite KMg2Al3Si2O10(OH)2 = MgAl2O4 + MgSiO3 + KAlSiO4 + H2O XH2O = 30 ppm
Intersection of CO2 and H2O buffers depends on XH2O. Exact fit gives XH2O = 24 ppm.
Albite – Halite – Andalusite – Quartz 2HCl + 2NaAlSi2O6 = 2NaCl + Al2SiO5 + 3SiO2 + H2O 3. Identify possible HCl buffers. XHCl = 0.76 ppm
Leucite – Forsterite – Fluor-phlogopite –Enstatite 2 HF + KAlSi2O6 + 2Mg2SiO4 = KMg3AlSi3O10F2 + MgSiO3 + H2O 4. Identify possible HF buffers. XHF = 4.6 ppb
Albite Andalusite Calcite Diopside Eastonite Enstatite Fluor-phlogopite Forsterite Halite Kalsilite Leucite Nepheline Quartz Spinel Sodalite Wollastonite
To create theoretical exoplanets, find intersections of CO2 and H2O buffers. XH2O = 30 ppm Making a planet hotter than Venus is difficult without increasing XH2O significantly.
Albite Anorthite Enstatite Fluor-phlogopite Forsterite Halite Kalsilite Leucite Microcline Magnesite Phlogopite Sodalite Wollastonite Magnesite – Enstatite – Forsterite MgCO3 + MgSiO3 = Mg2SiO3 +CO2 XH2O = 1000 ppm Wollastonite – Sodalite – Halite – Anorthite – Albite 12HCl + 6CaSiO3 + 5Na4[AlSiO4]3Cl = 17NaCl + 6CaAl2Si2O8 + 3NaAlSi3O8 + 6H2O Microcline – Forsterite – Fluor-phlogopite – Enstatite 2HF + KAlSi3O8 + 3Mg2SiO4 = KMg3AlSi3O10F2 + 3MgSiO3 + H2O Phlogopite – Forsterite – Leucite – Kalsilite 2KMg3AlSi3O10(OH)2 = 3Mg2SiO4 + KAlSi2O6 + KAlSiO4 + 2H2O
Summary • Planets like CoRoT-7b may have silicate atmospheres • May have extensive Na cloud • Heating over time may deplete planet in more volatile elements • Super-Venus exoplanets may have atmosphere-surface equilibria • Observations of gas abundances would allow an estimate of surface composition • Hot Venus is difficult to make without increasing H2O abundance signficantly • Cold Venus is much easier to make