Bleachworld: Atmospheric Evolution of Water Worlds
Transcription
Bleachworld: Atmospheric Evolution of Water Worlds
Bleachworld, AGU Fall Meeting 2011 Bleachworld: Atmospheric Evolution of Water Worlds Raymond T. Pierrehumbert The University of Chicago Eric Gaidos University of Hawaii 1 Bleachworld, AGU Fall Meeting 2011 The water loss scenario • With sufficiently large insolation, get hot, moist upper atmosphere • H2O exposed to UV, photolyzes to H and O • H is lost to space, O2 reacts with rocks • Then it’s game over for your ocean and life But what if there are no rocks to serve as a sink for O2? 2 Bleachworld, AGU Fall Meeting 2011 For this talk, a Waterworld is ... A planet with an ocean sufficiently deep that its rocky core does not lead to significant oxidative weathering. 3 Bleachworld, AGU Fall Meeting 2011 We are interested because ... • O2 back reaction could inhibit ocean loss from habitable-zone planets orbiting M stars during, active early stage of M star evolution • And we’d like to understand ... 4 Bleachworld, AGU Fall Meeting 2011 The case of GJ1214b • Old M-star, Tef f = 3026K • Low density super-Earth. Water-dominated composition? • Mass equivalent to 26,000 Earth oceans • Close orbit. L~ = 22000W/m2 = 16L • This puppy should be blasting out hydrogen like gangbusters! • Transit IR spectroscopy → No H2 envelope (Bean et al, w/ caveats) 5 Bleachworld, AGU Fall Meeting 2011 Dramatis Personae • The Radicals: OH, HO2,O1D • The Moderates: O3P,H,O3 • The Conservatives: H2O,H2,O2,H2O2 6 Bleachworld, AGU Fall Meeting 2011 How to re-form water? H + HO2 → OH + OH → O3P + H2O H + HO2 → O(3P) + H2O H + HO2 → O2 + H2 OH + O3 → HO2 + O2 H + O2 + M → HO2 7 Bleachworld, AGU Fall Meeting 2011 Ozone and its consequences O(3P) + O2 + M → O3 O3 + hν(NUV) → O(1D) + O2 O1D breaks up H2 (and lots of other stuff) 8 Bleachworld, AGU Fall Meeting 2011 A two-layer toy photochemistry model EUV,FUV NUV H2O Photolysis layer H2O H O3 H2O O2 H2O H2O2 H2 OH O(3P) H HO2 O3 O(1D) OH Reformation layer O2 9 Bleachworld, AGU Fall Meeting 2011 First look at photolysis layer (p = .004Pa) EUV,FUV NUV H2O Photolysis layer H2O H O3 H2O O2 H2O H2O2 H2 OH O(3P) H HO2 O3 O(1D) OH Reformation layer O2 10 Bleachworld, AGU Fall Meeting 2011 G star photon flux absorbed by H2O 2 Absorbed Flux, photons/m /s EUV 10 16 10 14 10 12 10 10 FUV Ly-α Flux Density Abs. flux Blackbody Abs. flux, Obs. Sun 8 10 0 50 100 150 wavelength (nm) 200 250 2 Bars H O per billion years 5 10 Cumulative Flux 4 10 1000 100 10 Cum. Flux, Blackbody Cum. Flux, Obs. Sun 1 0.1 0 50 100 150 wavelength (nm) 200 250 11 Bleachworld, AGU Fall Meeting 2011 For M stars, H2O photolysis dominated by Ly-α 7 Total Mass GJ1214b 6 10 5 10 GJ1214b insolation 4 10 Earthlike insolation 1000 Earth Ocean 100 Young M 10 -2.5 -3 Sun Lyman-α photolysis (bars/Gyr) 10 Old M -3.5 -4 -4.5 Log(R-Ly) -5 -5.5 -6 12 Bleachworld, AGU Fall Meeting 2011 Not much chemistry goes on in the photolysis layer 12 -3 Particle density ( cm ) 2 10 1.5 10 H2O O2 H O3P 12 12 1 10 11 5 10 0 0 6 5 10 7 1 10 7 7 1.5 10 2 10 2.5 10 time (seconds) 7 7 3 10 3.5 10 7 7 4 10 13 Bleachworld, AGU Fall Meeting 2011 The re-formation layer EUV,FUV NUV H2O Photolysis layer H2O H O3 H2O O2 H2O H2O2 H2 OH O(3P) H HO2 O3 O(1D) OH Reformation layer O2 14 Bleachworld, AGU Fall Meeting 2011 In presence of O2, H decays quickly in the reformation layer Isolated lower layer, p = 400 Pa, T = 300K, init [O ] = 10% 16 2 1 10 15 -3 Particle density ( cm ) 8 10 15 6 10 H H2 15 dH2O O2 H2O2 4 10 15 2 10 0 0 0.05 0.1 0.15 time (seconds) 0.2 0.25 15 Bleachworld, AGU Fall Meeting 2011 Now couple to photolysis products from upper layer:G star case 17 n =10 /cm 3 tot 3.5 10 10 10 7 10 9 7 10 8 7 7 10 10 6 10 5 10 4 3 H2 (molecules/cm ) 2 10 1.5 10 H2 7 1 10 7 5 10 6 H2O2 O3 H OH HO2 H, O3, H2O2 7 3 10 2.5 10 Lower Layer with G-star photolysis source of O(3P) and 2H 1000 100 0 0 5 10 4 5 5 1 10 1.5 10 time (seconds) 2 10 5 5 2.5 10 16 Bleachworld, AGU Fall Meeting 2011 M star: Young + Habitable Orbit or Old+ 1214b Orbit 17 n =10 /cm 3 tot 1.5 10 13 Lower Layer with M-star Ly-α photolysis source of O(3P) and 2H12 10 3 1 10 5 10 10 11 10 10 10 9 10 8 13 12 H2O2 O3 H 0 0 5000 4 OH HO2 4 1 10 1.5 10 time (seconds) 2 10 4 H, O3, H2O2 H2 (molecules/cm ) H2 4 2.5 10 17 Bleachworld, AGU Fall Meeting 2011 To Space Reformation layer is a sink, limits H escape EUV,FUV NUV H O3 H2O O2 H2O Photolysis layer O(3P) H Reformation layer 18 Bleachworld, AGU Fall Meeting 2011 Conclusions • Oxygen accumulated from losing 20% of initial ocean drives H and H2 to low concentrations, and likely chokes off hydrogen escape and irreversible water loss. • Calculations at 400K aren’t much different • Significant H escape still possible if it escapes from photolysis layer faster than it gets transported to lower atm. Need to couple chemistry to atmospheric escape model. AGU next year ? • We have not yet determined minimum O2 needed to cut off H escape. • Actually, not much bleach on bleachworld! 19