Sulfur Isotope Ratios and Constraints on Climate Alexander A. Pavlov LPL, University of Arizona, Tucson Main Message • Anomalous fractionation (MIF) in sulfur isotopes can be used as a constraint on the total amount of atmospheric sulfur and on the overall atmospheric oxidation state. Sulfur Isotopes 1) Sulfur has 4 stable isotopes: 32S (95.02%), 33S(0.75%), 34S (4.21%), and 36S (0.02%) 2) δ = ( Rsample/Rstandard – 1) x 1000 R = 34S/32S for δ34S 3) Typical terrestrial values for δ34S are within ± 50 per mil MIF in Sulfur • Standard mass fractionation line (MFL): δ33S ≅ 0.515 x δ34S; δ36S ≅ 1.91 x δ34S • In Archean sediments and Martian meteorites, the isotopes fall off this line (Farquhar et al., 2000) • Δ33S = δ33S - 0.515 x δ34S Δ33S = δ33S – 1000 x [(1 + δ34S/1000)0.515 – 1 ] Sulfur MIF is measured Δ33S – deviation from MFL. Δ33S Farquhar et al., JGR 2001 Analogy with Oxygen MIF • Sulfur is not the only element which show MIF (anomalous fractionation) • 16O, 17O, 18O • Δ17O = δ17O - 0.52 x δ18O • Used to constrain stratosphere/troposphere exchange • Oxygen MIF is produced in the stratosphere and oxygen bearing species which do not go through the stratosphere would not acquire MIF The only(!) experiment so far…. Farquhar’s experiment Sulfate Δ33S < 0 UV SO2 mixture SO2 remaining Δ33S < 0 Δ33S = 0 Δ33S > 0 Elemental S Farquhar et al., JGR 2001 Why is it exciting for the planetary atmospheres? Mass-dependent fractionation after deposition (biology, aqueous alteration etc.) can change (δ33S, δ34S) but it cannot introduce new produce Δ33S . The only way to lose Δ33S is to mix the atmospheric sulfur with unfractionated sulfur after deposition. Δ33S through time. Note that Δ33S essentially disappears when oxygen became abundant in the Earth’s atmosphere. Compiled from Farquhar et al. (2000), (2002), Mozjsis et al. (2003), Ono et al. (2003), Hu et al. (2003), Bekker et al. (2004), Johnston et al. (2005a), Whitehouse et al. (2005), Papineau et al. (2005). All unpublished data was collected at UMd. 0.4 Marine aerosols o 19 H 91 ud ba son ck gr 12 ou 59 nd er 12 u 59 pti on e 12 r u #1 59 pti ba on ck # 2 gr ou nd er r P in A C m m fa e r ll w in te r sp ri ng su ! 33S (‰) 0.8 0 -0.4 -0.8 Savarino et al., GRL 2003 2" at u bo Summary of the sulfur MIF data • So far sulfur MIF signature was observed in: a) Martian meteorites (small but non-zero Δ 33S ) b) Archean rocks (large Δ33S ) c) Antarctic ice cores during deposition of the volcanic sulfates from the large volcanic eruptions (Δ33S depends on the magnitude of eruption) Physical mechanism for the sulfur MIF • We know that MIF should be produced in the gas phase by some photochemical reaction. But which one? • Currently three reactions were suggested as the primary sulfur MIF source: A)SO2 + hν SO + O (Farquhar et al.) B)SO2* + SO2 SO + SO3 (Savarino et al.) C)SO3 + hν SO2 + O (Pavlov et al.) How does MIF signature place a constraint on the atmospheric oxidation state? Input Oxidizing Atmosphere OH, O2, O 33 SO + hν 2 SO : Δ S < 0 Volcanic SO2 flux 2 Δ33S = 0 SO: Δ33S > 0 A lot! Input Reducing Atmosphere Volcanic SO2 flux SO2 + hν SO2: Δ33S < 0 OH, O2, O Δ33S = 0 SO: Δ33S > 0 Not a lot! Output H2SO4 Δ33S = 0 Output H2SO4, SO2 Δ33S < 0 H2S, HS, S8 Δ33S > 0 Low-oxygen Sulfur Cycle S8 and Sulfate fluxes respond dramatically to the increase in oxygen/oxidants. 2 /sec) 1010 109 S8 SO2 108 H2SO4 107 Sulfur Deposition Fluxe 10-10 10-9 10-8 10-7 Oxygen abundance f(O2) 10-6 • What about sulfur MIF in the present Earth’s atmosphere? • How does sulfur MIF signal place a constraint on the total abundance of the atmospheric sulfur? Δ33S > 0 hν SO2 Δ33S < 0 SO “Initial” fractionation during SO2 photolysis. Fast conversion of SO back to SO2 cancels MIF in the aerosol Slow Fast Aerosol Δ33S = 0 Δ33S > 0 SO3 hν SO2 Δ33S < 0 Fast Slow Aerosol Δ33S ≠ 0 “Initial” fractionation during SO3 photolysis. Slow conversion of SO2 to SO3 allows MIF to be incorporated into the aerosol Pinatubo eruption 1) 30 Mt of SO2 into the stratosphere between 10°S and 10°N, at 16-30 km altitude in June. 2) MIF happens during SO3 photolysis only SO3 (Δ-) + hν → SO2 (Δ+) + O 3) Volcanic sulfur have Δ33S = 0 Main Message 1) In the weakly reducing atmospheres Δ33S is always present and depends on the total sulfur input into the atmosphere 2) In the oxidizing atmospheres MIF is much smaller but can be detectable if there is significant amount of sulfate aerosols at the high altitudes. Implications for Venus • There are several reservoirs of oxidized and reduced sulfur on Venus. Therefore, it is hard to avoid sulfur MIF in Venus aerosols. • The magnitude of sulfur MIF would place a constraint on the mixing between lower and upper atmosphere of Venus and the sulfur cycle in general.
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