the isotopic composition of carbon dioxide in the middle atmosphere

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Mao-Chang Liang 1 , Geoffrey A. Blake 1 , Brenton R. Lewis 2 , and Yuk L. Yung 1 1 Division of Geological and Planetary Sciences, California Institute of Technology, Pa sadena, USA 2 Research School of Physical Sciences and Engineering, The Australian National Univers ity, Canberra, Australia The Isotopic Composition of Carbon Dioxide in the Middle The Isotopic Composition of Carbon Dioxide in the Middle Atmosphere Atmosphere References References Yung et al. JGR, 1997; Thiemens et al. Sci ence, 1995; Lämmerzahl et al. GRL, 2002; Liang et al. JGR, 2005 (accepted) Abstract Abstract The isotopic composition of long-lived trace gases provid es a window into atmospheric transport and chemistry. Car bon dioxide is a particularly powerful tracer, because it s abundance remains >100 ppmv in the mesosphere. For the first time, we successfully reproduce the isotopic compos ition of CO 2 in the middle atmosphere. The mass-independe nt fractionation of oxygen in CO 2 can be satisfactorily e xplained by the exchange reaction with O( 1 D). In the stra tosphere, the major source of O( 1 D) is O 3 photolysis. High er in the mesosphere, we discover that the photolysis of 16 O 17 O and 16 O 18 O by solar Lyman- radiation yields O( 1 D) 10- 100 times more enriched in 17 O and 18 O than that from ozone photodissociation. New laboratory and atmospheric measure ments are proposed to test our model and validate the use of CO 2 isotopic fractionation as a tracer of atmospheric chemical and dynamical processes. Coupled with climate mo dels, the ‘anomalous’ oxygen signature in CO 2 can be used in turn to study biogeochemical cycles, in particular to constrain the gross carbon fluxes between the atmosphere and terrestrial biosphere. MIF of CO MIF of CO 2 2 1. Yung et al. (1997) mechanism: 16 O( 1 D) + C 16 O 16 O C 16 O 16 O + 16 O 3k 17 O( 1 D) + C 16 O 16 O C 16 O 17 O + 16 O 2k (1 + 1 ) 16 O( 1 D) + C 16 O 17 O C 16 O 16 O + 17 O k (1 + 2 ) 18 O( 1 D) + C 16 O 16 O C 16 O 18 O + 16 O 2k (1 + 3 ) 16 O( 1 D) + C 16 O 18 O C 16 O 16 O + 18 O k (1 + 4 ) 2. Isotopic fractionation of oxygen in CO 2 : 17 O(CO 2 ) 1 - 2 + 17 O( 1 D) - 17 O(CO 2 ) t 18 O(CO 2 ) 3 - 4 + 18 O( 1 D) - 18 O(CO 2 ) t where tropospheric values of 17 O(CO 2 ) t and 18 O(CO 2 ) t are 9 and 17 ‰, respective ly, relative to atmospheric O 2 . 3. Values of 1 - 4 : If scaled by reduced mass: 1 - 2 i s of opposite sign and similar magnitude to that from the quenching reactions of O( 1 D) with O or N . So In In troduction troduction Of the many trace molecules that can be used to examine at mospheric transport processes and chemistry (e.g., CH 4 , N 2 O, SF 6 , and the CFCs), carbon dioxide is unique in the middle atmosphere, because of its high abundance (~370 ppmv in th e stratosphere, dropping to ~100 ppmv at the homopause). T he mass independent isotopic fractionation (MIF) of oxygen first discovered in ozone is thought to be partially trans ferred to carbon dioxide via the reaction O( 1 D) + CO 2 in th e middle atmosphere. Indeed, while the reactions of trace molecules with O( 1 D) usually lead to their destruction, the O( 1 D) + CO 2 reaction regenerates carbon dioxide. This ‘recy cled’ CO 2 is unique in its potential to trace the chemical (reactions involving O( 1 D) in either a direct or indirect w ay) and dynamical processes in the middle atmosphere. When transported to the troposphere, it will produce measurable effects in biogeochemical cycles involving CO 2 . Sources of O( Sources of O( 1 1 D) D) 1. Stratosphere: O 3 + h (230-310 nm) O 2 + O( 1 D) 2. Mesosphere: O 2 + Lyman- O( 3 P) + O( 1 D) Thiemens et al. 1995 Lämmerzahl et al. 2002 1. Model simulation: Calculated by the Caltech/JPL one-dimensi onal KINETICS model, which reproduces the the vertical profiles of the isotopic composition of O 3 in the stratos phere (Liang et al. 2005) 2. Slopes: a) ~1.6 in the stratosphere (dashed line) b) <1.6 in the upper stratosphere c) ~0.3 in the upper mesosphere (line AB) d) ~0.5 above homopause (dash-dotted lin e) 3. Magnitude of 18 O(CO ) in the mesosphere: Three-box model illustration: a) 17 O(CO 2 ) = x t 17 O(CO 2 ) t + x s 1 7 O(CO 2 ) s + x m 1 7 O(CO 2 ) m - 17 O(CO 2 ) t 18 O(CO 2 ) = x t 18 O(CO 2 ) t + x s 18 O(CO 2 ) s + x m 1 8 O(CO 2 ) m - 18 O(CO 2 ) t b) x m << x s < x t and x t + x s + x m = 1 c) different degree of air mi O 2 Lyman- x m = (0, 0.05%, 0.1%) x t = (0.80, 0.75, 0.70) Contact: see http://www.gps.caltech.edu

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The Isotopic Composition of Carbon Dioxide in the Middle Atmosphere. Mao-Chang Liang 1 , Geoffrey A. Blake 1 , Brenton R. Lewis 2 , and Yuk L. Yung 1 1 Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, USA - PowerPoint PPT Presentation

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Page 1: The Isotopic Composition of Carbon Dioxide in the Middle Atmosphere

Mao-Chang Liang1, Geoffrey A. Blake1, Brenton R. Lewis2, and Yuk L. Yung1

1Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, USA 2Research School of Physical Sciences and Engineering, The Australian National University, Canberra, Australia

The Isotopic Composition of Carbon Dioxide in the Middle AtmosphereThe Isotopic Composition of Carbon Dioxide in the Middle Atmosphere

ReferencesReferences Yung et al. JGR, 1997; Thiemens et al. Science, 1995; Lämmerzahl et al. GRL, 2002; Liang et al. JGR, 2005 (accepted)

AbstractAbstractThe isotopic composition of long-lived trace gases provides a window into atmospheric transport and chemistry. Carbon dioxide is a particularly powerful tracer, because its abundance remains >100 ppmv in the mesosphere. For the first time, we successfully reproduce the isotopic composition of CO2 in the middle atmosphere. The mass-independent fractionation of oxygen in CO2 can be satisfactorily explained by the exchange reaction with O(1D). In the stratosphere, the major source of O(1D) is O3 photolysis. Higher in the mesosphere, we discover that the photolysis of 16O17O and 16O18O by solar Lyman- radiation yields O(1D) 10-100 times more enriched in 17O and 18O than that from ozone photodissociation. New laboratory and atmospheric measurements are proposed to test our model and validate the use of CO2 isotopic fractionation as a tracer of atmospheric chemical and dynamical processes. Coupled with climate models, the ‘anomalous’ oxygen signature in CO2 can be used in turn to study biogeochemical cycles, in particular to constrain the gross carbon fluxes between the atmosphere and terrestrial biosphere. .

MIF of COMIF of CO22

1. Yung et al. (1997) mechanism: 16O(1D) + C16O16O C16O16O + 16O 3k

17O(1D) + C16O16O C16O17O + 16O 2k (1 + 1) 16O(1D) + C16O17O C16O16O + 17O k (1 + 2) 18O(1D) + C16O16O C16O18O + 16O 2k (1 + 3) 16O(1D) + C16O18O C16O16O + 18O k (1 + 4)2. Isotopic fractionation of oxygen in CO2: 17O(CO2) 1 - 2 + 17O(1D) - 17O(CO2)t

18O(CO2) 3 - 4 + 18O(1D) - 18O(CO2)t

where tropospheric values of 17O(CO2)t and 18O(CO2)t are 9 and 17 ‰, respectively, relative to atmospheric O2.3. Values of 1-4: If scaled by reduced mass: 1 - 2 is of opposite sign and similar magnitude to that from the quenching reactions of O(1D) with O2 or N2. So 17O(CO2) and 18O(CO2) are equivalent to the case of 1-2=0=3-4

IntroductioIntroductionnOf the many trace molecules that can be used to examine atmospheric transport processes and chemistry (e.g., CH4, N2O, SF6, and the CFCs), carbon dioxide is unique in the middle atmosphere, because of its high abundance (~370 ppmv in the stratosphere, dropping to ~100 ppmv at the homopause). The mass independent isotopic fractionation (MIF) of oxygen first discovered in ozone is thought to be partially transferred to carbon dioxide via the reaction O(1D) + CO2 in the middle atmosphere. Indeed, while the reactions of trace molecules with O(1D) usually lead to their destruction, the O(1D) + CO2 reaction regenerates carbon dioxide. This ‘recycled’ CO2 is unique in its potential to trace the chemical (reactions involving O(1D) in either a direct or indirect way) and dynamical processes in the middle atmosphere. When transported to the troposphere, it will produce measurable effects in biogeochemical cycles involving CO2.

Sources of O(Sources of O(11D)D)1. Stratosphere:

O3 + h (230-310 nm) O2 + O(1D)2. Mesosphere:

O2 + Lyman- O(3P) + O(1D)

Thiemens et al. 1995 Lämmerzahl et al. 2002

1. Model simulation: Calculated by the Caltech/JPL one-dimensional KINETICS model, which reproduces the the vertical profiles of the isotopic composition of O3 in the stratosphere (Liang et al. 2005)2. Slopes: a) ~1.6 in the stratosphere (dashed line) b) <1.6 in the upper stratosphere c) ~0.3 in the upper mesosphere (line AB) d) ~0.5 above homopause (dash-dotted line)3. Magnitude of 18O(CO2) in the mesosphere: Measurements made by Thiemens et al. (1995) at 30N is likely due to fresh downwelling air at this latitude.

Three-box model illustration: a) 17O(CO2) = xt17O(CO2)t + xs17O(CO2)s + xm17O(CO2)m - 17O(CO2)t

18O(CO2) = xt18O(CO2)t + xs18O(CO2)s + xm18O(CO2)m - 18O(CO2)t

b) xm << xs < xt and xt + xs + xm = 1

c) different degree of air mixing from troposphere, stratosphere, and mesosphere is shown above.

O2 Lyman-

xm = (0, 0.05%, 0.1%)

x t = (

0.80

, 0.7

5, 0

.70)

Contact: see http://www.gps.caltech.edu/~mcl