stratospheric ozone distribution

41
STRATOSPHERIC OZONE DISTRIBUTION Marion Marchand CNRS-UPMC-IPSL

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STRATOSPHERIC OZONE DISTRIBUTION. Marion Marchand CNRS-UPMC-IPSL. SHAPE OF OZONE PROFILE. Altitude (km). UV. J O2 (s -1 ). Altitude (km). O 3 (molecules.cm -3 x 10 -12 ). Photolysis coefficient (s -1 ). O 2 (molecules.cm -3 x 10 -19 ). - PowerPoint PPT Presentation

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Page 1: STRATOSPHERIC OZONE DISTRIBUTION

STRATOSPHERIC OZONE DISTRIBUTION

Marion Marchand CNRS-UPMC-IPSL

Page 2: STRATOSPHERIC OZONE DISTRIBUTION

O2 + UV-c -> O + O

O + O2 + M -> O3 + M

d[O3]/dt = 2 JO2 [O2]0 2 4 6 8 10 12 14

0

10

20

30

40

Altitude (km)

O

3

(ppmv)

O

3

(molecules cm

-3

x 10

-12

)

Air (molecules cm

-3

x 5 x 10

-19

)

O2 (molecules.cm-3

x 10-19)

Alt

itu

de

(km

)

Photolysis coefficient (s-1)

O3 (molecules.cm-3 x 10-12)

JO2 (s-1)

Altitude (km)SHAPE OF OZONE PROFILE

UV

Page 3: STRATOSPHERIC OZONE DISTRIBUTION

VMR (Volume Mixing Ratio)=[O3]/[M] (-> better indicator of chemistry )

O3

[M] total air concentration (molec.cm-3x 10-16)

[O3] [M]

[O3] concentration

(molec.cm-3 x 10-12)

Page 4: STRATOSPHERIC OZONE DISTRIBUTION

Brewer (1949) quotes from Dobson et al. (1929): 'The only way in which we can reconcile the observed high ozone concentration in the Arctic in spring and the low concentration in the tropics, with the hypothesis that the ozone is formed by the action of the sunlight, would be to suppose a general slow poleward drift in the highest atmosphere with a slow descent of air near the poles. Such a current would carry the ozone formed in low latitudes to the poles and concentrate it there. If this were the case the ozone at the poles would be distributed through a moderate depth of atmosphere while that in low latitudes would all be high up.’ [SPARC]

O3 production from O2 photolysis (molec.cm-3)O3 column (Dobson units)

tropical minimum

tropical maximum

latitude

lati

tude

month

Alt

itu

de (

km)

Why?

Page 5: STRATOSPHERIC OZONE DISTRIBUTION
Page 6: STRATOSPHERIC OZONE DISTRIBUTION

(=O3 concentration)

Page 7: STRATOSPHERIC OZONE DISTRIBUTION

Brewer (1949) said `The observed distributions of water vapour can be explained by the existence of a circulation in which air enters the stratosphere at the equator, where it is dried by condensation, travels in the stratosphere to temperate and polar regions, and sinks into the troposphere.' [SPARC]

Troposphere is humid but stratosphere is very dry. Why?

very dry statosphere

humid troposphere

Temperature (°K)

tropopause

stratopause

Page 8: STRATOSPHERIC OZONE DISTRIBUTION

GLOBAL DISTRIBUTION OF CHEMICAL TRACERS

Page 9: STRATOSPHERIC OZONE DISTRIBUTION

hours

days

months

dO3/dt~f(dynamics)

dO3/dt~f(chemistry)

months

dO3/dt = f(chemistry + dynamics)

Page 10: STRATOSPHERIC OZONE DISTRIBUTION

RESIDENCE TIME OF AIR IN STRATOSPHERE

Page 11: STRATOSPHERIC OZONE DISTRIBUTION

CHEMISTRY OF OZONE:CONCEPTS

Page 12: STRATOSPHERIC OZONE DISTRIBUTION

OXYGEN-ONLY CHEMISTRY

° First chemistry scheme proposed by Chapman in 1930, also called the ‘Chapman cycle’.

° The reactions are

O2 + h → O + O jO2 < 242 nm

O + O2 + M → O3 + M kO+O2

O3 + h → O + O2 jO3 < 336 nm

O + O3 → O2 + O2 kO+O3

Page 13: STRATOSPHERIC OZONE DISTRIBUTION

O2 + h → O + O

O + O2 + M → O3 + M

O3 + h → O + O2

O + O3 → O2 + O2

d[O3]/dt = kO+O2.[O2].[O].[M] -JO3.[O3] -kO+O3.[O3].[O]

d[O]/dt = 2.JO2.[O2] +JO3.[O3] -kO+O2.[O2].[O].[M] -kO+O3.[O3].[O]

Page 14: STRATOSPHERIC OZONE DISTRIBUTION

° kO+O2 et JO3 interconvert

O3 and O very rapidly, so

introduce new species

Ox[=O + O3] known as “odd-oxygen”

d[Ox]/dt = d[O]/dt + d[O3]/dt

= 2.JO2.O2 - 2.kO+O3.O3.O

Production - Destruction

If Ox steady-state (i.e. d[Ox]/dt = 0),

JO2.[O2]= kO+O3.[O3].[O]

ODD OXYGEN CHEMICAL FAMILY

fast

fast

slowslow

Page 15: STRATOSPHERIC OZONE DISTRIBUTION

Mass balance for atomic oxygen O:

d[O]/dt = 2.JO2.[O2] +JO3.[O3] -kO+O2.[O2].[O].[M] -kO+O3.[O3].[O]

° if Ox steady-state (i.e. d[Ox]/dt = 0), JO2.[O2]= kO+O3.[O3].[O]

-> d[O]/dt = JO2.[O2] +JO3.[O3] -kO+O2.[O2].[O].[M]

° interconversion terms >> net chemical terms (chemical family approach): JO3.[O3] >> JO2.[O2]

-> d[O]/dt ~ JO3.[O3] -kO+O2.[O2].[O].[M]

° lifetime of O = [O]/loss = 1/(kO+O2.[O2].[M]) < 1 sec

-> O steady-state (i.e. d[O]/dt = 0),

[O]/[O3] = JO3 / (kO+O2.[O2].[M])

° as expected, interconversion terms determine partitioning within chemical family

Page 16: STRATOSPHERIC OZONE DISTRIBUTION

Volume mixing ratio

Altitude (km)

° Chapman’s model of [O]/[O3] validated against observations

° [O]/[O3] << 1 -> Ox[=O + O3] ~ O3 and d[Ox]/d= d[O3]/dt

O3

O

Page 17: STRATOSPHERIC OZONE DISTRIBUTION

° if Ox steady-state (i.e. d[Ox]/dt = 0),

JO2.[O2]= kO+O3.[O3].[O]

° if O steady-state (i.e. d[O]/dt = 0),

[O]/[O3] = JO3 / (kO+O2.[O2].[M])

° using [O]=f([O3]) expression in JO2.[O2]= kO+O3.[O3].[O],

[O3] = [O2] . (kO+O2.[M] / kO+O3)1/2 . (JO2 / JO3 )1/2

with [O2] =0.21 [M]

Page 18: STRATOSPHERIC OZONE DISTRIBUTION

Calculated [O3] from Chapman’s model is much too high compared to observations. Why?

d[O3]/dt = JO2.[O2] - kO+O3.[O3].[O]

calculated

observed

Page 19: STRATOSPHERIC OZONE DISTRIBUTION

OZONE DESTROYING CATALYTIC CYCLES

° Bates and Nicolet introduced in 1950 the idea of ozone being destroyed via the following catalytic cycle:

OH + O3 → HO2 + O2

HO2 + O → OH + O2

net: O + O3 → O2 + O2

° NO2 cycle in 1970 by Crutzen and also Johnston

NO + O3 → NO2 + O2

NO2 + O → NO + O2

net: O + O3 → O2 + O2

Page 20: STRATOSPHERIC OZONE DISTRIBUTION

° ClO cycle in 1974 by Stolarski and Cicerone.

Cl + O3 → ClO + O2

ClO + O → Cl + O2

net: O + O3 → O2 + O2

° A general form:

X + O3 → XO + O2 fast

XO + O → X + O2 slow

net: O + O3 → O2 + O2

with X, the catalyst, being radical H, OH, NO, Cl or Br

° slow reaction is the limiting step in the cycle,

d[O3]/dt ~ - 2.kXO+O.[XO].[O]

Page 21: STRATOSPHERIC OZONE DISTRIBUTION

d[O3]/dt ~ +2.JO2.[O2] -2.kO+O3.[O3]. [O] -2.kHO2+O3. [HO2]. [O3]

-2.kNO2+O. [NO2]. [O] -2.kHO2+O3. [ClO]. [O]

Catalyst: H, OH, NO, Cl, Br,..

Page 22: STRATOSPHERIC OZONE DISTRIBUTION

STRATOSPHERIC SOURCE GASES The key stratospheric source gases are long-lived in the troposphere, and hence, once emitted at the surface, they can reach the stratosphere

° Stratospheric hydrogen radicals (OH, HO2) originate mostly from H2O injected from the troposphere and from the in-situ oxidation of (natural and anthropogenic) CH4 by,

O(1D) + H2O → OH + OH

O(1D) + CH4 → OH + CH3 --> more oxidation, more OH

° Most of the stratospheric nitrogen oxide radicals (NO2, NO) originates from N2O oxidised in the stratosphere via the following reaction,

O(1D) + N2O → NO + NO

Page 23: STRATOSPHERIC OZONE DISTRIBUTION

STRATOSPHERIC SOURCE GASES ° Stratospheric chlorine radicals (Cl, ClO) originate mostly from CFCs that are photolysed by UV radiation following,

CFxCly + h → Cl + CFxCl(y-1) --> more oxidation, more Cl

Page 24: STRATOSPHERIC OZONE DISTRIBUTION

° Sources of stratospheric chlorine radicals (Cl, ClO)

natural

anthropogenic

Page 25: STRATOSPHERIC OZONE DISTRIBUTION

RESERVOIR SPECIES ° Up to now, we considered the different catalytic cycles independently. But radicals from one chemical family can interact with radicals from another family.

° Reactions between radicals lead to formation of species with longer lifetimes, much less reactive, called reservoirs, e.g.

ClO + HO2 → HOCl + O2

HO2 + NO2 + M → HO2NO2 + M

ClO + NO2 + M → ClONO2 + M

OH + NO2 + M → HNO3 + M

NO3 + NO2 + M → N2O5 + M

° Reservoir species can be dissociated back rather quickly to release ozone destroying radicals

Page 26: STRATOSPHERIC OZONE DISTRIBUTION

CHEMICAL MODEL O3 BUDGET : Production - Destruction

d[O3]/dt = 2 JO2 [O2] -2 k[XO][O] with X=O2, OH, NO, Cl

NOx (N2O)

HOx (CH4,H2O)

ClOx (CFCs)

production/destruction rate (molec.cm-3.s-1)

O/O3 cycle

O3=f(X, altitude)

Page 27: STRATOSPHERIC OZONE DISTRIBUTION

ozone abundance (mPa)

° complete destruction between 14 and 22 km

° - d[O3]/dt ~ 2 %/day

Page 28: STRATOSPHERIC OZONE DISTRIBUTION

PSC clouds formed at T < ~193 K by co-condensation of HNO3 and H2O

Page 29: STRATOSPHERIC OZONE DISTRIBUTION

Heterogeneous chemistry: ° chlorine activation (reservoirs species -> into chlorine radicals) ° O3 destruction

-> speed up reactions that are are very slow or non-existent in the gas-phase

Ice or HNO3/H2O PSCs

Page 30: STRATOSPHERIC OZONE DISTRIBUTION

CATALYTIC CYCLES OF POLAR OZONE DESTRUCTION

° BUT observed loss rates (- d[O3]/dt) ~ 2 %/day -> [O] is much too low (not enough sunlight during early spring) for ClO+O cycle to account for observed loss rates.

° Cl2O2 cycle in 1987 by Molina and Molina.

ClO + ClO + M Cl2O2 + M equilibrium

Cl2O2 + h → Cl + ClOO

ClOO + M → Cl + O2 + M

2 x ( Cl + O3 → ClO + O2 )

-> little sunlight is required (fast JCl2O2) and more efficient at low temperatures because it slows down thermal decomposition of Cl2O2 (Cl2O2 → ClO + ClO)

Page 31: STRATOSPHERIC OZONE DISTRIBUTION

° ClO-BrO cycle

ClO + BrO → Cl + Br + O2 slow

Cl + O3 → ClO + O2 fast

Br + O3 → BrO + O2 fast

net: O + O3 → O2 + O2

-> little sunlight is required because the cycle does not involve atomic oxygen O

° Polar ozone loss rate:d[O3]/dt ~ -2.JCl2O2. [Cl2O2] -2.kClO+BrO.ClO.BrO

Page 32: STRATOSPHERIC OZONE DISTRIBUTION

high chlorine loading andvery cold/ isolated polar vortex

Page 33: STRATOSPHERIC OZONE DISTRIBUTION

INTERACTIONS OZONE-CLIMAT

Page 34: STRATOSPHERIC OZONE DISTRIBUTION

Effet de Serre

=

Bilan au niveau de la Terre + effet de Serre:

Bilan au niveau de la couche (loi Kirchhoff):

a = 2

Bilan au niveau de la Terre sans effet de Serre (loi de stefan):

= Ts = 255 K seulement !

+ = _2

Page 35: STRATOSPHERIC OZONE DISTRIBUTION
Page 36: STRATOSPHERIC OZONE DISTRIBUTION

Stratospheric cooling / heating rate (K/day)

Heating: O3 + UV → O + O2

O + O2 + M → O3 + M (Q) -> dT/dz > 0

Cooling: mainly CO2 +/- IR H2O and O3 significant

Temperature

tropopause

stratopause

Page 37: STRATOSPHERIC OZONE DISTRIBUTION

O3 and T strongly coupled: d(O3)/dt > 0 -> d(T)/dt > 0 -> attenue le d(O3)/dt > 0 d(T)/dt > 0 -> d(O3)/dt < 0 -> attenue le d(T)/dt > 0

~ 45 kmRelation-2 O3-T:

O + O3 → O2 + O2

k = 2.e-11 *exp( -2350 / T)

Quand T diminue => ralentissement destruction O3

=>d(T)/dt > 0 -> d(O3)/dt < 0

Relation-1 O3 - T :O3 + UV → O + O2

O + O2 + M → O3 + M (Q) => d(O3)/dt > 0 -> d(T)/dt > 0

Page 38: STRATOSPHERIC OZONE DISTRIBUTION

total

Ozone changes

Greenhouse gas changes

Page 39: STRATOSPHERIC OZONE DISTRIBUTION

Diminution O3-strato modifie l’équilibre radiatif à la tropopause effet sur la T au sol :-Augmentation de la pénétration des UV dans le système surface-troposphère(Forçage positif)-Sans ajustement de T: réduction des émissions IR de corp noir vers la surface(Forçage négatif)-Avec ajustement de T: diminution de l’absorption du rayonnement UV par l’O3 => refroidissement de la stratosphère => réduction de l’émission des corps noirs vers le sol (Forçage négatif)

-0.15 Wm-2

Page 40: STRATOSPHERIC OZONE DISTRIBUTION

COMPLEXITY OF INTERACTIONS

CTM + GCM = CCM (Chemistry-Climate Model) -> predict the future evolution of ozone layer

DYNAMICS(T, winds)

RADIATION

CHEMISTRY

CO2

O3, CH4

CCM

Page 41: STRATOSPHERIC OZONE DISTRIBUTION

Future O3 = f(CFCs, greenhouse gases)

Montreal process: chlorine loading -> ozone layer

Kyoto process greenhouse gases -> climate