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International Polar Year 2007–2008 - WMO

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of the aerosol component in the atmosphere over the<br />

Atlantic from 60° N to the Antarctic coast (Kotlyakov<br />

et al., 2010). A variable, called a spectral aerosol<br />

optical thickness (AOT) of the atmosphere, is used<br />

to characterize attenuation of the solar radiation by<br />

the aerosol particles within the whole air column.<br />

Magnitudes of the aerosol attenuation of the solar<br />

radiation measured in the Antarctic were the lowest<br />

values on the Earth, and they did not exceed limits<br />

of their natural variability. This is again the evidence<br />

of the fact that still to the present time the Antarctic<br />

atmosphere is not polluted by any aerosol of the<br />

anthropogenic origin.<br />

ORACLE-O3 (no. 99)<br />

LOLITA-PSC and MATCH-PSC campaigns<br />

As part of the ORACLE-O3 (“Ozone layer and UV RAdiation<br />

in a changing CLimate Evaluated during IPY”)<br />

global project, LOLITA-PSC (“Lagrangian Observations<br />

with Lidar Investigations and Trajectories in Antarctica,<br />

of PSC”) is devoted to <strong>Polar</strong> Stratospheric Clouds<br />

(PSC) studies. Understanding the formation and evolution<br />

of PSC particles is an important issue to quantify<br />

the impact of climate changes on their frequency of<br />

formation and, further, on chlorine activation and subsequent<br />

ozone depletion. Statistical studies on PSC<br />

and temperature over the Dumont D’Urville in Antarctica<br />

have been updated (David et al., 2009) and a study<br />

based on the “Match” method, developed initially for<br />

ozonesondes, has been applied, for the first time, to<br />

lidar observations of PSC acquired during campaigns.<br />

These campaigns took place in Antarctica during winters<br />

2006, 2007 and 2008, involving the three PSC lidar<br />

deployed in Antarctica, at Dumont d’Urville (66.67°S,<br />

140.01°E), Davis (68.00°S, 78.50°E) and McMurdo<br />

(77.86°S, 166.48°E) and CALIPSO space-borne lidar observations.<br />

Observations were performed at each lidar<br />

station when the weather conditions permitted. Tendays<br />

forward trajectories calculations from any station<br />

are performed each time a PSC is detected at the station.<br />

We consider a match when a trajectory issued<br />

from a station passes less than 200 km of another lidar<br />

station during a PSC observation period and when potential<br />

vorticity variations remain less than 40% along<br />

the trajectory. From the ground-based lidars, the evolution<br />

of scattering ratio can be drawn along the trajectories,<br />

completed with the CALIPSO values selected<br />

with a maximum time difference of 2.5 minutes and a<br />

maximum time distance of 200 km from the trajectories.<br />

As expected, a clear correlation appears between<br />

high scattering ratio values and the coldest temperatures,<br />

close or below the ice formation temperature<br />

[see Fig. 2.1-5, pers. comm. Nadège Montoux, LATMOS<br />

(Laboratoire atmosphères, Milieux Observations Spatiales),<br />

DNRS, France].<br />

The impact of the model for trajectory and of the<br />

initialisation fields on the match determination was<br />

explored (Montoux et al., 2009 and publication in<br />

preparation). For cold temperatures, of interest for<br />

PSC formation, the pressure and altitude discrepancies<br />

are not significant. Time difference could occasionally<br />

impact, but do not seem to affect greatly,<br />

the lidar scattering ratios extracted. Yet, when close<br />

to PSC temperature thresholds, the temperature differences<br />

are a key issue and more realistic values for<br />

nitric acid and water vapour mixing ratios are needed<br />

to determine these thresholds (using, for instance,<br />

the Microwave Limb Sounder onboard the AURA satellite).<br />

The current step of the analysis is the modelling<br />

of PSC formation along the trajectories using the<br />

Danish Meteorological Institute microphysical box<br />

model (Larsen et al., 2000). The model includes microphysical<br />

Mie and T-Matrix modules, together with<br />

optical modules, and is able to simulate the size dis-<br />

Fig. 2.1-5. Evolution<br />

of the temperature<br />

(left) and of the lidar<br />

scattering ratio at<br />

532 nm (right) along<br />

different trajectories<br />

(color code) started<br />

from Davis station at<br />

0300 UTC 2 August<br />

2007 to 0300 UTC 12<br />

August 2007.<br />

(Courtesy: Nadège Montoux)<br />

s C I e n C e P r o g r a m 143

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