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97<br />
Stratospheric variability and its impact on surface climate<br />
Andreas Marc Fischer(1,2), Isla Simpson(3), Stefan Brönnimann(2), Eugene Rozanov(2,4), Martin<br />
Schraner(2)<br />
(1) Federal Office of Meteorology and Climatology, MeteoSwiss, Kraehbuehlstr. 58, 8044 Zurich, Switzerland<br />
(2) Institute for Atmospheric and Climate Science, ETH Zurich, 8092 Zurich, Switzerland. (andreas.fischer@env.ethz.ch)<br />
(3) Department of Physics, Imperial College, London, UK<br />
(2) PMOD/WRC, Dorfstrasse 33, 7260 Davos, Switzerland.<br />
1. Introduction<br />
The stratospheric layer plays a key role in communicating<br />
climate variability over vast regions of the Earth’s<br />
atmosphere. Some of its variability is attributable to natural<br />
drivers such as variations in El Niño Southern Oscillation<br />
(ENSO), solar irradiance, or volcanic eruptions and is<br />
manifest on different timescales from days to seasons and<br />
even longer timescales. Through downward wave<br />
propagation, variability in the stratosphere can impact on<br />
tropospheric climate variability modes and hence surface<br />
climate on different spatial scales. One of the most<br />
prominent stratospheric influence are sudden stratospheric<br />
warmings (SSWs) leaving an imprint on weather at the<br />
ground even a few weeks later (Baldwin and Dunkerton,<br />
2001).<br />
Figure 1 shows the observed surface air temperature (SAT)<br />
and sea level pressure (SLP) response with respect to five<br />
major tropical volcanic eruptions and to ENSO since 1880.<br />
The volcanic signal in the first boreal winter months after<br />
the eruption is characterized by a cooling over the oceans<br />
and a warming over the northern extra-tropical land masses.<br />
Several dynamical feedback mechanisms including the<br />
propagation of planetary waves have been proposed to<br />
explain the pathway of climate anomalies originating from<br />
the stratosphere (see e.g., Stenchikov et al., 2004).<br />
Over recent years much attention has been drawn to the<br />
climatic effect of El Niño on the northern extra-tropical<br />
stratosphere and its manifestation on surface. While the<br />
surface climate response over the North Pacific and North<br />
American region is well known, the signal over the North<br />
Atlantic European sector (negative North Atlantic<br />
Oscillation accompanied by cold (mild) temperatures over<br />
Northern (Southern) Europe) is subject to a large variability<br />
among individual El Niño events which complicates its<br />
interpretation. Ineson and Scaife (2009) provided evidence<br />
for a global teleconnection pathway from the Pacific region<br />
to Europe via the stratosphere. They showed that, in<br />
presence of SSWs, the stratosphere plays an active role in<br />
the manifestation of the European regional climate pattern.<br />
A better knowledge of the impact of stratospheric variability<br />
on regional surface climate is therefore highly relevant with<br />
respect to detection and attribution studies as well as<br />
improvements of seasonal prediction schemes.<br />
volcanic<br />
ENSO<br />
-1.8<br />
-0.6<br />
-0.6<br />
-0.2<br />
0.6<br />
0.2<br />
1.8<br />
0.6<br />
(°C)<br />
(°C/°C)<br />
Figure 1. Effect of tropical volcanic eruptions (top)<br />
and ENSO (bottom) on boreal winter (Jan-Mar) SAT<br />
and SLP since 1880. Temperature and SLP data<br />
were detrended. The top panel shows a composite of<br />
the first winters after five tropical eruptions<br />
(Krakatoa, Santa Maria, Mt. Agung, El Chichón,<br />
Pinatubo). The bottom panel shows regression<br />
coefficients using a NINO3.4 index (Sep-Feb<br />
average) after removing two winters after each<br />
major volcanic eruption<br />
2. Model Simulations<br />
To study stratosphere-troposphere exchange processes<br />
global chemistry-climate models (CCMs) have proven to<br />
be indispensable tools as they incorporate all relevant<br />
dynamical, radiative, and chemical processes in the<br />
atmosphere (Eyring et al., 2006).<br />
Here we present results of two different kinds of<br />
simulations with the CCM SOCOL (Schraner et al.,<br />
2008): (a) ensemble simulations (9 members) in transient<br />
mode across the 20 th century (Fischer et al., 2008a); (b)<br />
time-slice simulations (20 ensemble members) of an<br />
anomalously strong El Niño (1940-42) and a weak La<br />
Niña (1975-76) (Fischer et al., 2008b). SOCOL is a<br />
combination of the middle atmosphere version of<br />
ECHAM4 (MPI, Hamburg) and the chemistry-transport<br />
model MEZON (PMOD/WRC, Davos). The simulations