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130<br />

Regional climate change projections using a physics ensemble over the<br />

Iberian Peninsula<br />

P. Jimenez-Guerrero (1), S. Jerez (1), J.P. Montavez (1), J.J. Gomez-Navarro (1), J.A. García-Valero<br />

(2) and J.F. Gonzalez-Rouco (2)<br />

(1) Universidad de Murcia, Spain (sonia.jerez@gmail.com), (2) AEMET, Murcia, Spain, (3) Universidad Complutense de<br />

Madrid, Spain<br />

1. Introduction<br />

Some of the most widely used Regional Climate Models<br />

(RCMs) contain large numbers of parameterizations which<br />

are known, individually, to have a significant impact on<br />

simulated climate (Zhiwei et al., 2002). Up to date,<br />

considerable uncertainties exist in the the extent to which<br />

different choices of parameter-settings or schemes may<br />

influence present climate simulations and different<br />

projections for the future climate. The most thorough way to<br />

investigate this uncertainty is to run ensemble experiments<br />

in which relevant parameter combination is investigated.<br />

The use of ensemble techniques in regional climate<br />

modeling has been shown in several studies (such as the<br />

PRUDENCE -Christensen et al., 2007-, ENSEMBLES<br />

projects) as feasible for obtaining projections of climate<br />

change (Vidale et al., 2007) and to study the capacity of<br />

RCMs to reproduce the observed climatology (Lenderink et<br />

al., 2007).<br />

This work explores the sensitivity of different physical<br />

parameterizations (microphysics, cumulus and PBL<br />

schemes) within a regional climate version of the MM5<br />

model (Grell et al., 1994) when applied in a complex an<br />

heterogeneous area such as the Iberian Peninsula (IP).<br />

2. Experiments<br />

A multi-physics ensemble of eight climate change<br />

projections (2070-2099 vs. 1970-1999) have been performed<br />

with MM5 driven by ECHAM5 global climate model<br />

outputs, forced by the SRES A2 scenario for the future<br />

period. This ensemble is the result of the combination of two<br />

of the available options for cumulus (Grell and Kain-<br />

Fritsch), microphysics (Simple Ice and Mixed Phase) and<br />

PBL (Eta and MRF) parametrizations (Tab. 1). Common<br />

physics options are RRTM scheme for radiation and Noah<br />

Land-Surface Model. Documentation is available in the<br />

<strong>web</strong>site http://www.mmm.ucar.edu/mm5.<br />

Spatial configurations of the domains employed in the<br />

simulations consists of two two-way nested domains, arising<br />

a resolution of 30 km over the IP. Vertically, 24 sigma levels<br />

with the top at 100 mb are considered.<br />

3. Results<br />

The analysis focuses on multiyear seasonly mean values<br />

of two variables: 2-meter temperature and precipitation.<br />

3.1. Temperature<br />

The ensemble spread is caused by changes in the PBL<br />

scheme (being negligible the changes in other<br />

parameterizations). Overall, the MRF scheme for the PBL<br />

provokes the highest temperature increase (and also the<br />

highest absolute values), meanwhile the Eta scheme leads<br />

to the minimum variation and values. The average rise in<br />

the temperature is about 2 degrees for wintertime and<br />

more than 5 degrees during the summertime in the Iberian<br />

Peninsula (Fig. 1); however, it should be highlighted that<br />

the spread of these results is up to 50% of the estimated<br />

warming in some areas (Fig. 2).<br />

Figure 1: Mean JJA temperature increase projected,<br />

weighting all the ensemble members equally.<br />

Table 1: Experiments identifiers. The last two are still<br />

under development.<br />

Experiment Microphysics Cumulus PBL<br />

1 Simple Ice Grell Eta<br />

2 Simple Ice Grell MRF<br />

3 Simple Ice kain-Fritsch Eta<br />

4 Simple Ice kain-Fritsch MRF<br />

5 Mixed Phase Grell MRF<br />

6 Mixed Phase kain-Fritsch Eta<br />

7 Mixed Phase Grell Eta<br />

8 Mixed Phase kain-Fritsch MRF<br />

Figure 2: Ensemble spread in the projected JJA<br />

temperature increase in % with respect to the mean<br />

projected increase (shown in Fig. 1).

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