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IPCC <str<strong>on</strong>g>Workshop</str<strong>on</strong>g> <strong>on</strong> <strong>Climate</strong> <strong>Sensitivity</strong><br />

Paris, France, July 26–29, 2004<br />

Pre-C<strong>on</strong>ference Volume<br />

A Comparis<strong>on</strong> <strong>of</strong> <strong>Climate</strong> <strong>Sensitivity</strong> Am<strong>on</strong>g the Japanese Models<br />

Akio Kitoh 1 , Akira Noda 1 , Seiji Yukimoto 1 , Seita Emori 2 , Toru Nozawa 2 , Tomoo Ogura 2 , Masahide<br />

Kimoto 3 , Ayako Abe-Ouchi 3 , and Akimasa Sumi 3<br />

1 Meteorological Research Institute, Tsukuba, Japan<br />

2 Nati<strong>on</strong>al Institute for Envir<strong>on</strong>mental Studies, Tsukuba, Japan<br />

3 Center for <strong>Climate</strong> System Research, University <strong>of</strong> Tokyo, Tokyo, Japan<br />

1. Introducti<strong>on</strong><br />

Two Japanese models (MRI and CCSR/NIES models)<br />

showed the smallest and the largest climate sensitivity<br />

at the time <strong>of</strong> the IPCC TAR in 2001. Here we report<br />

recent changes in their models’ climate sensitivity.<br />

2. MRI model<br />

The MRI-CGCM2 (Yukimoto et al. 2001; Yukimoto and<br />

Noda 2002) has several versi<strong>on</strong>s depending <strong>on</strong> cloudradiati<strong>on</strong><br />

tuning. In its radiati<strong>on</strong> scheme, CO , H O, 2 2<br />

O , CH and N O are treated as the greenhouse effect<br />

3 4 2<br />

gases directly, and the direct effect <strong>of</strong> sulfate aerosol is<br />

explicitly treated, but the indirect effect is not included.<br />

For the AR4 scenario experiments, atmospheric<br />

c<strong>on</strong>centrati<strong>on</strong> <strong>of</strong> sulfate aerosols has been calculated<br />

for all SRES emissi<strong>on</strong> scenarios <strong>of</strong> sulfur dioxide by<br />

a chemical transport model MASINGER developed at<br />

MRI (Tanaka et al. 2003). The global mean surface air<br />

temperature rises about 2.4K, 2.7K and 2.0K at the end<br />

<strong>of</strong> the 21st century compared to the 1961-1990 value in<br />

A1B, A2 and B2 scenarios, respectively (Uchiyama et<br />

al. 2004).<br />

IPCC <str<strong>on</strong>g>Workshop</str<strong>on</strong>g> <strong>on</strong> <strong>Climate</strong> <strong>Sensitivity</strong> – 51<br />

The global and annual mean surface air temperature<br />

change at 2xCO 2 <strong>of</strong> the MRI-CGCM2.0 in the IPCC<br />

TAR was very small, that is, 1.1K, with effective<br />

climate sensitivity <strong>of</strong> 1.4K. In this simulati<strong>on</strong>, the<br />

energy budget was not balanced between the top and<br />

the bottom <strong>of</strong> atmosphere, and the global mean and<br />

meridi<strong>on</strong>al distributi<strong>on</strong> <strong>of</strong> radiative flux at the top <strong>of</strong><br />

atmosphere had a large difference from the observati<strong>on</strong>.<br />

The revised MRI-CGCM2.3 is improved in reproducing<br />

mean climate <strong>of</strong> global-mean and meridi<strong>on</strong>al<br />

distributi<strong>on</strong> <strong>of</strong> energy budget by mainly adjusting clouds<br />

representati<strong>on</strong>. With the improved versi<strong>on</strong> <strong>of</strong> the model,<br />

the effective climate sensitivity increased more than 1K.<br />

The decrease <strong>of</strong> negative feedback due to cloud forcing<br />

can explain most <strong>of</strong> the changes in climate sensitivity.<br />

The major difference <strong>of</strong> cloud feedback can be explained<br />

by the change in tropical low-level clouds for shortwave<br />

forcing and in tropical middle level clouds for l<strong>on</strong>gwave<br />

forcing. Associated with the tropical low-level clouds,<br />

the stratus and stratocumulus clouds over the eastern<br />

part <strong>of</strong> the oceans (especially over the eastern Pacific)<br />

have large impact <strong>on</strong> shortwave forcing. The change in<br />

the tropical middle level clouds is associated with the<br />

change in deep c<strong>on</strong>vective clouds.<br />

Figure 1. Z<strong>on</strong>ally averaged annual mean cloud amount change normalized by global-mean surface air temperature change for (left)<br />

MRI-CGCM2.0 and (right) MRI-CGCM2.3.

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