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49<br />

Interpolating temperature fields using static and dynamic lapse rates<br />

Chris Lennard<br />

Climate Systems Analysis Group, University of Cape Town, Cape Town, South Africa. email: lennard@csag.uct.ac.za<br />

1. Introduction<br />

Gridded climate data are important in many climate<br />

applications such as the validation of simulated results<br />

and understanding land-atmosphere interactions. Point<br />

source data often forms the basis of the gridded product<br />

and involves the interpolation of these data to a specified<br />

grid size. The nature of point source, observational<br />

temperature data is usually spatially heterogeneous and<br />

often lacks temporal consistency thus many interpolation<br />

techniques have been developed to aid the spatial<br />

generalization of point source data into a gridded product<br />

(e.g. Cressman 1959, Willmott et al. 1985, Biau et al.<br />

1999). Here, we present a novel approach, which uses<br />

empirical and dynamical methods, in the preparation of<br />

station data for interpolation as well a a more traditional<br />

approach. The latter used a static lapse rate field to get<br />

station data to a common level for interpolation whereas<br />

the new approach a dynamic lapse rate field. Each<br />

method is presented as well as the results from both and<br />

the merits of each discussed. We examined 36 years of<br />

station data over the Cape Fynbos region and used the<br />

Cressman interpolation scheme.<br />

2. Data and Methods<br />

The two preparation methods used lapse rates to<br />

reduce/raise station temperature data to a common level<br />

at which the interpolation was performed. The traditional<br />

approach reduced the station data at a constant lapse rate<br />

of 0.6 degrees per 100 m to sea level where the<br />

interpolation was performed. However, this method is<br />

unlikely to capture local scale phenomena such as<br />

temperature inversions, berg winds and localized<br />

orographic effects. In an attempt to capture these<br />

phenomena, the new method used empirical and dynamic<br />

methods to establish lase rate fields. First, self organizing<br />

maps (SOMs) were used to produce 12 characteristic<br />

synoptic circulations over South Africa for the 36 year<br />

time period (Fig. 1).<br />

Then, for each of these states, a regional climate model<br />

was run at a resolution of 3 km to generate 12 high<br />

resolution archetypal lapse rate fields. Figure 2 shows the<br />

lapse rate field for Cape Town International Airport for<br />

each of the synoptic states over 29 sigma levels.<br />

Every day in the station record mapped to one of the 12<br />

characteristic circulations so every station was raised by<br />

the SOM-specified lapse rate to a common level at the<br />

top of the atmosphere. The interpolation was then<br />

performed at this level. The interpolated temperature<br />

fields were then returned to the surface along respective<br />

lapse rates. We present the technique and the interpolated<br />

results and assess the value of using a dynamic lapse rate<br />

field versus a static one.<br />

Fig.1. Sea level pressure maps of the 12<br />

characteristic synoptic states.<br />

Fig. 2. Lapse rate fields for the SOM circulations<br />

above Cape Town International Airport. Sigma<br />

levels are not evenly spaced with height, more<br />

levels are at lower altitudes to capture boundary<br />

dynamics here. Sigma level 15 is at approximately<br />

3000 m, level 21 at approximately 6000 m and level<br />

30 at about 15000 meters.

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