Low (web) Quality - BALTEX
Low (web) Quality - BALTEX
Low (web) Quality - BALTEX
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
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.