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242 B. Stoevesandt et al.<br />

Bin Value<br />

10 4<br />

10 3<br />

10 2<br />

10 1<br />

10 0<br />

Bins of Column 3<br />

−10 0<br />

Bin<br />

10<br />

Bin Value<br />

Fig. 44.1. PDF of <strong>Wind</strong>speed change within 2 s within a 22 h measurement at Tjare<br />

(by Böttcher, data from http://www.winddata.com)<br />

Fig. 44.2. Typical mesh on a fx79-w-151 profile (left) and nodal points generated<br />

(right)<br />

44.2 The Spectral/hp Method<br />

The spectral/hp element method combines the accuracy of classical spectral<br />

codes with the flexibility of finite element methods (FEM). Global spectral<br />

methods use one representation of a function u(x) by a series through the<br />

complete domain. This idea is advanced by the spectral/hp method by subdividing<br />

the domain into finite – unstructured – elements. This is done by<br />

another transformation on the spectral function. To fulfill the necessary requirements,<br />

the spectral functions of the separate elements have to be C 0<br />

continuous.<br />

The subdivision into a mesh in combination with the use of unstructured<br />

meshes allows an adaption of the problem to the curved geometry and a well<br />

tuned resolution to the flowfield.<br />

There are two ways to achieve convergence using the spectral/hp method.<br />

The h-type convergence refers to convergence due to a refinement of the mesh,

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