Geoscience Reference
In-Depth Information
1-2 % of the half-width of the hill or mountain chain. Above the inner layer is the
outer layer within which the inertial forces dominate. The fractional speed-up is at
maximum at the boundary between the inner and the outer layer. Modern wind
turbines with hub heights around 100 m and more are usually in the outer layer
(Fig. 4.11 ). Therefore, they are exposed to less vertical wind gradients than over
level terrain. Building even higher towers with larger hub heights thus gives only a
relatively low gain in power yields.
Section 4.2 is valid for gentle hills only. Steeper hills and mountains lead to
non-linear features such as flow separation and other features named in Sect. 4.1
which are not adequately covered by the equations given in Sect. 4.2 . Non-linear
flow features can no longer be derived from analytical relations but require the
operation of numerical flow models. Some non-linearity effects become already
visible in the examples for the flow over an escarpment in Sect. 4.3 . Therefore,
wind assessment in rougher terrain where linearity is no longer assured has to be
done by site-specific numerical model simulations. This Chapter was designed to
point to the main flow features which influence the vertical wind profile over hills
and gentle mountains.
References
Allnoch, N.: Windkraftnutzung im nordwestdeutschen Binnenland: Ein System zur Standortbe-
wertung für Windkraftanlagen. Geographische Kommission für Westfalen, Münster, ARD-
EY-Verlag, 160 pp. (1992).
Anderson P.S., Ladkin R.S., Renfrew I.A.: An Autonomous Doppler Sodar Wind Profiling
System. J. Atmos. Oceanic Technol. 22, 1309-1325 (2005).
Astley, R.J.: A Finite Element Frozen Vorticity Solution for Two-Dimensional Wind Flow over
Hills. 6 th Australasian Conf. on Hydraulics and FIuid Mechanics, Adelaide, Australia, 443-
446 (1977).
Atkinson B.W.: Meso-scale Atmospheric Circulations. Academic Press, London etc., 495 pp.
(1981).
Bowen, A.J., D. Lindley,: A Wind-Tunnel Investigation of the Wind Speed and Turbulence
Characteristics
Close
to
the
Ground
over
Various
Escarpment
Shapes.
Bound.-Layer
Meteorol. 12, 259-271 (1977).
Bowen, A.J.: Full Scale Measurements of the Atmospheric Turbulence over Two Escarpments.
In: J.E. Cermak (ed.), Wind Engineering: Proc. 5 th
Internat. Conf., Fort Collins, Pergamon,
161-172 (1979).
Bradley, E. F.: The Influence of Thermal Stability and Angle of Incidence on the Acceleration of
Wind up a Slope. J. Wind Eng. Indust. Aerodynam. 15, 231-242 (1983).
Caccia, J.-L., Guénard, V., Benech, B., Campistron, B., Drobinski, P.: Vertical velocity and
turbulence
aspects
during
Mistral
events
as
observed
by
UHF
wind
profilers.
Ann.
Geophysicae 22, 3927-3936 (2004).
Defant, F.: Zur Theorie der Hangwinde, nebst Bemerkungen zur Theorie der Berg- und Talwinde.
Arch. Meteorol. Geophys. Bioklimatol. A 1, 421-450 (1949).
Emeis, S., H.P. Frank, F. Fiedler: Modification of air flow over an escarpment—Results from the
Hjardemal experiment. Bound.-Lay. Meteorol. 74, 131-161. (1995).
Emeis, S.: Vertical variation of frequency distributions of wind speed in and above the surface
layer observed by sodar. Meteorol. Z. 10, 141-149 (2001).
Search WWH ::




Custom Search