Page 44 - Wind Energy Handbook
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18                                                      THE WIND RESOURCE


          approximation is not reliable for estimating, say, the probability of a large gust
          within a certain period.
            The turbulence intensity clearly depends on the roughness of the ground surface
          and the height above the surface. However, it also depends on topographical
          features such as hills or mountains, especially when they lie upwind, as well as
          more local features such as trees or buildings. It also depends on the thermal
          behaviour of the atmosphere: for example, if the air near to the ground warms up
          on a sunny day, it may become buoyant enough to rise up through the atmosphere,
          causing a pattern of convection cells which are experienced as large-scale turbulent
          eddies.
            Clearly as the height above ground increases, the effects of all these processes
          which are driven by interactions at the earth’s surface become weaker. Above a
          certain height, the air flow can be considered largely free of surface influences. Here
          it can be considered to be driven by large-scale synoptic pressure differences and
          the rotation of the earth. This air flow is known as the geostrophic wind. At lower
          altitudes, the effect of the earth’s surface can be felt. This part of the atmosphere is
          known as the boundary layer. The properties of the boundary layer are important
          in understanding the turbulence experienced by wind turbines.


          2.6.2 The boundary layer

          The principal effects governing the properties of the boundary layer are the strength
          of the geostrophic wind, the surface roughness, Coriolis effects due to the earth’s
          rotation, and thermal effects.
            The influence of thermal effects can be classified into three categories: stable,
          unstable and neutral stratification. Unstable stratification occurs when there is a lot
          of surface heating, causing warm air near the surface to rise. As it rises, it expands
          due to reduced pressure and therefore cools adiabatically. If the cooling is not
          sufficient to bring the air into thermal equilibrium with the surrounding air then it
          will continue to rise, giving rise to large convection cells. The result is a thick
          boundary layer with large-scale turbulent eddies. There is a lot of vertical mixing
          and transfer of momentum, resulting in a relatively small change of mean wind
          speed with height.
            It the adiabatic cooling effect causes the rising air to become colder than its
          surroundings, its vertical motion will be suppressed. This is known as stable
          stratification. It often occurs on cold nights when the ground surface is cold. In this
          situation, turbulence is dominated by friction with the ground, and wind shear (the
          increase of mean wind speed with height) can be large.
            In the neutral atmosphere, adiabatic cooling of the air as it rises is such that it
          remains in thermal equilibrium with its surroundings. This is often the case in
          strong winds, when turbulence caused by ground roughness causes sufficient
          mixing of the boundary layer. For wind energy applications, neutral stability is
          usually the most important situation to consider, particularly when considering the
          turbulent wind loads on a turbine, since these are largest in strong winds. Never-
          theless, unstable conditions can be important as they can result in sudden gusts
          from a low level, and stable conditions can give rise to significant asymmetric
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