http://www.4shared.com/office/60og6CU1/FULLTEXT01.html
http://www.4shared.com/office/60og6CU1/FULLTEXT01.html
http://www.4shared.com/office/60og6CU1/FULLTEXT01.html
http://www.4shared.com/office/60og6CU1/FULLTEXT01.html
http://www.4shared.com/office/60og6CU1/FULLTEXT01.html
During the last decades the
exploitation of energy from the wind has become one of the most
promising renewable energy technologies. The main strive in today’s development
of wind turbines is to increase the efficiency of the turbine and to
build bigger rotors that are able to extract more power out of the wind.
When it comes to the planning and
designing of a wind park, also the aerodynamic interactions between the
single turbines must be taken into account. The flow in the wake of the
first row turbines is characterized by a significant deficit in wind
velocity and by increased levels of turbulence. Consequently, the
downstream turbines in a wind farm cannot extract as much power from the
wind anymore. Furthermore, the additional turbulence in the wake could
be a reason for increased material fatigue through flow-induced
vibrations at the downstream rotor.
The main focus of this experimental
study is to investigate the local velocity deficit and the turbulence
intensities in the wake behind an array of two model wind turbines. For
two different turbine separation distances, the wake is scanned at three
different downstream positions. The experiments are performed at the
wind tunnel (1.9m x 2.7m cross section) at NTNU Trondheim using two
model wind turbines with a rotor diameter of 0.9m. A hot wire probe is
used to scan the wake behind the model turbines in defined positions.
Moving axially downstream the velocity
deficit in the wake gradually recovers and the turbulence intensity
levels slowly decrease. Furthermore, a gentle expansion of the wake can
be observed. The wake profiles measured in close distances behind the
rotor are characterized by evident asymmetries. Further downstream in
the wake turbulent diffusion mechanisms cause a more uniform and more
symmetrical flow field. Moreover, the turbulence intensity behind the
second wind turbine is found to be significantly higher than behind one
unobstructed turbine.
Also, considerably higher velocity
deficits are found in the near wake behind the second turbine compared
to the wake behind one unobstructed turbine. However, the velocity
profile at five rotor diameters downstream in the wake behind the second
turbine is already very similar to the velocity distribution behind the
first turbine. Furthermore, the velocity field and turbulence intensity
distribution in the wake behind the second turbine is more symmetrical
and more uniform than behind the first turbine.