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Basics of W ind Energy and Power     21


              of the 59.3% of total wind energy that is extracted from wind is trans-
              ferred to the turbine, but some of it is used to overcome viscous drag
              on blades and create vortices in the wake. Within the turbine, most of
              the energy is converted into useful electrical energy, while some of it
              is lost in gearbox, bearings, generator, power converter, transmission
              and others. Most practical rotors with three blades reach an overall
              efficiency of about 50%. From a theoretical standpoint, Okulov et al. 2
              show that a rotor reaches the Betz limit with a large number blades
              operating at a very high tip speed ratio (the ratio of tip speed to wind
              speed).
                 Often, inventors claim to have created a rotor that achieves an
              efficiency that is greater than 59.3%; such claims are suspect and must
              be analyzed. There are turbine configurations that may violate the Betz
                                 3
              limit. A shrouded rotor that augments axial velocity is an example.
              No large turbine has been created, to the best of author’s knowledge,
              with a shroud; however, there are a few small horizontal and vertical
              axis turbines with shroud. The following are illustrative examples of
              the Betz limit.

              Example 1
              As an example, consider 1-MW rated turbine with rotor diameter =
              70 m and power curve, as shown in Fig. 2-8. Power curve is a key
              performance indicator of a turbine that is provided by the turbine
              manufacturer. It describes the relationship between power produced
              and wind speed. A Betz limit curve is also plotted in Fig. 2-9. It is
              alwaysabovethepowercurve,whichimpliesthattheturbineiswithin
              the Betz limit at all wind speeds.
                                      16 ρA r v 3 0  16 ρA r v 3 0
                             P Betz (v 0 ) =  =                   (2-33)
                                      27  2     27  2
              To show calculations at one point in the curve, ν 0 = 12 m/s with air
                                3
              density of 1.225 kg/m :
                                           2  3
                                        70
                               16 1.225π  2  12
                      P Betz (v 0 ) =          = 2.4 MW           (2-34)
                               27      2
              Note the power curve indicates a power production capacity of
              slightly less than 1 MW, which is less than P Betz .
              Example 2
              As a second example, consider a turbine with rotor diameter = 2 m
              and power rating of 2 KW at 12 m/s.

                                                2  3
                                             2
                                   3
                               ρA r v 0  1.22π  2  12
                         P ideal =   =             = 3.3 kW       (2-35)
                                 2          2
                         P Betz = 0.59 P ideal = 1.953 kW         (2-36)
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