Environmental Engineering Reference
In-Depth Information
The integrations in Equations (2-12) are normally performed numerically, applying
Simpson's Rule. The magnitude of the
rotor shaft power
can then be calculated from shaft
torque and speed, as follows:
P
R
=
Q
W
(2-13)
where
P
R
= rotor shaft power (N-m/s)
Rotor Power Coeficient
The conventional measure of the aerodynamic performance of a wind turbine rotor (re-
gardless of coniguration) is its
rotor power coeficient
, which is the ratio of the
rotor power
density
(mechanical power at the turbine shaft per unit of swept area) to the
wind power
density
, or
C
P
,
R
=
P
R
/
A
p
W
P
R
0.5r
U
3
A
(2-14)
=
where
C
P,R
= rotor power coeficient
P
R
= mechanical power at the turbine rotor shaft (W)
Axial Induction (Retardation) of the Wind
The axial induction factor,
a
, in Equation (2-11b) is the fractional decrease in wind speed
between the upwind free-stream and the plane of the rotor, as power is extracted at the rotor
from the wind. According to the
axial momentum theory
[Rankine 1865, W. Froude 1878, R.
Froude 1889], the wind speed downstream of the rotor is reduced further by the same amount
as upstream. On this basis, the total retardation of the free-stream wind, from upstream of the
rotor to the
far wake
downstream, is 2
a
. This would indicate that the maximum value of
a
for a wind turbine is 0.5, when the wind speed in the far wake
is zero. However, momentum
theory is considered to be invalid for induction factors larger than about 0.4 [Wilson 1994].
By applying the Rankine-Froude theory to the calculation of rotor power, it has been
shown that
C
P
= 4
a
(1-
a
)
2
,
a
£ 0.4
(2-15a)
from which
(2-15b)
C
P
,
max
= 0.593
at
a
= 1/3
Therefore, an axial induction factor of approximately 1/3 is a common goal for a wind
turbine operating at its
design wind speed
(see Figure 2-12).
As discussed in detail by Eggleston and Stoddard [1987], the axial induction factor can
be determined from the rotor thrust force, normalized as follows:
T
0.5
r
U
3
A
C
T
=
(2-16)
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