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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 4—Wind Turbine Power 4–46<br />

Figure 27: Shaft torque output of Sandia 17-m Darrieus in variable-speed operation.<br />

we can argue that the maximum shaft torque varies as the square of the rotational speed. In<br />

Fig. 27, for example, the peak torque in a 12 m/s wind is 10,600 N·m/rad at 60 r/min. The<br />

peak torque in a 6 m/s wind is 2650 N·m/rad at 30 r/min. The peak torque has changed by<br />

a factor of four while the rotational speed has changed by a factor of two.<br />

The turbine torque T m must be opposed by an equal and opposite load torque T L for<br />

the turbine to operate at a steady rotational speed. If T m is greater than T L ,theturbine<br />

will accelerate, while if T m is less than T L the turbine will decelerate. The mathematical<br />

relationship describing this is<br />

T m = T L + I dω m<br />

N · m/rad (51)<br />

dt<br />

where I is the moment of inertia of the turbine, transmission, and generator, all referred to<br />

the turbine shaft.<br />

The relationship between shaft torque and an optimum load torque for the Sandia 17-m<br />

Darrieus turbine is illustrated in Fig. 28. We have assumed a load torque with the optimum<br />

variation<br />

Wind Energy Systems by Dr. Gary L. Johnson November 21, 2001

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