Difference between revisions of "Wind Energy - Physics"
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<math>E=\frac{1}{2}mv^2</math> | <math>E=\frac{1}{2}mv^2</math> | ||
− | of the air-mass ''m ''crossing the area ''A ''during a time interval <br> | + | of the air-mass ''m ''crossing the area ''A ''during a time interval <br> |
<math>\dot{m}=A \rho \frac{dx}{dt}=A\rho v</math>. | <math>\dot{m}=A \rho \frac{dx}{dt}=A\rho v</math>. | ||
− | Because power is energy per time unit, combining the two equations leads back to the primary mentioned basic relationship of wind energy utilisation | + | Because power is energy per time unit, combining the two equations leads back to the primary mentioned basic relationship of wind energy utilisation |
− | <math>P=\dot{E}=\frac{1}{2} | + | <math>P=\dot{E}=\frac{1}{2}\dot{m}v^2=\frac{1}{2}\rho A v^3</math> |
Revision as of 17:53, 16 May 2011
Wind Power
The power P of a wind-stream, crossing an area A with velocity v is given by
It varies proportional to air density , to the crossed area A and to the cube of wind velocity v.
The Power P is the kinetic energy
of the air-mass m crossing the area A during a time interval
.
Because power is energy per time unit, combining the two equations leads back to the primary mentioned basic relationship of wind energy utilisation