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&nbsp;''during a time interval <br>
+
of the air-mass ''m ''crossing the area ''A&nbsp;''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}*\dot{m}*v^2=\frac{1}{2}\rho A v^3</math>
+
<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 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