- #1
Grinch
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Dear all,
I'm just doing some thinking around the maximum theoretical power that can be extracted from wind by using a wind plant.
Derivation of the power inside a block of wind is not difficult then I'll simply report some consideration regarding this subject (look at the attached paper for details).
At first we've to assume some air density, speed, and area of the air parcel that is going to the plant, put all together will give (look at the Pwr relation on the page 2 of attached PDF):
Pwr = 1/2 * (rho * V^3 * A)
As defined A stand for the area of the air parcel.
Now I've a question about the role of the blade area into the output power that I can generate from the plant. Looking at the formulae seems that the blade area have no influence because the area A are simply calculated as pi*R^2 where R is the blade length.
Of course there is some consideration about the blade speed, if too slow only a little part of the air will be collected, if too high turbolence may also decrease the output power and then there is a compromise from the air speed and the blade speed but the concept is there is a way to show a dipendence from the blade area and the total air parcel cross section area or really this is not important and the final resul will be independent from the geometrical blade area?
In other word, if I suppose a blade area equal to S and n°3 blade my total useful area will be equal to 3S then, if we've a unity ideal conversion ratio the energy that I can collect from the air parcel should be proportional to 3S then also the final power sould be proportional to the 3S area... or not... (take also care that my question is different than the Bets law http://en.wikipedia.org/wiki/Betz'_law, is just a matter to know if really the blade area isn't important or have some role into the final energy and then power computation).
Thanks in advance
Grinch
I'm just doing some thinking around the maximum theoretical power that can be extracted from wind by using a wind plant.
Derivation of the power inside a block of wind is not difficult then I'll simply report some consideration regarding this subject (look at the attached paper for details).
At first we've to assume some air density, speed, and area of the air parcel that is going to the plant, put all together will give (look at the Pwr relation on the page 2 of attached PDF):
Pwr = 1/2 * (rho * V^3 * A)
As defined A stand for the area of the air parcel.
Now I've a question about the role of the blade area into the output power that I can generate from the plant. Looking at the formulae seems that the blade area have no influence because the area A are simply calculated as pi*R^2 where R is the blade length.
Of course there is some consideration about the blade speed, if too slow only a little part of the air will be collected, if too high turbolence may also decrease the output power and then there is a compromise from the air speed and the blade speed but the concept is there is a way to show a dipendence from the blade area and the total air parcel cross section area or really this is not important and the final resul will be independent from the geometrical blade area?
In other word, if I suppose a blade area equal to S and n°3 blade my total useful area will be equal to 3S then, if we've a unity ideal conversion ratio the energy that I can collect from the air parcel should be proportional to 3S then also the final power sould be proportional to the 3S area... or not... (take also care that my question is different than the Bets law http://en.wikipedia.org/wiki/Betz'_law, is just a matter to know if really the blade area isn't important or have some role into the final energy and then power computation).
Thanks in advance
Grinch
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