Flow (liquid or gas) across a rotating surface's face

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Discussion Overview

The discussion revolves around the impact of the angle at which wind interacts with the blades of a wind turbine on the maximum power output equation. Participants explore how to adjust the area parameter in the power equation when the wind is not perpendicular to the turbine blades, particularly focusing on the implications of using cosine and sine functions in this context.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions how to modify the maximum power equation when wind approaches at an angle, specifically mentioning the equation Pmax= 8/27Sρu13 and suggesting S=Scosθ.
  • Another participant points out that using cos(150°) results in a negative value, which raises concerns about the physical interpretation of negative power output.
  • A different participant proposes an alternative area calculation, S=πR²=π(Rcosθ)², and seeks clarification on whether this approach is correct.
  • Some participants emphasize the importance of visualizing the problem by drawing the disk and flow vector to understand the orientation of the surface normal vector.
  • There is a suggestion that flipping the direction of the surface normal could change the angle to 30°, resulting in a positive current, indicating a need to consider the orientation of vectors in the calculations.
  • One participant stresses that understanding the physical meaning behind the formulas is crucial, rather than just applying them mechanically.

Areas of Agreement / Disagreement

Participants express differing views on the correct approach to calculating the effective area when wind is at an angle. There is no consensus on whether to use cosθ or an alternative method, and the discussion remains unresolved regarding the implications of negative values in this context.

Contextual Notes

Participants highlight the need for clarity on the definitions of surface normal vectors and the implications of angle orientation, but do not resolve the mathematical steps or assumptions involved in the calculations.

QuarkDecay
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<< Mentor Note -- Two threads on the same question merged into one thread >>

How does the maximum Power equation change if there's an angle to the way the wind falls into the wind turbine's blades?

Example, when it falls vertically to the blades, it's
Pmax= 8/27Sρu13

But if there's for example an angle of θ=150ο then what? My book says you need to do S=Scosθ, but cos(150o)= -0.89. Which is negative and doesn't make sense for the Power to be negative?

I thought maybe I should do S=πR2=π(Rcosθ)2 instead. Is that wrong or what am I supposed to do?
 
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QuarkDecay said:
Example, when it falls vertically to the blades, it's
Pmax= 8/27Sρu13

But if there's for example an angle of θ=150ο then what? My book says you need to do S=Scosθ, but cos(150o)= -0.89. Which is negative and doesn't make sense for the Power to be negative?
150 degrees would be behind the turbine.
 
Suppose we have a surface that scans a cycle, with an S=πR2, when its axis faces the gas' flow vertically.
Now if the gas' flow gets an angle of θ=150ο, what will the S be? My book says it's Scosθ, but with an angle of 150o it gives me a negative number, which doesn't make a lot of sense considering the nature of the problem (needs to calculate the power output of a wind turbine)
Should I do S=πR2= π(Rcosθ)2 instead?

Also why should it be cosθ and not sinθ? Can someone explain the math behind this?
 
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Just draw the disk and the flow vector with the definition of the surface normal vector such to give an angle of ##150^{\circ}## and see for yourself that the book is right with it's definition. The flow through the surface element ##\mathrm{d}^2 \vec{f}## is given given by ##\vec{j} \cdot \mathrm{d}^2 \vec{f}## it gives the amount of fluid flowing per unit time through the little surface element. This gets negative in your case, and it has a very simple physical meaning, but you have to consider the (arbitrary) choice between the two possibilities to orient the surface-normal vectors along the surface!

Hint: This should also become clear, if you simply flip the direction of the surface normal then the angle is ##30^{\circ}## and your current gets positive!
 
vanhees71 said:
Just draw the disk and the flow vector with the definition of the surface normal vector such to give an angle of ##150^{\circ}## and see for yourself that the book is right with it's definition. The flow through the surface element ##\mathrm{d}^2 \vec{f}## is given given by ##\vec{j} \cdot \mathrm{d}^2 \vec{f}## it gives the amount of fluid flowing per unit time through the little surface element. This gets negative in your case, and it has a very simple physical meaning, but you have to consider the (arbitrary) choice between the two possibilities to orient the surface-normal vectors along the surface!

Hint: This should also become clear, if you simply flip the direction of the surface normal then the angle is ##30^{\circ}## and your current gets positive!

So Scos(150o)=πR2cos(150o) is the right choice?
 
Yes, but draw a picture and understand it (including the sign)! Physics is not about using some formula to get a result but it's about understanding why you use this formula and what it means for the phenomenon described!
 
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