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

In summary, the maximum power equation changes when there is an angle to the way the wind falls into the wind turbine's blades. The equation becomes Pmax= 8/27Sρu13, where S=Scosθ. When there is an angle of θ=150ο, the equation becomes Pmax= 8/27Sρu13, where S=πR2cos(150o). This is the correct choice, as cos(150o) gives a negative number which makes sense in the physical context. It is important to understand the reasoning behind using this formula and its implications.
  • #1
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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  • #2
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.
 
  • #3
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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  • #4
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!
 
  • #5
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?
 
  • #6
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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1. What is the difference between flow across a rotating surface's face and flow across a stationary surface's face?

Flow across a rotating surface's face refers to the movement of a liquid or gas across a surface that is in motion, while flow across a stationary surface's face refers to the movement of a liquid or gas across a surface that is not in motion. The rotation of the surface can greatly affect the flow patterns and dynamics of the fluid.

2. How does the rotation speed of the surface affect the flow?

The rotation speed of the surface can greatly influence the flow across its face. Higher rotation speeds can lead to increased turbulence and mixing, while lower rotation speeds can result in smoother flow patterns. The specific effect will depend on the specific fluid properties and surface geometry.

3. What is the Coriolis effect and how does it impact flow across a rotating surface's face?

The Coriolis effect is the apparent deflection of a moving object due to the rotation of the Earth. In the context of flow across a rotating surface's face, the Coriolis effect can cause the fluid to deflect in a direction perpendicular to the rotation axis. This can result in complex flow patterns and can affect the overall flow rate and direction.

4. Are there any practical applications for understanding flow across a rotating surface's face?

Understanding flow across a rotating surface's face is crucial in various industries such as aerospace, energy, and manufacturing. It is used to design and optimize systems such as turbines, pumps, and mixers. It is also important in understanding the flow of fluids in natural systems such as oceans and atmospheric weather patterns.

5. What are some methods for studying flow across a rotating surface's face?

There are several methods for studying flow across a rotating surface's face, including computational fluid dynamics (CFD), wind tunnel experiments, and analytical models. CFD allows for detailed simulations of the flow patterns and can provide insights into the underlying physics. Wind tunnel experiments involve physical testing of models to observe the flow in real-time. Analytical models use mathematical equations to predict the behavior of the fluid and can provide quick approximations of the flow. Each method has its advantages and is often used in combination for a more comprehensive understanding of the flow.

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