# Wind Energy Physics

Intermediate

Wind Energy Physics
The swept area of a turbine is its aperture window that captures the wind. The area is directly proportional to the amount of wind energy available to the turbine.
Believe it or not, one-bladed turbines have the highest potential power coefficient, but they are difficult to keep balanced. Two- and three-bladed turbines are the proven standard, balancing aerodynamic efficiency and stability during turbulent winds.
Ducts and shrouds are common attempted augmentations to divert more wind into, or increase wind speed through, the turbine’s blades. However, the nature of fluid dynamics makes the wind adept at flowing around these obstructions rather than through them. Savvy turbine designers use larger swept area to increase power input instead of trying to trick the wind.
Multiple blades only help in getting the turbine started in low-wind situations. After that, one blade’s wake quickly interferes with the blade following it.
Many “innovative” designs just complicate a system that would work better if simplified. Luckily, most kooky designs never leave the prototype stage.

Wind turbine design encompasses multiple disciplines, but perhaps the most important—and often the least understood, even by would-be turbine designers—is fluid dynamics. Understanding the physics laws that govern wind power, presented here, can help consumers make wise wind turbine technology choices.

## The Energy Equation

The purpose of a wind turbine is to convert kinetic energy (energy of a moving mass) of the wind into electrical energy. Energy conversion is common to all machines because they must obey the law of energy conservation—energy cannot be created or destroyed, but only changed from one form to another. For example, your car converts the chemical energy stored in fuel (if it’s an electric car, batteries) to kinetic energy, moving it down the road. A wind turbine also obeys this law when it extracts the kinetic energy in the wind and converts it to electrical energy.

The amount of kinetic energy in any moving mass is calculated with this equation:

Kinetic energy = 1/2 × mass × velocity2

For wind energy, the velocity in the equation is wind speed. The mass is for a particular volume of air. Consider the example of wind blowing through an open window. The illustration describes how a volume of the air passing through the window relates to window area, wind speed, and time. This makes sense if you consider that the larger the opening, the harder the wind is blowing, and the longer the window is open, the more air volume will flow through it.

The mass of this volume of air is arrived at by multiplying the volume by the air density. Putting this all together, we write our equation for wind energy as:

Kinetic energy = 1/2 × air density × area × wind speed3 × time

## Power in the Wind

Although a wind energy system’s final objective is to generate energy, it is more convenient to describe its size in terms of power. The relationship between power and energy is a simple one—energy is power multiplied by time. This is why power is defined in watts and energy in watt-hours. The terms power and energy are often confused and even used interchangeably in casual discussions, but in a technical analysis, it is important to make the distinction.

If we are interested in the power in the wind, we divide the energy by time. This gives us the governing equation for power available in the wind passing through an area as:

Pwind = 1/2 × air density × area × wind speed3

We see that the amount of wind power is dependent on three variables. The first is air density, a quantity defined by Mother Nature, over which we have no real control. Another is swept area, that is, the projected area perpendicular to the wind that the turbine intercepts. One thing is clear from the equation: everything else being equal, a larger swept area can generate more power.

## Pages

I agree with you, the wind creates a difference in pressure on the profile of the wing. The pressure difference with the blade surface creates a force. This force may be decomposed into an axial force and a normal force. The axial force associated with the radius of the blade creates a motor torque. Normal force creates stresses on the blade. For a sailboat, the axial force allows to advance it, the normal force creates constraints on the sail and makes lodging the sailboat. My project is to transform these constraints into additional energy recovery. There will be a wind turbine model and a tidal turbine model and after two prototypes

I understand your concept and I admit it is tempting to try to harness that very strong normal force. But I would caution you that it cannot be done for free. What I mean is that the simple act of allowing the blade to move in a new path - in the direction of the wind - will change the relative wind velocity experienced by the blade, and hence change the axial force on it - the component of force that produces the torque. Your sailing analogy is apropos. The normal force on the sail tends to heel the boat and not move it forward. This heeling force can be reduced by eliminating the keel and allowing the boat to drift downwind. The boat will not go faster, however, as the boat just drifts downwind. The moral of the story is the normal force is the price paid for the efficiency achieved by the design. I think you will find that harnessing the normal force will actually reduce overall efficiency, not increase it. But again, good luck and let us know how your tests turn out.

I appreciate your comments. I wrote for a simpler theory for students in engineering school and I am transforming it into latex to publish an article and I also prepare a video.
Thank you

I would like to make a comment on the power factor. It is limited to about 60% from the Betz limit. This law is defined according to the calculation of kinetic energy. Large wind turbines are stopped when the wind is too strong. They do not produce too much but they are subject to excessive stresses which can break the blades. For a Darrieus turbine at each turn, the arms have extension and compression stresses. By using a crank-rod system, it is possible to recover additional energy. Theoretically it is possible to have a yield higher than the limit of Betz.

Interesting comment normandajc. Simple physics says that an applied force must result in acceleration or load (stress) on an object. For a wind turbine the applied force is from the wind. You can come up with all sorts of ways to convert that applied force to useful energy, but in the end, you are always constrained by the laws of physics. I wish you luck with your new concept, but I would not count on being able to defeat physics. But please share your results if you decide to pursue your concept to a prototype field test unit.

Kenslow is actually correct. Betz totally ignores rotation in his calculations, and Glauert admits the calculations are wrong if rotation occurs. See page 194 of his most famous work "Airplane propellers", he proved nothing about wind turbines and was primarily focused on propeller design, only 17 out of 191 pages cover wind turbine design and they contain errors. Glauert died in 1934 before it was published and without proof reading it.

The differences between Betz' and Glauert's approaches explain the absence or inclusion of wake rotation in the calculations. Betz took the simplest approach of treating the entire turbine rotor as an ideal disc, often referred to as actuator disc theory (ADT). ADT considers the flow through the plane of the rotor as a whole. As such, it is both highly simplified and non-conservative since it treats the entire rotor area as having the same efficiency without considering real effects such as tip and hub losses, not to mention differences along the span of the blades.
Glauert uses the more realistic approach of dividing the blades into spanwise sections, often referred to as Blade Element Momentum (BEM) theory. This approach attempts to calculate the contribution of each spanwise position of each blade, omitting the hub (which has no airfoil) and including changes along the span due to different angular velocities.
Because ADT only considers flow through a plane, any rotational velocity would be irrelevant because the component of velocity that is not perpendicular to the plane would not pass through the plane. BEM can account for rotational velocity because the rotational component changes the inflow velocity and angle of attack for individual blade elements. BEM is certainly the more accurate method to determine propeller performance and is commonly used in wind turbine aero-elastic design codes today.
Having said all that, Betz' approach still represents an ideal case where all the flow through the disc (note that Betz' theorem is not limited to propellers, nor even circular discs or in fact even to air) is converted to useful power. If such an ideal disc could be created (it can't, but the propeller has proven to come closest), it could approach the Betz Limit for efficiency. A propeller may be influenced by rotational velocity components that Betz ignores, but any gains can never make up for the real-world losses of a real propeller (tip, hub and frictional losses), let alone exceed the ideal theoretical limit proven by Betz.
In summary, BEM is the more accurate approach for wind turbine design because it more accurately reflects reality. But reality does not solely incur benefits; the Betz limit still applies.

Awesome! Do you want to write a BPB "Back Page Basics" for HP (and for our non aero-physist readership) about theoretical max power from the wind. We don't need to nit-pick over a few percentage points...that's for the engineers. But we'd love for the typical reader to understand the limits, and recognize BS in the new-design investment scams.

I'd be happy to write more on this topic Ben, though it sounds like you are asking for a summary of this very article. Please clarify if there is something more or different that you feel was not covered and maybe HP will consider it.

Yes, more precisely, Betz, Glauert, and modern Blade Element Momentum Theory all rely on the flawed 19th century Froude's actuator disc theory. This is part of the problem, Froude's ADT equations are in fact invalid and diverge from that of real airflow as axial induction factors approach 0.5. Also most all methods including Glauert's are based on simplifying assumptions which either remove or improperly account for rotational terms within the energy equation. That said, my only point is to emphasize that these are strictly very outdated theorems, not laws nor physical limits, and to accept otherwise serves only to stifle innovation.

It is important to remember that the theorems are just models, varying in complexity, and must be viewed as such. All engineering uses models to some extent, with the critical aspect being that the assumptions on which the model is based are applicable to the real situation being modeled. Therefore I would not categorize the ADT as "flawed" or even "outdated." It is a very good tool for a generalized performance model of energy extraction from a fluid flow. It is not so good for wind turbine blade design. I also would not blame the theorems for stifling innovation. If one chooses to use use the wrong tools for design, it is not the tools fault.
Finally, the ADT is in fact quite valid for what it is intended as it is based on fundamental fluid physics. As the article states, the Betz proof is technology agnostic and simply defines the amount that a fluid must be slowed (by 2/3rds) to maximize power extracted from the flow. It is quite valid for this purpose and is applicable to wind turbines regardless of any other - better - tools used to design them.

From your refernced source, Martin Hansen's Aerodynamics of Wind Turbines, 2nd ed. page 41 "It is possible to exceed the Betz limit by placing the wind turbine in a diffuser."

Hansen makes the mistake (in my view) of ignoring the area intercepted by the diffuser. By ignoring the diffuser area one can claim that the turbine could exceed the Betz limit, but this is technically incorrect, and - as Hansen notes - the diffuser has to be accounted for both structurally and economically (so why not aerodynamically?). Furthermore, as Hansen also notes, this concept of an augmented rotor "beating Betz" by (erroneously) ignoring the diffuser area has never been demonstrated on a full-size turbine despite many attempts costing many millions of dollars.

Betz limit is not a true limit. It doesn't take rotational velocities into account. That's why it was immediately discounted by the engineering community when it was claimed.

Michael,

I am not aware of Betz' theory being discounted by the engineering community when it was proposed in 1919, so please share any evidence you have in that regard. As for it not being a "true limit" you are correct in so far as it is only a theoretical limit and can never be truly achieved with a real wind turbine.
I am unsure of what you refer to as "rotational velocities," but the effect of wake rotation has been considered in regards to wind turbine rotor efficiency. In 1935, British aerodynamicist Hermann Glauert investigated the effect of wake rotation on theoretical rotor efficiency. His conclusion reinforced Betz' result, proving that the theoretical efficiency approaches 16/27 as the tip speed ratio of the rotor approaches infinity. [ref: Hansen M. O. L. (2015). Aerodynamics of Wind Turbines]

Not sure what your point is. Are you saying that the Betz limit might be higher if you consider rotational velocities? Or lower?

I don't think your question was directed to me Michael, but you raise an interesting point. A propeller rotor induces a rotational velocity as well as an axial velocity on the inflow. In general this provides no benefit but rather a loss because that induced rotation is energy imparted by the rotor into the flow (assuming no rotation originally exists in the inflow). There is potential that inflow with rotation could provide benefit to a rotor that induces opposite rotation, but that would require a specific condition that is unlikely in reality, and the benefit would not be great since the rotational induced velocity is a much smaller effect than axial induced velocity from which the vast majority of power is extracted from the flow. And in the end, ideal rotational velocity on a real rotor cannot provide enough benefit to exceed the ideal condition described by Betz in the theoretical world prescribed by the laws of physics.