Pressure and Lift around a Wing

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Airflow around a wing creates a pressure difference, with lower pressure above the wing and higher pressure below, resulting in lift. The downward motion of air is essential for generating this lift, as the wing diverts airflow downward, leading to an upward force on the wing. Bernoulli's principle indicates that faster-moving air has lower pressure, but understanding the molecular interactions behind this can be complex. Computational Fluid Dynamics (CFD) and wind tunnel tests are crucial for accurately modeling and verifying lift calculations. The discussion emphasizes the importance of recognizing the fundamental principles of aerodynamics while avoiding oversimplifications.
  • #61
boneh3ad said:
it achieves this purpose, not the other way around.
How would you feel about saying that the purpose of a planes propellor is to push air backwards or that an aircraft's engine is there to turn the propellor or that the fuel is put into make the engine go? Or even that the pilot is there to make the passengers arrive at JFK.
Causes and effects. :smile:
 
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  • #62
sophiecentaur said:
How would you feel about saying that the purpose of a planes propellor is to push air backwards or that an aircraft's engine is there to turn the propellor or that the fuel is put into make the engine go? Or even that the pilot is there to make the passengers arrive at JFK.
Causes and effects. :smile:

Well, I might argue that the pilot is there so he can earn his paycheck and eat. :wink:
 
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  • #63
boneh3ad said:
Well, I might argue that the pilot is there so he can earn his paycheck and eat. :wink:
The toe bone's connected to the foot bone, the foot bone's connected to the ankle bone . . . . . now hear de word of de lawd.
 
  • #64
boneh3ad said:
I am amused by his view of the purpose of a wing. I'd argue that the purpose of the wing is to hold up the plane, and imparting some downward motion to the air is the means by which it achieves this purpose, not the other way around. Otherwise I'd agree.

From the frame of reference of the pilot - yep, keeping that plane up is Primary. Take a look at his physics site:

http://www.av8n.com/physics/
 
  • #65
boneh3ad said:
Well, I might argue that the pilot is there so he can earn his paycheck and eat. :wink:
Well as a private pilot I spend my money to fly - unfortunately the money tree has lost most of its leaves.
 
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  • #66
Joseph M. Zias said:
Well as a private pilot I spend my money to fly - unfortunately the money tree has lost most of its leaves.
I sit in my garden and watch guys like you, flying overhead every day. I can hear the cool person of hard earned cash disappearing down a black hole. As a former boat owner, I can sympathise (by a factor of ten, at least).
 
  • #67
Fog37, In reply I think you might want to look at what happens at the leading edge of the wing. I am getting close to the limits of my understanding here.
The air running into the leading edge curve is flung/forced upwards which compacts the air above the wing, at the same time making a lower pressure near the surface of the wing. The pressure layers higher up cannot exert downward force because they are being constantly compacted and separated from the wing by the up flow from the curved leading edge.
Pretty cool question you asked, as it made me reorganize what I "knew" about airfoils and think about the details more.
Thanks
DC
Added: Are you familiar with the triangular strips of metal that are put on the leading edge of the wings, near the fuselage to make that part of the wing stall before the outboard part where the ailerons are?
Rather interesting little detail on real-world wings.
 
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  • #68
DarioC said:
I am getting close to the limits of my understanding here.
This should "get you over the top" then... . :oldwink:

Click, SHOW MORE, to see more about Doug McLean ...
.
 
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  • #69
OCR said:
This should "get you over the top" then... . :oldwink:

Click, SHOW MORE, to see more about Doug McLean ...
.
I think this is an excellent video. As an interested amateur, I wish that I had seen this decades ago. It really gives one a clue that any simple explanation necessarily omits too much and is misleading when predicting lift and drag. That is why CFD programs are used in spite of the huge amount of computer power required and the limitations of the answers.
 
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  • #70
I think this is the video I mentioned. Pulsed smoke flow in wind tunnel. Check at about 47 seconds.

 
  • #71
DarioC said:
Fog37, In reply I think you might want to look at what happens at the leading edge of the wing. I am getting close to the limits of my understanding here.
The air running into the leading edge curve is flung/forced upwards which compacts the air above the wing, at the same time making a lower pressure near the surface of the wing. The pressure layers higher up cannot exert downward force because they are being constantly compacted and separated from the wing by the up flow from the curved leading edge.
Pretty cool question you asked, as it made me reorganize what I "knew" about airfoils and think about the details more.

Air running into the leading edge is directed both over and under the wing, not simply over it. You are correct that the pressure away from the surface does not impact it directly (only the surface pressure acts on the surface), but it is related.

Consider the streamlines as they move around the airfoil over the top. Near the leading edge they are deflected upward and have a curvature whose center points away from the airfoil. Curved motion requires a centripetal force, which here must be provided by a pressure gradient. Since the pressure far from the airfoil must be atmospheric, this means that the pressure in that region must be locally higher than atmosphere. This shouldn't be surprising because this is the result of being near the stagnation point.

After that point, the curvature flips direction as the streamlines bent to follow the curve of the airfoil over the top. Now the center of curvative is in or below the wing and the pressure must therefore decrease as you approach the surface. There is therefore a low pressure near the surface at that point.

So the pressure far from the surface does not directly impact the lift force, but it definitely plays an indirect role here.

DarioC said:
Added: Are you familiar with the triangular strips of metal that are put on the leading edge of the wings, near the fuselage to make that part of the wing stall before the outboard part where the ailerons are?
Rather interesting little detail on real-world wings.

That's not what those triangles do. Those are vortex generators and they actually delay stall. The turbulence they induce energizes the boundary layer near the wall and makes it more resistant to separation.

FactChecker said:
I think this is an excellent video. As an interested amateur, I wish that I had seen this decades ago. It really gives one a clue that any simple explanation necessarily omits a too much and is misleading when predicting lift and drag. That is why CFD programs are used in spite of the huge amount of computer power required and the limitations of the answers.

Well, CFD is quite effective for lift. It isn't terribly accurate for drag. Computers do a terrible job of predicting laminar-turbulent transition, for example, and as a result do a terrible job predicting separation.
 
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  • #72
On the triangles, I think somehow you have misunderstood which "triangles" I meant. The ones I am talking about are very small long strips that are located on the leading edge of the inboard part of the wing. Their purpose is to disturb the airflow at high angles of attack and cause the inboard part of the wing to "stall" before the sections outboard that have the ailerons. The desired result is the you dump a lot of the lift of the wing before you loose roll control when the aileron area stalls. It allows you to get a good comfortable sink rate during the final flare. A Beachcraft Bonanza has them as I remember and some others I am sure. I suspect they are called something like leading edge spoilers.

They are completely different in appearance and function from the various vortex generator "tabs."

Of course air goes under the wing as well as over it, but I was talking about the air going over the wing specifically, I wasn't discussing the air going under the wing, that is why I didn't write anything about that part of the airflow.

Anyone who has compared the landing characteristics of a Piper cub versus a Taylorcraft will understand the significance of the shape of the wing leading edge. Interestingly enough those two planes were designed by the same person.
 
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  • #73
DarioC said:
I suspect they are called something like leading edge spoilers.
Stall strips... eh ? . :oldsmile:

main-qimg-f1c237b3f058011c8fd39e2873e05cd2-c.jpg


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  • #74
Yes that is one. Thanks for the photo.
 
  • #75
Thank you DarioC , Boneh3ad and everyone else.

I am back to thinking about the fundamentals of pressure.

In a fluid at rest, the pressure at a hypothetical point ##P## could be measured using a Bourdon vacuum pressure gauge (the higher the spring compression the higher the pressure). The measured pressure at the infinitesimal point ##P## is the same no matter the orientation of the gauge (pressure is isotropic both in hydrostatics and fluid dynamics).

But when the fluid is moving, the pressure at a particular point along a specific streamline will be dependent on the fluid speed and on the way we measure it: if we placed Bourdon gauge facing the fluid upstream, the fluid would come to rest against the measuring surface of the gauge and the measured pressure would depend on the fluid speed (stagnation point): the higher the flow speed the higher the stagnation pressure. At that same stagnation point, with the first gauge remaining in place, the pressure measured by an extra Bourdon gauge oriented perpendicularly to the first gauge would be the same since the pressure is isotropic.

What if we don't create a stagnation point but use a Bourdon gauge oriented perpendicularly to the streamline? I guess it is called a tap if we measure that pressure at the surface of the pipe (pressure does not change across the streamlines). What pressure would the gauge measure in that case? This pressure would be smaller than the pressure at the stagnation point and the faster the fluid is moving along the streamline the smaller that pressure measured by the Bourdon gauge would be. In both case (fluid at rest or moving), the pressure ##p## in Bernoulli's theorem is the same. However, it is interesting that its value changes depending on the way we measure it (facing the fluid and creating a stagnation point or perpendicularly to a streamline).

In a pipe that has a narrowing, since the fluid must accelerate to maintain the same flow rate (##m^3 / s##), the pressure in the narrowing must be smaller to have a pressure gradient.Thanks!
 
  • #76
fog37 said:
The pressure on top of the wing is slightly lower than the free stream pressure. This pressure distribution produces a net force Ltop on top of the wing directed downward.
Wouldn't the total force acting on the upper surface of the wing be pointing upward?
fog37 said:
The pressure at the bottom of the wing is slightly larger than the free stream pressure farther away from the wing and produces a net lift force Lbottom.
The actual pressure distribution depends on the airfoil and angle of attack, but typically, while the pressure acting on the lower surface near the trailing edge may be above free stream, the rest of the bottom surface experiences pressures less than free stream. So the total force (on the lower surface) would be directed downward, but smaller than force acting on the upper surface.

(The variable L usually stands for lift, so it's better to represent total force by F, or Fupper, and Flower).
 
  • #77
There is almost nothing about that analysis that makes sense to me. At the most fundamental level, a fluid cannot exert a pressure force on a surface in any direction other than normal to it and toward it. Any force on the upper surface points down, and any force on the lower surface points up.
 
  • #78
David Lewis said:
Wouldn't the total force acting on the upper surface of the wing be pointing upward?
That goes against all the mechanics I ever learned. A gas can't 'suck'. The lift has to be because of the fact that there is more total (positive) pressure upwards than (positive) pressure downward.
 
  • #79
The pressure above the surface is lower than the free stream atmospheric pressure. The pressure below the wing is higher than the free stream atmospheric pressure. A pressure gradient is directed from high pressure to low pressure which I assume that is where the net force point. would point.

We know lift is due to the pressure difference between the top and bottom surface. But, given the relative difference between free stream pressure and the pressures at the wing produce a net force point down on both the top and bottom surfaces?
 
  • #80
Again, it is literally impossible for a fluid to "pull" on a surface. The force is always directed normal to and into the surface. Always.
 
  • #81
Ok, I finally get it. What matters is the local pressure distribution on the top and bottom surfaces of the wing to produce the net lift force.

A gradient is a vector pointing from small to large values. I guess I got confused about these negative of the pressure gradients, ##- \nabla p##, one directed towards from the top surface and one directed away from the bottom surface.
 
  • #82
fog37 said:
a net force point down on both the top and bottom surfaces?
I suggest that you really meant to use the word towards ?
 
  • #83
Diagram of lift coefficient distribution from Airplane Performance Stability and Control -- Perkins and Hage.
 

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  • #84
fog37 said:
The pressure above the surface is lower than the free stream atmospheric pressure. The pressure below the wing is higher than the free stream atmospheric pressure. A pressure gradient is directed from high pressure to low pressure which I assume that is where the net force point. would point.
One needs to be careful about the difference between pressure and pressure gradient. The pressure force is always normal to the surface and directed from the gas toward the surface. The pressure gradient is derived from the difference in pressure. It is positive in the direction of increasing pressure. It is not the same as the force from the pressure and positive is in the opposite direction from the force.
We know lift is due to the pressure difference between the top and bottom surface. But, given the relative difference between free stream pressure and the pressures at the wing produce a net force point down on both the top and bottom surfaces?
The force on both surfaces is from the gas side toward and normal to the surface. If there is lift, the total force on the bottom is greater than the total force on the top.
 
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  • #85
FactChecker said:
The pressure gradient is derived from the difference in pressure.
The difference between which pressures?
FactChecker said:
The pressure force is always normal to the surface and directed from the gas toward the surface.
There is pressure (force/area), and then there is force. Which one are you analyzing? If it's force, then aerodynamic force has both normal and tangential components. The tangential component (skin friction) arises due to viscosity within the boundary layer.
 
  • #86
David Lewis said:
The difference between which pressures?
Between the pressures at two infinitely close points. It's a derivative of the pressure.
There is pressure (force/area), and then there is force. Which one are you analyzing?
Sorry. I should have said the force due to the pressure.
If it's force, then aerodynamic force has both normal and tangential components. The tangential component (skin friction) arises due to viscosity within the boundary layer.
Good point. I was ignoring any tangential force for discussion of lift. Actually, this is not my area of expertise and I am not sure exactly how the viscosity relates to pressure in this situation.
 
  • #87
boneh3ad said:
Again, it is literally impossible for a fluid to "pull" on a surface. The force is always directed normal to and into the surface. Always.

Hi Boneh3ad,
I am still pondering about Bernoulli's equation: in Bernoulli's equation where the pressure ##p## is called static pressure and the term ##\frac{\rho v^2}{2}## is called dynamic pressure. Is the term ##p## called static because it is measured by a device that is not moving relative to the fluid? Any device moving at the same speed as the fluid would measure zero pressure. The dynamic pressure term can only be measure by bringing the fluid to rest (at a stagnation point). So it is the just the increment to ##p## when we measure ##p## exactly against the direction of fluid motion perpendicular to the streamline. We would only measure ##p## if we measured the pressure parallel to the streamline. Somehow that pressure parallel to the streamline is affected by the speed of the fluid (the faster the fluid the lower that pressure and the higher the stagnation pressure).

Does this make any sense?
 
  • #88
fog37 said:
Is the term ##p## called static because it is measured by a device that is not moving relative to the fluid?

Static pressure is so named because it is the pressure that has to due with the fluid's state (as opposed to its motion). It is otherwise known as thermodynamic pressure or just pressure.

fog37 said:
Any device moving at the same speed as the fluid would measure zero pressure.

This isn't true. A device moving at the same speed as a given fluid would still register a pressure due to the impact of the various fluid molecules on the sensing element.

fog37 said:
The dynamic pressure term can only be measure by bringing the fluid to rest (at a stagnation point).

Dynamic pressure can never be measured. You can measure static pressure using a static port (i.e. a pressure port that does not disturb the flow in any way that alters its velocity, usually flush-mounted in a surface in the flow). You can measure total pressure (or stagnation pressure, if you prefer) with a Pitot probe that slows the flow down to zero at the measurement point. The different between these two allows you to calculate the dynamic pressure (in an incompressible flow).

fog37 said:
So it is the just the increment to ##p## when we measure ##p## exactly against the direction of fluid motion perpendicular to the streamline. We would only measure ##p## if we measured the pressure parallel to the streamline. Somehow that pressure parallel to the streamline is affected by the speed of the fluid (the faster the fluid the lower that pressure and the higher the stagnation pressure).

I am having a hard time understanding what you are saying here. The first portion is very confusing, and the second portion seems to make a conceptual error in the phrase "pressure parallel to the streamline". Pressure is a scalar quantity. It has no direction, so all of this talk of perpendicular and parallel really doesn't make sense to me.
 
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  • #89
fog37 said:
Any device moving at the same speed as the fluid would measure zero pressure.
Zero gauge pressure, perhaps (with respect to itself?), but it would still have absolute pressure.

Note: in practice, essentially all pressure is measured as gauge pressure. Even a supposed absolute pressure measuring device just uses a reference pressure of a vacuum. This is useful to remember for the next issue...
The dynamic pressure term can only be measure by bringing the fluid to rest (at a stagnation point).
That's total pressure. As said previously, dynamic pressure is total pressure minus static pressure. But you can measure dynamic pressure in one shot by using static pressure as the reference pressure, as in a pito-static tube.
So it is the just the increment to ##p## when we measure ##p## exactly against the direction of fluid motion perpendicular to the streamline. We would only measure ##p## if we measured the pressure parallel to the streamline.
You have some jumbled words there, but in general, its static pressure that is measured by orienting the pressure port parallel to the flow and total pressure or dynamic pressure measured by orienting it perpendicular to the flow.
Somehow that pressure parallel to the streamline is affected by the speed of the fluid (the faster the fluid the lower that pressure and the higher the stagnation pressure).
The first part isn't correct: Since static pressure is measured the same whether you are moving with the flow or not, it wouldn't be correct to say it is in general lower for higher speed fluid. For example, an airplane's static pressure port measures exactly the same static pressure regardless of its own speed. But the dynamic pressure is a function of speed.
 
  • #90
russ_watters said:
Zero gauge pressure, perhaps (with respect to itself?), but it would still have absolute pressure.

It wouldn't necessarily be zero gauge. It depends on what the gauge is measured against. For example, in wind tunnel testing, gauge pressure is usually measured against local atmosphere, which is not the same as the static pressure at the port location, so the gauge pressure would be nonzero.

russ_watters said:
Note: in practice, essentially all pressure is measured as gauge pressure. Even a supposed absolute pressure measuring device just uses a reference pressure of a vacuum. This is useful to remember for the next issue...

The definition of absolute pressure is pressure referenced to a vacuum, so in that sense, you are measuring both a gauge and absolute pressure simultaneously. They are the same in this instance.

russ_watters said:
The first part isn't correct: Since static pressure is measured the same whether you are moving with the flow or not, it wouldn't be correct to say it is in general lower for higher speed fluid. For example, an airplane's static pressure port measures exactly the same static pressure regardless of its own speed. But the dynamic pressure is a function of speed.

Be careful here. This applies to the static pressure port related to the Pitot-static system on an airplane only because those systems are designed to measure static pressure where the velocity is locally equivalent to the free stream. It would not be correct to apply this to static pressure in general. Consider a series of static pressure ports along the chord of an airfoil moving at constant velocity. They will all be registering different static pressure values owing to the varying flow speed over that portion of the wing.
 

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