Questions about density and being in the air

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The discussion centers on the principles of lift generation in helicopters and the misunderstanding of density versus pressure. One participant argues that lift is created by a difference in air density above and below the rotor blades, while another asserts that lift results from the rotor's downward thrust and the resulting pressure differential, not density changes. The conversation highlights that lift can be explained through Newton's laws, emphasizing that pushing air down generates an upward force. Additionally, the participants clarify that the mechanics of lift involve pressure changes rather than density differences, and that the rotor functions similarly to an airfoil. Overall, the debate underscores the importance of distinguishing between pressure and density in understanding lift dynamics.
  • #31
Student100 said:
That we are treating air as a Newtonian fluid in the discussion, and that it will flow "Newtonianally"? For the air to push downward it must flow? To thereby use Newton's third law?
The OP never mentioned anything about a Newtonian fluid in his post. In fact, I doubt if he even knows what a Newtonian fluid is. For all we know, the fluid could be an Euler fluid, and everything that was said in the responses applies equally well to Euler fluids. So why did you feel it was necessary to defend what you wrote when Nasu pointed out your error? Everyone reading this thread recognized right away that you were confusing Newton's third law with the flow relationship for Newtonian fluids. We wouldn't have held that against you. Everybody has these mental lapses. Why couldn't you just let it go at that? Now you've called attention to it for the third time.

Chet
 
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  • #32
Student100 said:
For the air to push downward it must flow? To thereby use Newton's third law?
Separate issues. Going back to the sealed box example, imagine a fan mounted within a vertical duct in a horizontal plane inside the box so that the only flow within the box is through the fan. After the initial transition, there is no vertical component of flow, just an increased pressure differential within the box maintained by the fan.

Newton's third law still applies even if there is no flow, but just a pressure differential.
 
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  • #33
Student100 said:
Thanks Russ, I had just assumed they all operated like blowers.
Note that even blowers can be different types and use mixtures of different operating principles. You can reverse the curvature of the blades or even spin a blower backwards and it will still move air in the same direction (just not necessarilly as well)!

https://www.cincinnatifan.com/blower-wheels.htm
 
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  • #34
rcgldr said:
Separate issues. Going back to the sealed box example, imagine a fan mounted within a vertical duct in a horizontal plane inside the box so that the only flow within the box is through the fan. After the initial transition, there is no vertical component of flow, just an increased pressure differential within the box maintained by the fan.

Newton's third law still applies even if there is no flow, but just a pressure differential.

Seems like an apple to oranges comparison. One that in itself applies idealizations to the box, blower, and flow- physics itself is an idealization of nature. I don't understand why this is so controversial.

I still don't understand how you apply N3 to lift and not call it an idealization, but then call pressure differentials an idealization. Flows are non-inertial - the entire system is non-inertial. The entire idea behind Navier-Stokes is apply N2, with viscosity and turbulent flows. You simplify the calculations by looking at a time average for turbulence, and further simplify it by treating the air as a Newtonian fluid with linear viscosity. To use N2, you then introduce the fictitious forces. If this is the case, as far as I understand it, using N3 to calculate lift must be an idealization, as much so as the pressure differential treatment.
 
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  • #35
Khashishi said:
A fan blade is basically the same as a wing. The blades on a propeller are thinner than a house fan because it is engineered to spin faster but it's not that different. (A thick fan blade would cause some problems with cavitation as the air could not replace itself after the path of blade in time for the next blade.)

Hmm. This is not very right. The blades on a typical box fan are a fairly thin, and the blades on an aeroplane propeller thicker.

The thin box fan blades fulfill to criteria. They are less expensive to produce than thick blades, and can be nearly as efficient as they operate at a nearly constant angle of attack. The thicker blades of an airplane propeller, in general, will have the airflow attached over a greater length of the cord, thus less drag, more lift and more efficient.

Airplane propellers do not suffer cavitation. In addition, cavitation in ship propellers is not a result of interference between blades. Cavitation results from local low pressure areas generating gas voids.
 
  • #36
Student100 said:
I still don't understand how you apply N3 to lift and not call it an idealization.
I never claimed that you could calculate or model lift solely based on Newton's third law, only that it applies to all forces, since all forces only exist as one part of a Newton third law pair of forces.
 
  • #37
rcgldr said:
I never claimed that you could calculate or model lift solely based on Newton's third law, only that it applies to all forces, since all forces only exist as one of a Newton third law pair of forces.

In inertial frames. This isn't an inertial frame of reference.
 
  • #38
rcgldr said:
... all forces only exist as one part of a Newton third law pair of forces.

Student100 said:
In inertial frames. This isn't an inertial frame of reference.
If the ambient air (the air unaffected by an aircraft) is used as a frame of reference, it is an inertial frame. If an aircraft is not accelerating, then the wing as a frame of reference is an inertial frame.
 
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  • #39
rcgldr said:
If the is air is used as a frame of reference, it is an inertial frame. If an aircraft is not accelerating, then using the wing as a frame of reference is an inertial frame.

Then why introduce fictitious forces into the proper calculations of lift if we could simply agree on an inertial frame of reference?

Flows I thought could never be considered inertial frames.

Inertial frames are all just approximately inertial frames correct?
 
  • #40
Student100 said:
Flows I thought could never be considered inertial frames.
I updated my prior post. It's the ambient air (air unaffected by an aircraft) that can be used as an inertial frame of reference, or the ground in a no-wind situation.
 
  • #41
rcgldr said:
I updated my prior post. It's the ambient air (air unaffected by an aircraft) that can be used as an inertial frame of reference, or the ground in a no-wind situation.

Even that air is subject to the fictitious forces to apply N1 & N2, is this not correct?
 
  • #42
rcgldr said:
... the ambient air (air unaffected by an aircraft) that can be used as an inertial frame of reference, or the ground in a no-wind situation.
Student100 said:
Even that air is subject to the fictitious forces to apply N1 & N2, is this not correct?
Ignoring issues related to the rotation of the earth, the ambient air (the air unaffected by the aircraft), is not accelerating. The only idealization here is assuming that ambient air would not be accelerating. The same idealization is also made when using the wing as a frame of reference, as the oncoming flow approaching a wing is considered to have constant velocity. I don't see how any fictitious forces could exist from the perspective of an inertial frame.
 
  • #43
rcgldr said:
Ignoring issues related to the rotation of the earth, the ambient air (the air unaffected by the aircraft), is not accelerating. The only idealization here is assuming that ambient air would not be accelerating. The same idealization is also made when using the wing as a frame of reference, as the oncoming flow approaching a wing is considered to have constant velocity. I don't see how any fictitious forces could exist from the perspective of an inertial frame.

But you have to make assumptions about the fluid to make it inertial. That's my entire confusion here, is that not an idealization? Would such an event ever occur in nature? Then is it not an idealization to apply N3 to lift?

That's all I'm trying to clear up.
 
  • #44
Student100 said:
you have to make assumptions about the fluid to make it inertial.
I'm not sure I understand your point here, but I'm going to guess that you're thinking that if a fluid is not a Newtonian fluid, then it doesn't follow Newtonian physics, which isn't true. A Newtonian fluid is a fluid in which the viscous stresses arising from its flow, at every point, are linearly proportional to the local strain rate. It's a idealization of viscosity, not about Newton's laws of physics. Wiki article

http://en.wikipedia.org/wiki/Newtonian_fluid

Regardless of viscous effects, in an inertial frame of reference, then all fluids would be "inertial". A force exerted onto the air, results in a change in pressure and/or temperature and/or acceleration, and the reaction follows Newton's laws of physics.

Getting back to the original posters question, a change in pressure coexists with a change in density. Wiki article:

http://en.wikipedia.org/wiki/Compressibility_factor#Compressibility_of_air

In the case of a wing, a density differential coexists with the pressure differential, but it's the net pressure differential on a wing that corresponds to lift and drag forces exerted by the air onto the wing. For level flight, you can calculate the net pressure differential by the wing loading divided by the wing area.

http://en.wikipedia.org/wiki/Wing_loading

Take the example of a large commercial aircraft, the MD-11F, at 173 lbs / ft^2 wing loading, this is equal to about 1.2 psi (lbs / in^2) net pressure differential. Say this is distributed as +0.4 psi below the wing and -0.8 psi above. At near sea level where ambient pressure is about 14.7 psi, these differences are relatively small: +0.4/14.7, -0.8/14.7. At 35,000 feet, ambient pressure is only 3.2 psi, so the relative differences in pressure (and density) are greater, but the net pressure differential is the same. At higher altitudes, due to the lower density of the air, a greater speed and/or greater angle of attack is needed to maintain level flight.
 
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  • #45
Going back to the original point made:

Air is not a perfect fluid, and the concept of pressure is an idealization. But Newton's third law is not an idealization. Push air down and you go up. That's the ONLY way you can generate lift with a wing.

My point, Newtons third law is an idealization.

To apply it we have to consider an inertial frame of reference. This doesn't exist in lift calculations. Therefore, to apply N3 we make assumptions about the fluid and the plane, or an idealization of an otherwise complex interaction.

The discounting of pressure because it's an idealization, is therefore, flawed.
 
  • #46
I must be missing something -- what is the difficulty here?

An airfoil and a typical (box) fan blade and a ship's propeller all operate on essentially the same principle. Toy helicopters are in fact found with blades very similar to house fans, and they fly. There are also sails, which have basically no thickness at all and are found in all sorts of widths and aspect ratios.

Is there some controversy about whether Newton's 3rd law is true?
 
  • #47
Student100 said:
My point, Newtons third law is an idealization. To apply it we have to consider an inertial frame of reference.
Newton's third law is not something you apply as part of a calculation, it simply exists. As stated before all forces only exist as one of a pair of Newton third law forces. In this case, the aircraft exerts a force onto the air, and the air exerts an equal in magnitude but opposing force onto the aircraft.

Student100 said:
This doesn't exist in lift calculations.
Generally 3d lift calculations divide the upper and lower surfaces of a wing into a very large number of tiny squares, and calculate the pressure at each square, then sum up these pressures to determine the net pressure differential that corresponds to the force that the air exerts onto the wing. Newton's third law still applies, it would be the force that the wing exerts onto the air.
 
  • #48
Student100 said:
Going back to the original point made:
My point, Newtons third law is an idealization.

To apply it we have to consider an inertial frame of reference. This doesn't exist in lift calculations. Therefore, to apply N3 we make assumptions about the fluid and the plane, or an idealization of an otherwise complex interaction.

The discounting of pressure because it's an idealization, is therefore, flawed.

You mean that the Earth is not good enough as an inertial system for lift calculation? What assumption do you need to make about fluid in order to apply Newton's third law?
Are you thinking about the effect of Coriolis forces in lift calculations?

It's not clear why did you even bring in the discussion the inertial systems. It looked like you did it just to keep arguing about the "idealization" of Newton third law.

This seem to go around in loops. :)
Or rather in spiral, getting more and more remote from the original question.
 
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  • #49
I like the N3 explanation better than the pressure difference explanation simply because my daily observation said so

Why does a toy helicopter goes higher when I put my palm about 5 inches under it ? Saying that the pressure difference becomes higher as the volume of air under the heli becomes smaller can't be true as my hand won't change the volume. It goes higher because it exerts force on my palm, which will push the toy upward.

And why can't helicopters climb as high as aircraft ? Some may say that the air density would be too low for it to generate lift, but hey, the decrease of air density under the rotor should be directly proportional with the decrease of air density above the rotor, it should still be able to generate lift right ?

thus I concluded at too high of altitude, the air under the rotor becomes too light to exert force on, which result in the helicopter unable to climb no more

And excuse me for my English.. Its not my first language
 
  • #50
Ariel24K said:
And why can't helicopters climb as high as aircraft ? Some may say that the air density would be too low for it to generate lift, but hey, the decrease of air density under the rotor should be directly proportional with the decrease of air density above the rotor, it should still be able to generate lift right ?
How much lift do you think a helicopter could generate on the moon where the air density is zero?

Density is not a force, so it can't be directly associated with lift (which is a force). On the other hand, pressure is a force per unit area normal to surfaces, and so pressure differences are the direct cause of lift.

Chet
 
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  • #51
Chestermiller said:
How much lift do you think a helicopter could generate on the moon where the air density is zero?

Density is not a force, so it can't generate lift. Pressure, or rather pressure differences, generate lift. This is a force.

Chet

Ah sorry I got the density and pressure difference mixed up after reading the original post, thanks for clearing up
 
  • #52
Some people here are making this way too complicated. Air flow around helicopter blades is approximately incompressible. You can assume incompressible flow and get very close to the right aerodynamics, good enough unless you are actually designing a high performance helicopter blade, in which case you wouldn't be asking this question.

Incompressible means density doesn't change. Lift derives from the difference in pressure, in simple terms the Bernoulli equations with constant density (rho).
https://en.wikipedia.org/wiki/Bernoulli's_principle

Compressible flow occurs as the flow approaches the speed of sound, so don't worry about it, and it doesn't change one's understanding of the answer. For buoyancy to matter you need something the size of a blimp, not a blade.
 

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