Derivation of the change of air pressure with height

In summary: Yes, the weight of the air above exerts a downward force. According to the 3rd law there must be a corresponding counterforce, acting upward on the Earth and according to the 2nd law the air would be accelerated if this would be the only force acting on it. But in the static case the air doesn't accelerate. Therefore there must be another force acting on the air. Do you agree? If yes, which force is this?The force that acts on the air is the pressure from above the slab. This is the pressure that balances the weight of the air above.
  • #1
Adesh
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If we take a slab of air with cross-sectional area of [itex] A[/itex] and height [itex] dz[/itex] in our atmosphere. Now, what we do is make an argument like this :-

Pressure from below must balance both the weight and Pressure from above to keep the slab at rest. ( I have added an attachment for clarification)

And from this are argument we do something like this :
[itex] P_{above} = P [/itex]
[itex] W_{slab} = mg [/itex] , Pressure from weight is [itex] \rho \times A \times dz \times / A = \rho ~dz~g [/itex] ( [itex] \rho [/itex] is the density of air)

Therefore, [itex] P_{below} = P + \rho~dz~g [/itex]

[itex] dP = P_{above} - P_{below} = - \rho ~dz~g [/itex]

[itex] \frac{dP} {dz} = - \rho ~g [/itex]

Now, my question is why we didn't not take into account the weight of air which is above the slab? I mean the air which lies above our sample slab must have weight this weight would have been pushing our slab downwards and therefore pressure from below must also balance this. The mass of air which lies above the slab must have number molecules and gravity would attract them and we should center of mass and assume the gravity to act over there and this force of gravity should cause a pressure on our slab.

I tried to argue that pressure from above is due to weight of air only, but after sometime I thought that this argument is not good as fluid causes pressure due to collision of it's molecules .

So, I want to restate my problem again : Why in our derivation we didn't take into account the pressure caused by the weight of the air that lies above our slab?

Thank you, any help will be much appreciated. I tried to be as clear as I could be.
 

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  • #2
Adesh said:
So, I want to restate my problem again : Why in our derivation we didn't take into account the pressure caused by the weight of the air that lies above our slab?

What do you think what ##P_{above}## is?
 
  • #3
DrStupid said:
What do you think what ##P_{above}## is?
It is the collision of air molecules.
 
  • #4
Adesh said:
It is the collision of air molecules.

That's the microscopic view. From a macroscopic point of view pressure is force per area. In case of ##P_{above}## this force comes from the air above. Do you agree?
 
  • #5
Adesh said:
Now, my question is why we didn't not take into account the weight of air which is above the slab?
The weight of the air above does not act on the slab of air. Why would we include it in the forces on the slab?

When you do a free body diagram you include only forces acting on the body in question. In this case there are three such forces on the slab: the pressure from above the slab, the pressure from below the slab, and the weight of the slab. The weight of the air above does not act on the slab. Including it would be wrong.
 
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  • #6
DrStupid said:
That's the microscopic view. From a macroscopic point of view pressure is force per area. In case of ##P_{above}## this force comes from the air above. Do you agree?
Yes.
 
  • #7
Dale said:
The weight of the air above does not act on the slab of air. Why would we include it in the forces on the slab?

When you do a free body diagram you include only forces acting on the body in question. In this case there are three such forces on the slab: the pressure from above the slab, the pressure from below the slab, and the weight of the slab. The weight of the air above does not act on the slab. Including it would be wrong.
That's what I want to know. Why including it will be wrong?
 
  • #8
Adesh said:
Why including it will be wrong?
Because it doesn’t act on the slab. Only forces acting on the slab should be included.
 
  • #9
Dale said:
Because it doesn’t act on the slab. Only forces acting on the slab should be included.
So on what it acts?
 
  • #10
Adesh said:
So on what it acts?
The weight of the air above acts on the air above. Is that somehow not obvious?

The weight of any object is the gravitational force acting on that object. The thing that it acts on is literally part of the definition of the weight. How can this be unclear?

What do you think weight is?
 
  • #11
Adesh said:
Yes.

OK, the air exerts a downward force. According to the 3rd law there must be a corresponding counterforce, acting upward on the Earth and according to the 2nd law the air would be accelerated if this would be the only force acting on it. But in the static case the air doesn't accelerate. Therefore there must be another force acting on the air. Do you agree? If yes, which force is it?
 
  • #12
The weight of the air above is captured in the pressure above, ##p_{above}##
 
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  • #13
Chestermiller said:
The weight of the air above is captured in the pressure above, ##p_{above}##
Really? thank you I had same thought but I was fearing that I would be wrong.
 
  • #14
Dale said:
The weight of the air above acts on the air above. Is that somehow not obvious?

The weight of any object is the gravitational force acting on that object. The thing that it acts on is literally part of the definition of the weight. How can this be unclear?

What do you think weight is?
If I hold a heavy sack on my head won't I feel that something is pushing me down? That feeling of pushing down is because I'm barring the sack from falling due gravity and hence applying a force equal and against the gravity.
 
  • #15
DrStupid said:
OK, the air exerts a downward force. According to the 3rd law there must be a corresponding counterforce, acting upward on the Earth and according to the 2nd law the air would be accelerated if this would be the only force acting on it. But in the static case the air doesn't accelerate. Therefore there must be another force acting on the air. Do you agree? If yes, which force is it?
Sir, what I'm saying is: the air which lies above the slab would have it's weight just like our slab has a weight and weight always acts downwards, therefore slab must be bearing the weight of the air above it (just like we bear the weight of something if we hold it over our head).
 
  • #16
Adesh said:
Sir, what I'm saying is: the air which lies above the slab would have it's weight just like our slab has a weight and weight always acts downwards

I just assume that to be the answer to my last question.

Adesh said:
therefore slab must be bearing the weight of the air above it (just like we bear the weight of something if we hold it over our head).

"bearing the weight" means exerting an upward force that compensates the weight. In this case it is the upward force I was talking about in #11. Does that tell you something about the origin of ##P_{above}##?
 
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  • #17
Adesh said:
If I hold a heavy sack on my head won't I feel that something is pushing me down?

Sure. It's the sack pushing on your head. It's a contact force, often called the normal force in elementary physics problems. It's not the weight of the sack (which is a force exerted on the sack by Earth).

That feeling of pushing down is because I'm barring the sack from falling due gravity and hence applying a force equal and against the gravity.

You're applying a force on the sack that's equal and opposite to the force the sack exerts on you (Newton's Third Law). The reason the sack doesn't fall is because the force you exert on it is equal to the force Earth exerts on it (Newton's Second Law).
 
  • #18
Adesh said:
If I hold a heavy sack on my head won't I feel that something is pushing me down? That feeling of pushing down is because I'm barring the sack from falling due gravity and hence applying a force equal and against the gravity.
You are misunderstanding the physics. The feeling of something pushing you down is entirely due to the contact force (pressure) on your head. If you reduce the contact force without changing the weight then the feeling reduces. If you reduce the weight without changing the contact force then the feeling is unchanged.

The feeling is not due to the weight, it is due to the pressure. The weight of the sack acts on the sack, not on me. Only the contact force from the sack acts on me, not it’s weight.
 
  • #19
DrStupid said:
I just assume that to be the answer to my last question.
Means [itex] P_{above} [/itex] is just the weight of the air lying above it, okay. I was thinking that it is the pressure caused due to collision of molecules of air with our sample slab. Thank you. You have explained it in a nice way"bearing the weight" means exerting an upward force that compensates the weight. In this case it is the upward force I was talking about in #11. Does that tell you something about the origin of ##P_{above}##?
 
  • #20
Dale said:
You are misunderstanding the physics. The feeling of something pushing you down is entirely due to the contact force (pressure) on your head. If you reduce the contact force without changing the weight then the feeling reduces. If you reduce the weight without changing the contact force then the feeling is unchanged.

The feeling is not due to the weight, it is due to the pressure. The weight of the sack acts on the sack, not on me. Only the contact force from the sack acts on me, not it’s weight.

Sir, I think due to my mistake of using the word “weight” as the acting force on something is causing the confusion.
I meant by “weight” the force [itex]mg[/itex] which I must provide to something to keep it from falling. So if I’ holding a sack on my head, I need to apply a force equal to its weight and this force is being applied by itself due Newton’s 3rd Law but I have to stay up for 3rd Law to work. Since both forces are acting ( my force and sack’s weight) on different objects therefore I would feel something heavy or being pushed down feeling.
Let me know if my essence of understanding is wrong over here. I have got a great chance to amend it ( if it’s wrong) from great mentors like you. Thank you.
 
  • #21
Adesh said:
I meant by “weight” the force mg which I must provide to something to keep it from falling.
First, that force is the contact force, not the weight. Second, in many situations the contact force will not be equal to mg.

Adesh said:
therefore I would feel something heavy or being pushed down feeling.
Yes, that is the contact force, or in other words the pressure. Any influence that the weight of the upper object might have is transmitted to the lower object through the pressure. Once you have accounted for the contact force (pressure) then you have already accounted for the weight of the upper object.
 
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  • #22
Dale said:
First, that force is the contact force, not the weight. Second, in many situations the contact force will not be equal to mg.

Yes, that is the contact force, or in other words the pressure. Any influence that the weight of the upper object might have is transmitted to the lower object through the pressure. Once you have accounted for the contact force (pressure) then you have already accounted for the weight of the upper object.
What about the pressure caused due to collision of molecules?
 
  • #23
Adesh said:
What about the pressure caused due to collision of molecules?
Can you be more specific with your question?
 
  • #24
Dale said:
Can you be more specific with your question?
There may be two kinds of pressure:-

1. Defined by you as the contact force.

2. Pressure due to collision of molecules with the walls of container that we use in thermodynamics . So the air above the slab must be colliding with our slab and hence may be causing some collisional pressure.
 
  • #25
I think, you already had the right ansatz in #1. Just use the general equation
$$\vec{\nabla} p=-\rho g.$$
We need an equation of state. A good ansatz is the polytrope
$$p=p_0 (\rho/\rho_0)^n,$$
where ##p_0## and ##\rho_0## are the pressure at height ##z=0##. Since the pressure and density change only along ##z##, we have
$$\mathrm{d}_z p=-g \rho_0 (p/p_0)^{1/n}$$
with the solution
$$p(z)=p_0 \left (1-\frac{n-1}{n} \frac{\rho_0}{p_0} g z \right)^{n/(n-1)}.$$
For ##n=1## (isothermal equation of state for an ideal gas) we have
$$\mathrm{d}_z p=-g p \rho_0/p_0$$
and thus
$$p(z)=p_0 \exp \left (-\frac{g \rho_0}{p_0} z \right).$$
On the other hand
$$p_0=\rho_0 k T/m,$$
where ##k## is Boltzmann's constant, ##T## the (absolute) temperature, and ##m## the mass of the gas molecules,
$$p(z)=p_0 \exp \left (-\frac{g m}{k T} z \right).$$
This is the barometric formula for an isothermal atmosphere.
 
  • #26
Adesh said:
There may be two kinds of pressure:-

1. Defined by you as the contact force.

2. Pressure due to collision of molecules with the walls of container that we use in thermodynamics . So the air above the slab must be colliding with our slab and hence may be causing some collisional pressure.
Sure. 1 is the pressure for a solid (your sack/head example), 2 is the pressure for a gas (the OP situation).

What is the question?
 
  • #27
Dale said:
Sure. 1 is the pressure for a solid (your sack/head example), 2 is the pressure for a gas (the OP situation).

What is the question?
Does the weight of air same as the pressure exerted by it? (That collisional pressure)
 
  • #28
Adesh said:
Does the weight of air same as the pressure exerted by it? (That collisional pressure)
What exactly is collisional pressure and how does it differ from just plain old pressure?
 
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  • #29
Adesh said:
Does the weight of air same as the pressure exerted by it?
No, it is not the same. The weight is a gravitational force. The pressure is a “collisional” force as you put it. Even in situations where the magnitude of the forces are the same they are still distinct forces originating from different physical interactions
 
  • #30
Chestermiller said:
What exactly is collisional pressure and how does it differ from just plain old pressure?
Plain old pressure? Sir I haven’t understood your allusion.

Collisional pressure is the pressure caused by fluids, such as on piston or walls of container containing it. So, if we take a slab of air then molecules from above would cause collisional pressure on the slab and the weight of the air above would cause additional pressure. This is the problem, why we didn’t take that pressure from weight into our account.
 
  • #31
Adesh said:
if we take a slab of air then molecules from above would cause collisional pressure on the slab and the weight of the air above would cause additional pressure
This is incorrect. All of the pressure is “collisional”, including whatever pressure might be related to the weight of the gas. There is no additional pressure.
 
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  • #32
Dale said:
This is incorrect. All of the pressure is “collisional”, including whatever pressure might be related to the weight of the gas. There is no additional pressure.
But here you have said that it’s not same
Dale said:
No, it is not the same. The weight is a gravitational force. The pressure is a “collisional” force as you put it. Even in situations where the magnitude of the forces are the same they are still distinct forces originating from different physical interactions
 
  • #33
Yes. The pressure is not the weight. All of the pressure is collisional, all of the weight is gravitational. What is at all unclear here?

I cannot believe that this is confusing. Draw a free body diagram for the slab of air.
 
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  • #34
Dale said:
Yes. The pressure is not the weight. All of the pressure is collisional, all of the weight is gravitational. What is at all unclear here?

I cannot believe that this is confusing. Draw a free body diagram for the slab of air.
Wouldn’t gravity going to attract the air above the slab and since the slab lies below therefore it has to bear that force by which gravity is pulling the air above. So slab must have be having some pressure from below which should balance both collisional pressure and force of gravity of air above.
 
  • #35
Please draw the free body diagram, as requested. Also, label each force and identify:
1) the type of force
2) the object providing the force (I.e. the other object in the third law pair for each force)
 
<h2>1. What is the definition of air pressure?</h2><p>Air pressure is the force exerted by the weight of air molecules in the Earth's atmosphere.</p><h2>2. How does air pressure change with height?</h2><p>The change in air pressure with height is known as the pressure gradient. As altitude increases, the number of air molecules in a given volume decreases, resulting in a decrease in air pressure.</p><h2>3. What is the equation for calculating the change in air pressure with height?</h2><p>The equation for calculating the change in air pressure with height is known as the barometric formula: P = P<sub>0</sub> * e<sup>-Mgh/RT</sup>, where P is the pressure at a given altitude, P<sub>0</sub> is the pressure at sea level, M is the molar mass of air, g is the acceleration due to gravity, h is the height, R is the gas constant, and T is the temperature.</p><h2>4. How does temperature affect the change in air pressure with height?</h2><p>Temperature also plays a role in the change of air pressure with height. As temperature increases, air molecules gain more energy and move faster, resulting in a decrease in air density and a decrease in air pressure with height.</p><h2>5. What are some real-world applications of understanding the change in air pressure with height?</h2><p>Understanding the change in air pressure with height is important in meteorology, aviation, and mountaineering. It can also help predict weather patterns and understand the behavior of gases in different atmospheric conditions.</p>

1. What is the definition of air pressure?

Air pressure is the force exerted by the weight of air molecules in the Earth's atmosphere.

2. How does air pressure change with height?

The change in air pressure with height is known as the pressure gradient. As altitude increases, the number of air molecules in a given volume decreases, resulting in a decrease in air pressure.

3. What is the equation for calculating the change in air pressure with height?

The equation for calculating the change in air pressure with height is known as the barometric formula: P = P0 * e-Mgh/RT, where P is the pressure at a given altitude, P0 is the pressure at sea level, M is the molar mass of air, g is the acceleration due to gravity, h is the height, R is the gas constant, and T is the temperature.

4. How does temperature affect the change in air pressure with height?

Temperature also plays a role in the change of air pressure with height. As temperature increases, air molecules gain more energy and move faster, resulting in a decrease in air density and a decrease in air pressure with height.

5. What are some real-world applications of understanding the change in air pressure with height?

Understanding the change in air pressure with height is important in meteorology, aviation, and mountaineering. It can also help predict weather patterns and understand the behavior of gases in different atmospheric conditions.

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