Warm air goes up....reason on a microscopic scale?

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In summary: If you have a large enough number of molecules to have a well defined temperature then you also have a well defined density.
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Wrichik Basu
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I was wondering about the microscopic reason warm air rises up, while cold air comes down. I am aware of the macroscopic reason - density changes. But what happens microscopically? Decrease in density means that the gas molecules are widely spaced out, but their mass remains the same. Then why does warm air go up?
 
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  • #2
Hi,

Microscopically, it's all collisions, collisions and collisions.
Basically 'hotter gas' means 'higher kinetic energy of molecules'.
Faster molecules go further and redistribute kinetic energy in the 'slower' volume.
Faster molecules exert more 'pressure'

All from the kinetic theory of gases, which google to find something you like to study from :smile:

(PS I do hope some real expert like @Chestermiller puts me right if I claim too much :rolleyes: )
 
  • #3
BvU said:
Faster molecules go further and redistribute kinetic energy in the 'slower' volume
And the slower molecules just come down when displaced from their position?
 
  • #4
You can't have read all this stuff in the link yet ? A bit heftier is e.g. this pdf. But a textbook might be more suitable.

'just come down' doesn't describe it in a conceptually responsible manner. It's probably right statistically, though.

Microscopically, gravity is just a puny effect. But for the huge number of molecules involved it only works in one direction: 'down', so macroscopically it sure counts.
 
  • #5
BvU said:
You can't have read all this stuff in the link yet ? A bit heftier is e.g. this pdf. But a textbook might be more suitable.

'just come down' doesn't describe it in a conceptually responsible manner. It's probably right statistically, though.

Microscopically, gravity is just a puny effect. But for the huge number of molecules involved it only works in one direction: 'down', so macroscopically it sure counts.
I know kinetic theory of gases. I know that the molecular speeds and collisions increase with increase in temperature. I just wanted to know why the increased collisions and velocity pushes the molecules up.
 
  • #6
The density of a hotter gas is lower macroscopically. But you were asking about microscopic effects.
Wrichik Basu said:
I just wanted to know why the increased collisions and velocity pushes the molecules up.
'They need more room' is unsatisfactory, I suppose ?
 
  • #7
Wrichik Basu said:
I was wondering about the microscopic reason warm air rises up, while cold air comes down. I am aware of the macroscopic reason - density changes. But what happens microscopically? Decrease in density means that the gas molecules are widely spaced out, but their mass remains the same. Then why does warm air go up?
The decrease in density is the reason. Temperature is a statistical phenomenon so you need a decent number of molecules. If you have a large enough number of molecules to have a well defined temperature then you also have a well defined density.
 
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  • #8
BvU said:
'They need more room' is unsatisfactory, I suppose ?
It's satisfactory.

What happens to the gas which is cool? It needs less room. That's why it comes down?
 
  • #9
Dale said:
The decrease in density is the reason. Temperature is a statistical phenomenon so you need a decent number of molecules. If you have a large enough number of molecules to have a well defined temperature then you also have a well defined density.
So you're saying that kinetic theory of gases explains change in density, and density, in turn, explains the rising of hot gases, right?
 
  • #10
Hmmm. Might if have something to do with the fact that the pressure at the bottom of a mass of air is higher than at the top? Would the warm air molecules be able to better transfer their kinetic energy to the cooler air molecules near the top than the bottom because of this pressure difference? I assume that the warm mass of air that's rising is not composed of the same air molecules as it rises, but is the result of the net transfer of energy to air molecules progressively higher and higher up.
 
  • #11
Drakkith said:
cooler air molecules
You can't really have hot or cold molecules. A mass with molecules that are, on average, faster, will be hot etc.. Hot and Cold are Macroscopic terms.
I feel that the OP is under a bit of a misapprehension that better understanding things necessarily has to involve a microscopic approach. The statistics of a situation are highly relevant to what happens and the behaviour of an individual part of a system may tell you nothing useful.
 
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  • #12
sophiecentaur said:
You can't really have hot or cold molecules. A mass with molecules that are, on average, faster, will be hot etc.. Hot and Cold are Macroscopic terms.

Sorry, Sophie, but I don't see how my post uses the terms hot and cold (or warmer and cooler) in an incorrect or inaccurate way. I'm still talking about the statistical behavior of large numbers of molecules, a situation where hot and cold apply just fine.
 
  • #13
Wrichik Basu said:
So you're saying that kinetic theory of gases explains change in density, and density, in turn, explains the rising of hot gases, right?
I agree with that, but what I was saying is that the concept of temperature only makes sense with a whole bunch of molecules, and once you have enough molecules to have temperature then you also have enough molecules to have density.
 
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  • #14
Drakkith, I think your intuition about the pressure differential is right. In zero gravity hot air doesn't "move", it only slowly equalizes in temperature.

I suspect the higher average kinetic energy gives the "hot" molecules more opportunity to escape both up and down, whereas the "cold molecules" have less opportunity to do so, feeling gravity more in comparison. This probably results in a sort of "sorting algorithm", where hot molecules slowly percolate up.
 
  • #15
Drakkith said:
Sorry, Sophie, but I don't see how my post uses the terms hot and cold (or warmer and cooler) in an incorrect or inaccurate way. I'm still talking about the statistical behavior of large numbers of molecules, a situation where hot and cold apply just fine.
I don't think I'm being picky to pick on the use of hot or cold as a way to describe a molecule. That was what you appeared to b e doing in your post. Rather than 'hot molecules', you could use "hot gas with mostly faster molecules in it" but it is the gas that's hot and not the molecules
We're in the region of the Maxwell's Demon which is a though experiment in which there is a trap door which let's fast molecules through one way and slow molecules through the other way - thus separating all the 'hot' molecules from all the 'cold' molecules. Thermodynamics doesn't allow that.
I remember a guy describing the three electron beams in an old CRT tube as having red green and blue electrons in them. That was almost allowed into a BBC TV Science programme script until I got agitated about it. Same (not false) dichotomy.
 
  • #16
rumborak said:
This probably results in a sort of "sorting algorithm", where hot molecules slowly percolate up.
But the molecules are likely rather to transfer their momentum to nearby molecules than to move by themselves. Gas conducts heat faster than diffusion of different gases. And conduction works downwards too. This is why I am not happy with trying to deal with the 'small' in statistical processes.
 
  • #17
sophiecentaur said:
I don't think I'm being picky to pick on the use of hot or cold as a way to describe a molecule. That was what you appeared to b e doing in your post.

That's certainly not what I intended.

sophiecentaur said:
Rather than 'hot molecules', you could use "hot gas with mostly faster molecules in it" but it is the gas that's hot and not the molecules

Ah, but the gas is composed of a large number of molecules, so saying "hot molecules" should be synonymous with "hot gas" in this case.

rumborak said:
I suspect the higher average kinetic energy gives the "hot" molecules more opportunity to escape both up and down, whereas the "cold molecules" have less opportunity to do so, feeling gravity more in comparison. This probably results in a sort of "sorting algorithm", where hot molecules slowly percolate up.

I'm not so sure. I'm thinking along the same vein as sophie, in that individual molecules are mostly randomly moving about and it is their net transfer of energy upwards that leads to the hot mass of rising air, not because the original molecules in the warm air are all moving upwards.
 
  • #18
Wrichik Basu said:
I was wondering about the microscopic reason warm air rises up, while cold air comes down. I am aware of the macroscopic reason - density changes. But what happens microscopically?

That's an interesting question and to consider it seriously, you would have to model a microscopic situation.

For starters, suppose we have two containers having the same dimensions In one container, we have one slow moving particle and in the other container a fast moving particle. As the particles move and bounce off the walls of the container, does one spend more time near the top of the container than the other? If the container was tall and the slow moving particle was very slow, it might never bounce up near the top of the container.

For another simplistic situation, consider the case when the slow moving particle does have enough energy to hit the top of the container and bounce off of it. Consider particles that are bouncing straight up and down. As time passes, which of the particles spends more time in (say) the top half of the container? I haven't computed the answer , but it amounts to combining the analysis of two elementary physics problems - i.e. "A ball is shot upward from the ground with initial velocity V0 ..." and "A ball is thrown straight down from a height H with an initial velocity -V1..". (The question isn't which particle spends the greater percentage of its "own" time in the top half of the container, the question is which particle has spent more time in the top half of the container after a long time T has elapsed. )
 
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  • #19
Drakkith said:
I'm not so sure. I'm thinking along the same vein as sophie, in that individual molecules are mostly randomly moving about and it is their net transfer of energy upwards that leads to the hot mass of rising air, not because the original molecules in the warm air are all moving upwards.

What you are describing is heat conduction. However, air actually being a pretty good insulator, it could not account for the often drastic and fast changes.
Nah, hot air rising is likely to be due to convection instead. Even in the atmosphere, that's how wind comes about after all.
 
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  • #20
rumborak said:
What you are describing is heat conduction. However, air actually being a pretty good insulator, it could not account for the often drastic and fast changes.

Hmm. Good point.
 
  • #21
Drakkith said:
saying "hot molecules" should be synonymous with "hot gas"
I think this is the nub of our disagreement. You are implying that the word 'molecules' increases the understanding of the phenomenon. We're in the same neck of the woods as when people want to discuss circuit theory in terms of 'electrons', as if that will help them in any way at all. The microscopic has its place but that place is not everywhere. If I throw a brick at you and I describe its trajectory, would it help in any way at all to discuss the molecules of the brick, rather than using macroscopic Newtonian Physics.
Of course, I realize that you know the basics but I always try to look at these questions from the point of view of someone who doesn't. Your approach to this particular problem could serve to promote the mistaken impression that the microscopic is the only really valid approach. But just look at General Relativity. So far, it has not been reconciled with QM, which is the ultimate in microscopic approaches.
 
  • #22
sophiecentaur said:
You are implying that the word 'molecules' increases the understanding of the phenomenon.

No, I'm just using "hot molecules" in lieu of "molecules of the hot mass of air".

sophiecentaur said:
We're in the same neck of the woods as when people want to discuss circuit theory in terms of 'electrons', as if that will help them in any way at all.

It often does as long as the person asking understands that while you can talk about what the an individual or small number of charges in a wire are doing, the equations and components that are encountered in basic circuit theory are described and formulated in terms of the net behavior of a large number of charges.

sophiecentaur said:
Your approach to this particular problem could serve to promote the mistaken impression that the microscopic is the only really valid approach.

This is silly. The OP literally asked what's going on at the molecular level, so I don't know why you're berating me for some imagined slight against scientific education when all I've done is say "cooler air molecules" instead of whatever you personally prefer. I appreciate your dedication to wanting to teach people the correct terms and avoid inaccuracies and pitfalls, but I can't help but feel as if you're twisting what I've said all the way to the breaking point and blowing it well out of proportion.
 
  • #23
Drakkith said:
This is silly. The OP literally asked what's going on at the molecular level, so I don't know why you're berating me
Sorry. I am 'berating' the idea and not the man. :smile:
I would say that the correct answer is that there is not a one step answer at the molecular level and I think the OP should have been given that message from the start (or at least a massive caveat). The relationship between PV and T can be derived from a particle model as can the density but, once you've got the macroscopic model, surely you stick with it. When a gas departs from Ideal, due to the effect of Van Der Waal's forces, any PVT calculations can still be done. Where is one supposed to stop in the use of microscopic models? Would every physics calculation have to include lower than statistical treatment in order for it to be 'acceptable'? I guess my Engineering background can be blamed for my being prepared to have my scientific life full of black boxes but the onion approach to learning seems to work very well; you only need to peel away another layer when the one you are at starts to let you down.
 
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  • #24
@Drakkith and @sophiecentaur hope that the misunderstanding has been resolved, because it doesn't look good when two esteemed members of PF don't agree over something :smile:

From all the discussions, I've come to this conclusion: I should explain change in density using kinetic theory, and then use density for explaining the rest.

Thanks for the explanations. I've once again received a proper explanation at PF, and thanks to all for that :partytime::partytime:
 
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  • #25
Consider a bunch of microscopic dots, moving in random directions in a box. Consider an imaginary surface cutting the box into a top and bottom half. The dots in the bottom half move faster than the dots in the top half. So, there are more dots that move across the surface from the bottom half to the top half than vice versa.

But, as more bottom dots start to invade the top half, collisions between the bottom and top dots pushes some more top dots into the bottom half.
 
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  • #26
In a gas, if the particles have differing temperatures this can be represented as 'size' since a hotter particle is moving faster it covers more distance over a given time period, so it ends up being a case of the Brazil Nut question, where the larger items come to rest on the top of the smaller particles since they are able to travel down while the larger particle will be constrained this direction. So the larger particles end up self-sorting in the gravity field to have larger (or hotter) particles (atoms or molecules) coming out on top of the smaller/cooler ones.
 
  • #27
Wrichik Basu said:
@Drakkith and @sophiecentaur hope that the misunderstanding has been resolved, because it doesn't look good when two esteemed members of PF don't agree over something :smile:

Hey, I'll be more worried when Sophie starts agreeing with everything I say. Then I'll know he's finally lost his marbles and I don't have any left to spare.:-p
 
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  • #28
Wrichik Basu said:
@Drakkith and @sophiecentaur hope that the misunderstanding has been solved, because it doesn't look good when two esteemed members of PF don't agree over something :smile:

From all the discussions, I've come to this conclusion: I should explain change in density using kinetic theory, and then use density for explaining the rest.
Thanks for the explanations. I've once again received a proper explanation at PF, and thanks to all for that :partytime::partytime:
No worries - we always kiss and make up in the end. :wink: And we weren't disagreeing about the Physics - just the approach, which is often a matter of preference.

Steelwolf said:
since a hotter particle is moving faster
This idea doesn't allow for collisions and momentum exchange. Which is the "hot" particle after a collision? This just makes my point again, that particles are just fast or slow. Why can they be hot or cold when, if you do your homework, you realize that Temperature is a measure of the Average Kinetic Energy of all the particles?
 
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  • #29
Instead of a kinetic approach, I would try with a statistical approach. In general, a particle has a kinetic energy (due to motion) and a potential energy (due to gravitational force acting on the particle). In statistical physics there is an equipartition theorem, which, loosely speaking, says that energy likes to be distributed equally in all forms. So if particle has a lot of kinetic energy (corresponding to high temperature), then it also likes to have a lot of potential energy (and hence likes to go up). The only question is - why do particles like to distribute energy equally? That's because it maximizes entropy. When there is a lot of particles, then there is more phase space available for equidistributed energy than for all energy distributed in one form only.
 
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  • #30
Here is a related problem, inspired by ergodic reasoning in the sense that phase-space average (as in the post above) is replaced by a time average. Suppose that you have two elastic balls A and B, both initially at the same height h from the Earth. Suppose also that both have an initial velocity directed towards the Earth, but that the ball A has a larger initial speed than the ball B. Thus they have equal initial potential energies but unequal initial kinetic energies. When the balls hit the Earth, they will elastically recoil and then go up. After a while they will again start to fall down, and so on. So each of the balls will exhibit a periodic motion up and down. However, if you compute the average position of each ball over time, the average height of the faster ball A will be higher than the average height of the slower ball B.
 
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  • #31
Wrichik Basu said:
I was wondering about the microscopic reason warm air rises up, while cold air comes down. I am aware of the macroscopic reason - density changes. But what happens microscopically? Decrease in density means that the gas molecules are widely spaced out, but their mass remains the same. Then why does warm air go up?

Let's try this as a thought experiment. (Mostly because I'm in the middle of two tasks at work.)

Start with a mass of air in an enclosed space at extremely low temperature.

Gravity is going to be exerting a force that pulls the molecules to the bottom of the space.

If you look at collisions as a statistical phenomenon, there is greater number of molecules below (higher density), at the bottom, to run into than there is above, at the top.

As you increase the temperature of the air, the energetic molecules move farther up in the air column due to fewer molecules to collide with. Each molecule travels farther before colliding with another molecule if it goes up than it would if it went down. i.e. the warm air 'rises".
 
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  • #32
If you have a mass of hot air surrounded by cool air, on earth, the cool air above will have lower density than that below. Which means the molecules are more widely spaced, so that the faster molecules of the hot gas will tend to travel further upwards before they have a collision than if they were traveling into the denser air below. The molecules of the hot gas will tend to diffuse out in all directions, but most quickly in the direction of furthest travel / least density. Also, the temporary drop in density where a fast molecule invades and knocks away a molecule of cool gas will be restored to equilibrium more quickly where there is more pressure - i.e. at the bottom - so the base of the warm air does not move as easily down as the top moves up.

So the mass of hot gas should get more diffuse while tending to rise.

For an intuitive explanation, does that work?
 
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  • #33
I think of this as still being a buoyancy issue. For the same reason that a hot air balloon rises, the colder air has higher pressure than the hotter air at the same altitude. In my opinion, the density difference is a factor at the molecular level. Due to the higher density of the colder air, the collisions of molecules between cold and hot air over time involve collisions and energy exchange with a greater number of cold air molecules and fewer number of hot air molecules, so the average effect per molecule is greater for the less dense hot air molecules than the more dense cold air molecules. The end result is a net upwards force that at the macroscopic level is buoyancy.
 
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  • #34
It is buoyancy, there is no doubt about that, but I am not convinced that explanation in terms of buoyancy is a fully microscopic explanation.

From my two posts above the following very simple microscopic explanation can be extracted. When particle goes up it increases it's potential energy at the expense of it's kinetic energy. The more kinetic energy particle has, the more of this energy it can spend to increase it's potential energy.

However, to explain the effect, the energy conservation is not enough. In order for all fast particles go up they must all have a momentum directed upwards, which seems incompatible with momentum conservation if initially those particles had momenta in different directions. That's why the environment particles with lower kinetic energy are needed, by moving in the downward direction and thus saving the total momentum conservation. That's how buoyancy emerges from a microscopic point of view, in terms of momentum and energy conservation of particles.

The picture above is particularly compelling in general relativity, where energy and momentum conservation of fluid in the gravitational field are both encoded in a single equation ##\nabla_{\mu}T^{\mu\nu}=0##. See e.g. S. Weinberg, Gravitation and Cosmology, Eq. (5.4.5) derived from (5.4.3).
 
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  • #35
If we assume we're talking about (say) normal ground level air pressure, is the free path of a gas molecule long enough for the argument about potential/kinetic energy to be significant? I would have thought an upward moving fast gas molecule would collide with another molecule long before there would be any significant gain in potential energy? I know it is from Wikipedia, but here (https://en.wikipedia.org/wiki/Mean_free_path) it suggests a mean free path in the tens of nanometres.

Does that explanation about potential/kinetic energy exchange really account for rising warm air? Does the huge number of molecules involved mean that even this tiny effect becomes significant? I guess it needs some maths?

Edit : Apologies - Only the first two paragraphs of the previous post showed on my browser at first - I have since seen the whole of that post, and see that my comments were not so relevant !
 
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