Why is Air Colder and Less Dense at Higher Altitudes?

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Air at higher altitudes is colder and less dense due to two main factors: the cooling effect of expansion as air rises and the decrease in atmospheric pressure. While cold air is generally denser than warm air, at high altitudes, the overall density decreases because the number of air molecules per volume is lower. The discussion also highlights that when air expands, it cools, and this cooling can lead to complex interactions with pressure and temperature. An experiment involving a sealed milk carton illustrates that the pressure change from altitude can cause the carton to collapse rather than expand. Understanding these principles involves recognizing the interplay between temperature, pressure, and density in atmospheric physics.
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If cold air is more dense, why is higher altitude air colder and less dense?
 
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Two reasons: space is cold and air cools as it expands(it expands as it rises)
 
Does its heat sink while the air rises?
 
Does the air move up through the heat while the heat stays relatively stationary?
If warm air is thinner than cold air and it expands as it cools, does it somehow re condense?
I'm trying to get my mind around cold dense air versus cold thin air.
So if you took a thin plastic milk carton, (one of the good ones, with the screw on cap) up to a mountain top on a cold day, screwed on the cap and drove down into the valley into a hot day, would the milk carton crush in on itself? or would it expand and maybe pop?
 
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rjjd@att.net said:
So if you took a thin plastic milk carton, (one of the good ones, with the screw on cap) up to a mountain top on a cold day, screwed on the cap and drove down into the valley into a hot day, would the milk carton crush in on itself? or would it expand and maybe pop?

Well, the expansion due to heat will far outstrip the compression due to rise in air pressure, so it will most definitely expand.
 
DaveC426913 said:
Well, the expansion due to heat will far outstrip the compression due to rise in air pressure, so it will most definitely expand.

So, in this case cold air is not more dense than warm air, and therefore, cold air is not necessarily more dense than warm air, but only in some situations.
 
Why do you think cold air is by definition 'more dense'?

Consider a pneumatic tyre just after you have pumped it up.

Is the air inside more or less dense than the surroundings?

And is it hotter or colder than the surroundings?
 
Studiot said:
Why do you think cold air is by definition 'more dense'?

Consider a pneumatic tyre just after you have pumped it up.

Is the air inside more or less dense than the surroundings?

And is it hotter or colder than the surroundings?

I think cold air is more dense than warm air because if I put an empty water bottle in the freezer over night it will crush in on itself. But I don't know if this principal is universal for cold or hot air.
I think your question is a good one. I think I can make a way to get a thermometer inside a can and then pressurize it to see if it changes.

I squirted a blast of air out of a can for cleaning keyboard dust. I noticed that the can got cold. I assume that the can being pressurized must have been endothermic, therefore the release of pressure must be exothermic. Thus, the temperature decrease.
 
Obviously pressure is very important.

At constant pressure air is colder when it is less dense. If you increase the pressure the density of the air will increase (as you are effectively squashing the air into a smaller volume). Consider the case where you increase the pressure on the air, and yet the density remains the same -- in this case something must be fighting against the squeezing tendency due to the increasing pressure, that something is the increase in kinetic energy of the gas particles, that something is an increase in temperature -- the rise in pressure is met with a rise in temperature if density is to be conserved.

So to the OP. What happens to the pressure at higher altitudes? What are the implications for this on the temperature and density of air?
 
  • #10
Aren't pressure and density synonymous? At least when it comes to air?
 
  • #11
rjjd@att.net said:
I squirted a blast of air out of a can for cleaning keyboard dust. I noticed that the can got cold. I assume that the can being pressurized must have been endothermic, therefore the release of pressure must be exothermic. Thus, the temperature decrease.
The cold is from the gases (propellants) in the can.

When the can is held upright and activated, gas flows out through the nozzle. The pressure inside the can therefore drops, and is no longer sufficient to keep the contents as a liquid; so some of the liquid boils, until the equilibrium pressure is re-established. The vaporization of a liquid is endothermic; thus, heat is absorbed, and the can becomes cold.

http://en.wikipedia.org/wiki/Gas_duster#Cooling
 
  • #12
rjjd@att.net said:
Aren't pressure and density synonymous? At least when it comes to air?
No. There is an interplay between pressure, density, and temperature.
 
  • #13
rjjd@att.net said:
Does the air move up through the heat while the heat stays relatively stationary?
Heat is not a thing, separate from the air. The air has a certain amount of heat, which it carries with it as it rises.
If warm air is thinner than cold air and it expands as it cools, does it somehow re condense?
If there is moisture in it, the moisture can condense. That's how a thunderstorm works.
I'm trying to get my mind around cold dense air versus cold thin air.
The atmosphere has a pressure gradient to it, so it gets less dense as you go up. But at any particular altitude, warmer air is less dense than colder air.
So if you took a thin plastic milk carton, (one of the good ones, with the screw on cap) up to a mountain top on a cold day, screwed on the cap and drove down into the valley into a hot day, would the milk carton crush in on itself?
It would collapse.
Aren't pressure and density synonymous? At least when it comes to air?
Not quite, no. At any altitude, any non-rigid volumes of air will have the same pressure, but may have different density.
 
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  • #14
russ_watters said:
rjjd@att.net said:
So if you took a thin plastic milk carton, (one of the good ones, with the screw on cap) up to a mountain top on a cold day, screwed on the cap and drove down into the valley into a hot day, would the milk carton crush in on itself? or would it expand and maybe pop?
It would collapse.

Huh. I thought it would expand but, running some numbers through the formulae, you're right - if we use a tall enough mountain.

Going from Everest to Sea level would triple the pressure, causing the volume of the gas to be reduced to one third.
Going from -20C to 20C is actually going from 253K to 293K, which would only cause an expansion by one seventh.
Net effect is a collapse.
 
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  • #15
I think enough examples have now been provided to demonstrate that what happens in a gas is more complicated that one simple statement will allow. Further what happens also depends upon outside circumstances.

The question of does a gas cool or warm when it expands depends upon how the expansion is generated and whether the gas is confined or free.

So if we heat a gas in hot air balloon, the gas expands into the confines of the balloon, increasing the pressure and temperature whilst reducing the density.

By constrast if we expand a gas from a cylinder of compressed air into the open air, the gas cools as it expands and its pressure and temperature and density reduces.

Mathematically the controlling physics are known as the Gas Laws and the Laws of Thermodynamics.

go well
 
  • #16
DaveC426913 said:
Huh. I thought it would expand but, running some numbers through the formulae, you're right - if we use a tall enough mountain.

Going from Everest to Sea level would triple the pressure, causing the volume of the gas to be reduced to one third.
Going from -20C to 20C is actually going from 253K to 293K, which would only cause an expansion by one seventh.
Net effect is a collapse.
Actually, I read too fast and didn't see the cold mountain part, but thanks for bailing me out! :biggrin:

Regardless, yes, atmospheric pressure drops very quickly as you go up in altitude.
 
  • #17
DaveC426913 said:
Huh. I thought it would expand but, running some numbers through the formulae, you're right - if we use a tall enough mountain.

Going from Everest to Sea level would triple the pressure, causing the volume of the gas to be reduced to one third.
Going from -20C to 20C is actually going from 253K to 293K, which would only cause an expansion by one seventh.
Net effect is a collapse.

I confirm this as I have inadvertently done this experiment in reverse. Buy a packet of crisps at sea level. Drive up a thousand metres or so and look at your crisp packet. In my experience the crisp packet has expanded.
 
  • #18
rjjd@att.net said:
If cold air is more dense, why is higher altitude air colder and less dense?

In atmospheric physics, there are two kinds of density.

One is mass density, that is, kilograms per cubic meter. The mass density of a volume of air depends upon its composition, its temperature, and its pressure. Colder humid air is less dense than slightly warmer dry air at the same pressure, because the mass of a vapor molecule is less than the mass of a dry air molecule. However, air at high elevations is less dense than air at lower elevations because the number density is less.

The second density is number density, that is the number of molecules per cubic meter. The formula follows Avogadro's Law and is n= P/kT. Here n is the number of molecules per cubic meter, P is the pressure in Pascals, k is Boltzman's Constant, and T is the temperature in Kelvins. Obviously, the number density of a parcel of air depends upon both the temperature and the pressure. The number density of high altitude air is less than that of low elevation air at the same temperature because the number density reflects the Maxwell molecular speed distribution for any given temperature. This is a common exercise in discussions of kinetic gas theory and statistical mechanics. That is, showing that the number density reflects the barometric formula.
 
  • #19
billiards said:
I confirm this as I have inadvertently done this experiment in reverse. Buy a packet of crisps at sea level. Drive up a thousand metres or so and look at your crisp packet. In my experience the crisp packet has expanded.
It will though it is not as simple as that. You tested pressure change only, did you test temp change? Were your crisps* exposed to below freezing temps a thousand metres up?

*whatever crisps are...
 
  • #20
I think this is a case for the nspcc.

(National Society for the Prevention of Cruelty to Crisps)
 
  • #21
billiards said:
I confirm this as I have inadvertently done this experiment in reverse. Buy a packet of crisps at sea level. Drive up a thousand metres or so and look at your crisp packet. In my experience the crisp packet has expanded.

I've had something of the same experience, but in reverse to yours.

I once bought some juice boxes (big mistake, as those tiny, child-sized straws are really hard for an adult to work with), and, as I live at sea level, I noticed that the boxes looked a little crushed, and, when I stuck the straw into them, they began to drip the juice out in a steady stream within about a minute, before I'd even sucked on the straw. The only explanation I can think of is that the air pressure differential between where it was packed (which I assume must be somewhere near Top-O'-the-Universe, Colorado, or, possibly, the moon!) and where I live must have been great enough to compress the fluid content of the juice box to a certain maximum, with state of compression the puncture of the box by the straw released, allowing the compressed juice to flow into the less-dense humid sea-level air.

And, if anybody wants to argue with my position on the issue of the siphon effect along the lines of that Australian guy's bizarre gravity theory, please start a new thread under "General Physics". (I'll be looking for it, as I occasionally need a sure-thing victory!)
 
  • #22
DaveC426913 said:
It will though it is not as simple as that. You tested pressure change only, did you test temp change? Were your crisps* exposed to below freezing temps a thousand metres up?

*whatever crisps are...

Are you having a giraffe or what? My favourite are prawn cocktail.
 
  • #23
billiards said:
Are you having a giraffe or what? My favourite are prawn cocktail.

I'm presuming some sort of potato chip. But I'm also presuming some sort of nuance to it. Like, instead of potato, it's made out of vegamite.
 
  • #24
BadBrain said:
when I stuck the straw into them, they began to drip the juice out in a steady stream within about a minute, before I'd even sucked on the straw.
I have noticed they do this too. I think it's endemic, not situational.
 
  • #25
So if you took a liter of cold air and counted all the molecules, it would have more than what you would have in a liter of warm air.
If you then compressed each of them into 500 ml you would double the atmospheric pressure. Right?
If you compressed them again into 250 ml, you would double them again. Right?
Because the cold air has more mass, doesn't the atmospheric pressure exponentiate at a different rate than the warm air? Double is double. Right?

If you blow up a balloon on a hot day and carry it into a walk-in cold box it should rise to the ceiling.
But if you carried it in and then popped it the warm air would mix with the cold air before it could rise. Where would the warmth go?

If you hit seven golf balls at seven o'clock with a seven iron the balls will go a certain distance.
If you wait until eight o'clock and hit eight balls with an eight iron they go about the same distance.
That's because the sun comes up, hits the ground and emits radiant heat. This warms the air and the molecules push against each other and the air expands and becomes thinner. Thus, less resistance on the golf balls.
assuming you didn't get tired.

Sorry I went away. I went to PF jail until I got a new nickname.
I don't like it. I want to change it. I hope I can.
But if they don't let me I'll have another constant reminder of indiscretions past.
 
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  • #26
klimatos said:
In atmospheric physics, there are two kinds of density.

One is mass density, that is, kilograms per cubic meter. The mass density of a volume of air depends upon its composition, its temperature, and its pressure. Colder humid air is less dense than slightly warmer dry air at the same pressure, because the mass of a vapor molecule is less than the mass of a dry air molecule. However, air at high elevations is less dense than air at lower elevations because the number density is less.

The second density is number density, that is the number of molecules per cubic meter. The formula follows Avogadro's Law and is n= P/kT. Here n is the number of molecules per cubic meter, P is the pressure in Pascals, k is Boltzman's Constant, and T is the temperature in Kelvins. Obviously, the number density of a parcel of air depends upon both the temperature and the pressure. The number density of high altitude air is less than that of low elevation air at the same temperature because the number density reflects the Maxwell molecular speed distribution for any given temperature. This is a common exercise in discussions of kinetic gas theory and statistical mechanics. That is, showing that the number density reflects the barometric formula.

Your answer is PERFECT!

But it's a little technical, and can be more easily explained thus:

Near the surface of the Earth (let's say at sea level, which is where I live), the air is squished by the weight of the air above it. We physicists call this squishing "compression". The higher one climbs into the atmosphere, the less air there is above you to compress, or squish, the air around you. With less compression of the air at your higher altitude (say, the top of a 6,000 ft mountain), the easier it is for the molecules with make up the air to spread out lazily (in line with the Second Law of Thermodynamics, better known to laymen as the Law of Entropy). Thus, the air up there, because it is thin, enjoys low density because there's much less air above it to press down upon it. In terms of physics, the air at that altitude needs to resist far less gravitational potential energy trying to become gravitational kinetic than does the air further down, which has so much more air bearing down upon it. This allows the higher-altitude air to easily vent any heat, to which we physicists refer as "Thermal Energy", by just moving a little faster for a little while, until the energy, usually derived from solar radiation, is dissipated via the increased motion of the air molecule.

Now, further down, any piece of air that receives a lot of Thermal Energy from the sun has to expend this energy by increasing the movement of its molecules to an extent that forces these molecules further apart from one another, to the point that they must often infringe upon the portion of the Earth-touching atmosphere which has colder, less energetic air. Thus, hot air at the surface creates space for the more rapid motion of its molecules by pushing cooler air aside, keeping its own density as low as possible to accommodate the greater need for freedom of motion for its high-energy molecules. Another way of saying this is that there are two types of air pressure: air pressure due to the weight of the air above the air mass you're standing in, which might be called "Gravitational Air Pressure", or "High-Density Air Pressure", and air pressure due to the average kinetic energy of the molecules (which is the real meaning of the word "temperature") which make up the air mass you're in, which might be called "Thermal Air Pressure", or "Low Density Air Pressure".

Now, as hot air always rises (because it just HAS to squeeze itself out the confines of the higher-density cooler air), it eventually reaches an altitude at which its thermal energy can be more easily vented, as there are fewer molecules around to interfere with this process. This is something like the way a refrigerator or an air conditioner (these two devices actually being, in principle, the same device) works, by taking hot air with air molecules at at a high level of average kinetic energy and, by compressing this air by means of the exertion of mechanical energy (which means squeezing the hot air by squishing it with a piston driven into a cylinder, with the piston being powered by an electric motor) until the average kinetic energy of the air's molecules is severely reduced, with the result that, when the compression is released, the resulting air is much colder than it was when it entered the cylinder. Where does the heat go? Look at your refrigerator or your air conditioner: it certainly has a radiator in the back, which vents the heat into the atmosphere. And, where does the heat of a rising hot air mass covering a large portion of the surface of the Earth go at it rises to a higher altitude? How about outer space? The possibility exists that outer space might just be larger, and, thus, better able to absorb thermal energy, than your apartment!
 
  • #27
Another way of saying this is that there are two types of air pressure: air pressure due to the weight of the air above the air mass you're standing in, which might be called "Gravitational Air Pressure", or "High-Density Air Pressure", and air pressure due to the average kinetic energy of the molecules

What a pity you have mixed up this reasonable statement with a bunch of misconceptions.

A really, really poor way to attempt to heat a gas is to shine a light on it (solar radiation).
 
  • #28
Studiot said:
What a pity you have mixed up this reasonable statement with a bunch of misconceptions.

A really, really poor way to attempt to heat a gas is to shine a light on it (solar radiation).

Heating a gas by means of light may be inefficient, but are you denying the role of solar radiation in Earth's climate?

Is heat itself not light on the infrared end of the Electromagnetic spectrum?

How do you account for the seasons if not for the oscillating inclination of the Earth relative to the sun?

Do you posit another particle besides the photon as the carrier of the Electromagnetic force?
 
  • #29
The majority of the heating of the Earth's atmosphere comes directly from the surface, both land and sea.

The solar irradiation (apart form a few isolated frequencies) largely passes through the atmosphere and is absorbed by the ground/ocean.
 
  • #30
Studiot said:
The majority of the heating of the Earth's atmosphere comes directly from the surface, both land and sea.

The solar irradiation (apart form a few isolated frequencies) largely passes through the atmosphere and is absorbed by the ground/ocean.

OK, so most of it comes INDIRECTLY from the sun, but the sun is still the ultimate source of most of the heat in the Earth's atmosphere.

Your statement does not make false my claim as originally stated:

"... usually derived from solar radiation."
 
  • #31
Be aware that this is not your only misconception (or slack terminology whatever you wish).

Thus, hot air at the surface creates space for the more rapid motion of its molecules by pushing cooler air aside, keeping its own density as low as possible to accommodate the greater need for freedom of motion for its high-energy molecules.

The atmosphere is bound to Earth by the Earth's gravity.
The pressure energy due to the weight of the air column is due to gravity.
 
  • #32
Studiot said:
Be aware that this is not your only misconception (or slack terminology whatever you wish).



The atmosphere is bound to Earth by the Earth's gravity.
The pressure energy due to the weight of the air column is due to gravity.

That's what I said:

"In terms of physics, the air at that altitude needs to resist far less gravitational potential energy trying to become gravitational kinetic than does the air further down, which has so much more air bearing down upon it"

But gravity is not the sole source of air pressure: heat is another source of air pressure, as is sound (read about the unmanned Apollo 4 mission, which was flown before the installation of the launch complex's sound suppression system).
 
  • #33
BadBrain said:
as is sound (read about the unmanned Apollo 4 mission, which was flown before the installation of the launch complex's sound suppression system).
While that is fascinating, surely you don't suggest that heating due to liftoff of rockets (or any other sounds) affects the climate of our atmosphere...
 
  • #34
DaveC426913 said:
While that is fascinating, surely you don't suggest that heating due to liftoff of rockets (or any other sounds) affects the climate of our atmosphere...

That's NOT what I'm saying!

By sound pressure I am referring to acoustical overpressure, NOT to heating.

And I'm NOT claiming that this has any impact on a planetary scale.

All I'm claiming is that the building in which Walter Cronkite was seated suffered severe shaking and a ceiling collapse during the liftoff, which phenomena he reported on-air.

See:

 
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  • #35
BadBrain said:
That's NOT what I'm saying!

By sound pressure I am referring to acoustical overpressure, NOT to heating.

And I'm NOT claiming that this has any impact on a planetary scale.

All I'm claiming is that the building in which Walter Cronkite was seated suffered severe shaking and a ceiling collapse during the liftoff, which phenomena he reported on-air.

See:



Then why do you bring it up in a discussion about atmospheric pressure, heating and cooling? Seems to be a red herring.
 
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  • #36
DaveC426913 said:
Then why do you bring it up in a discussion about atmospheric pressure, heating and cooling? Seems to be a red herring.

It's not a red herring. I was simply indicating alternative sources of air pressure besides gravity. Hot air is less dense than cold air, yet a hot air cell exerts greater atmospheric pressure than cold air. What causes the difference in pressure? Thermal energy. Likewise, the acoustic overpressure that brought the ceiling down on Walter Cronkite's head was another source of air pressure (albeit highly localized).

By the way, not only was your "rockets heating up the atmosphere" point a red herring, it was also a straw-man argument. You owe me and the PF community an apology.
 
  • #37
BadBrain said:
It's not a red herring. I was simply indicating alternative sources of air pressure besides gravity. Hot air is less dense than cold air, yet a hot air cell exerts greater atmospheric pressure than cold air. What causes the difference in pressure? Thermal energy. Likewise, the acoustic overpressure that brought the ceiling down on Walter Cronkite's head was another source of air pressure (albeit highly localized).

By the way, not only was your "rockets heating up the atmosphere" point a red herring, it was also a straw-man argument. You owe me and the PF community an apology.

:smile: Will the court read back the proceedings please. We are discussing hot and cold air masses, pressure, and sources of energy heating up the atmo, and you actually list rockets as a source - somehow you consider this a fact relevant to the discussion.

That is not a strawman (let alone mine); it is a red herring, and it is 100% yours. I simply called you out on it.

(You do realize that other people are following this, and can read everything you wrote, including post 32...)

How about we just stick to the topic.
 
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  • #38
DaveC426913:

Here, in part relevant to this discussion, is my post # 32, which I am totally aware that everyone can read, and I hope everyone will read.

"But gravity is not the sole source of air pressure: heat is another source of air pressure, as is sound (read about the unmanned Apollo 4 mission, which was flown before the installation of the launch complex's sound suppression system)."

In response to Studiot's post reminding me of gravity's role in gravitational air pressure, I posted this for the purpose of indicating multiple possible sources of air pressure, and I was correct in so stating.

I intended no red herring, simply a discussion of air pressure, which is the topic of this thread.

Your response was thus:

"While that is fascinating, surely you don't suggest that heating due to liftoff of rockets (or any other sounds) affects the climate of our atmosphere... "

This restatement of my position, which imputes to me a declaration that rockets or other sources of acoustical pressure waves contribute to climate change by means of thermal energy, which declaration cannot reasonably be inferred from my own statement, constitutes a fraudulent restatement of my position, for the apparent purpose of facilitating your attack upon my position.

This is the very definition of a straw-man argument, which does, in fact, constitute academic fraud.
 
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  • #39
DaveC426913:

Should you feel that I'm dealing unfairly with you, just press the report button, and let's let the mentors decide.
 
  • #40
Before this gets out of hand, let me point out that the net pressure change due to any wave is precisely zero. Sound wave are no exception.
 
  • #41
Studiot said:
Before this gets out of hand, let me point out that the net pressure change due to any wave is precisely zero. Sound wave are no exception.

You're precisely right! (Hey, I've heard of the sine wave function, too!)

Please remind me of that when Hurricane Irene hits me this Sunday! I'm sure I'll be greatly comforted by that fact ay that time!

YEAH, RIGHT!
 
  • #42
Winds are not sounds, although they can generate sounds; aeolian sounds do not hurt.
 
  • #43
Studiot said:
Winds are not sounds, although they can generate sounds; aeolian sounds do not hurt.

I never claimed that winds necessarily result from acoustic overpressure waves (though you should have been with me when I was living in Greenwich Village and a huge petroleum tank farm in New Jersey blew up!). I have, in fact, referred to phenomena (i.e., the tug-of-war between high-pressure systems and low-pressure systems) which primarily involve thermal energy differentials within the respective air masses.

Winds can blow down trees, and wreck homes, and send storm surges ashore to drown those of us who live at sea level.

You're correct in stating that winds, in themselves, are not sounds: they constitute the transfer of air from high-pressure zones to low-pressure zones in order to restore pressure equilibrium. But, while they're busy restoring isobaric equilibrium, they're also busy destroying my neighborhood and killing my neighbors.

GET IT?
 
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  • #44
BadBrain said:
...they're also busy destroying my neighborhood and killing my neighbors.

GET IT?


Now that is a straw man. :biggrin:

And it is still off-topic.
 
  • #45
In a perhaps forlorn attempt to get back to the original posting question, I should like to offer a clarification to what appears to be a common misconception of many of the posters. That is, when you change the air temperature the pressure changes in response.

This may be true in confined laboratory vessels, but it is not true in the free atmosphere. It is extremely common for atmospheric temperatures to change significantly without any significant change in atmospheric pressures. What happens is that molecular number density (n=P/kT) changes instead.

We must be very careful in applying laboratory gas laws to the free atmosphere. Many such laws only apply under conditions of equilibrium (not found in the free atmosphere) or when one parameter is held constant (not possible in the free atmosphere).
 
  • #46
Studiot said:
The majority of the heating of the Earth's atmosphere comes directly from the surface, both land and sea.

The solar irradiation (apart form a few isolated frequencies) largely passes through the atmosphere and is absorbed by the ground/ocean.

The ultimate source of the atmosphere's heat is from solar radiation. The proximate source (according the Kiehl & Trenberth's widely cited 1997 study on the atmosphere's heat budget) is 15% from the Sun and 85% from the Earth's surface. This is why the higher you go the colder it gets.
 
  • #47
So if I drop an unopened can of beer and it doesn't explode, I notice the pressure on the can has increased. Avdgrado...(the French guy) states that the contents have not changed. While I put energy into the beer via dropping it therefore energy is not matter; or at least it does not exist independently of itself.
 
  • #48
Inquiziot said:
So if I drop an unopened can of beer and it doesn't explode, I notice the pressure on the can has increased. Avdgrado...(the French guy) states that the contents have not changed. While I put energy into the beer via dropping it therefore energy is not matter; or at least it does not exist independently of itself.

Actually, you're referring to Avogadro, who was Italian, not French.

Anyways, by dropping the can of beer onto the floor, you've converted part of the gravitational potential energy contained within the can into kinetic energy, which kinetic energy was converted upon impact with the floor into mechanical energy sufficient to bring some off the beer's CO2 out of solution and convert it to bubbles of gas, which resultant increase in the pressure within the can (due to the increase in the partial pressure of CO2 in gaseous, rather than dissolved, form) reflects an increase in the energy within the contents of the can, without altering its overall chemical constitution (as solution versus gas represents a physical change, rather than a chemical one). The physical change will eventually resolve itself by virtue of the CO2 going back into solution, with the energy from being dropped being released into the ambiance probably via thermal radiation through the can (which should be gas-tight). Some of the kinetic energy might be converted into mechanical energy which dents the can, and/or into thermal energy as the result of friction between the can and the floor.

In any case, Avogadro was primarily interested in partial pressures resulting from material constitution, and a temporary change in pressure due to input of energy from outside the system appears to be beyond his field of interest.

By the way, one of my most prized possessions just so happens to be a sealed soda can with NO SODA INSIDE! (Am I a nerd or what?) It hasn't collapsed yet, but it dents very easily.

Cheers!
 
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  • #49
I believe I owe a fuller explanation of my last post, which doesn't quite satisfy me.

While I claim the can to be gas-tight, the canning process obviously requires the expulsion of whatever air remains within the can after sealing through the seal, which obviously cannot resist the pressure of the air while immersed in boiling water (indeed, it's not supposed to be able to resist that pressure if the canning process is to work correctly). But, intuitively, the pressure increase within the can resulting from the energy input from immersion in boiling water should be far greater than that resulting from being dropped a few feet onto a floor which may well be flexible (OK, so that's another possible partial outlet of the kinetic energy from the fall: conversion into mechanical energy resulting in the movement of the floorboards). Therefor, the can is gas-tight to an extent sufficient for our purposes.

The explanation for the fact that my soda-free soda can hasn't collapsed? Probably the fact that exposure to the heat source during the canning process is limited in time to the extent needed to force the air out of the can and to kill any pathogens that may exist within the can. Therefor, as this process would have been developed under the assumption that the can had, indeed, contained soda, it simply would have been insufficient to drive most of the air from the can. Still, the fact of how easily it dents clearly shows that the air pressure within the can is less than the ambient air pressure.

Hope I helped.
 
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  • #50
billiards said:
No. There is an interplay between pressure, density, and temperature.

So could there be a scenario where there would be high pressure, high density, high temperature and very little air?

Or the reverse; could there be much air (in a small space) with low press,temp, and density?

Or break down the first question separately;
1. Could you have high density with little air?
2. Could you have high pressure with little air?
And probably the most interesting question; Could you have high temprature and little or no air?
-Russell
 
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