Explaining How Air Weighs in an Evacuated Flask

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The discussion centers on understanding why an evacuated flask weighs less than when it contains air, with the initial weight being 350g and increasing to 356.3g due to the weight of the air. Participants clarify that the added weight is due to air pressure exerting force on the bottom of the flask, which balances the upward force from the air inside. They emphasize that the air molecules, while moving and not directly touching the flask, still exert pressure that contributes to the overall weight. The conversation also touches on buoyancy and how different gases affect weight, particularly in the context of balloons filled with helium, hydrogen, or a vacuum. Ultimately, the principles of pressure and buoyancy are key to understanding the weight differences observed.
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Hi guys, i was hoping to get an explanation for something that is bugging me. QUESTION - An evacuated flask weighs 350g and with air present it weighs 356.3g ... now i understand that the weight will increase due to the fact that air weighs something, but the part that confuses me is if we consider the fact that the particles are moving around inside te flask and not touching the flask.
What would be a good way of explaining this ?? I am thinking along the lines of the flask weight is the sum of the flask + contents ... but its far from an ellegant explanation.
Thanks
Jayse
 
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You have to be kidding,right...?Is there any sign that the air molecules (mainly N_{2} and O_{2}) could pass through the amorphous structure of glass,so that the "mass conservation" would not be possible...?

Daniel.
 
Hey, I am not sure if i explained the problem to well...
The flask does weigh more (its not a shock ... i hope :S) but the way i intially thought of a solution was to consider the gas to be solid or liquid and imagine the constituents of air neatly sat at the bottom of the flask. But the problem states that the air moves does not touch the flask (or if it does we can assume that the collisions with each dA (unit area) of the flask will be equally balanced with a pressure force in the opposite direction. Its got me all muddled!
 
The air molecules inside are still being pulled by gravity, the pressure on the bottom of the flask is responsible for the added weight, as the particles are getting pulled down (I believe).
 
Yeh that makes sense, like atomospheric pressure pushing on us ... on the side what would be the difference between a sealed box filled with a balloon ... and the same scenario but this time the balloon is attached to a weight which is being suspended.
Would the second box weigh more ... and will it weigh box + balloon + weight ?
 
Jayse_83 said:
Hi guys, i was hoping to get an explanation for something that is bugging me. QUESTION - An evacuated flask weighs 350g and with air present it weighs 356.3g ... now i understand that the weight will increase due to the fact that air weighs something, but the part that confuses me is if we consider the fact that the particles are moving around inside te flask and not touching the flask.
What would be a good way of explaining this ?? I am thinking along the lines of the flask weight is the sum of the flask + contents ... but its far from an ellegant explanation.
Thanks
Jayse
I don't understand how the particles can move around inside the glass without touching it. There must be some physical mechanism, even if it's indirect (such as a second container). If there isn't any transfer of force from air (ultimately) to glass, then, yes the air would effectively be weightless!(which won't happen)
 
In reality the molecules of gas do collide with the sides of the flask. But this is not the reason the flask weighs more. Were it collisions with the sides of the container causing the added mass then the mass would be temperature dependent. This is not the case (lets leave relativity out of this!)

It is not so clear to me that you can ignore what is happening on the BOTTOM of the container. Suppose that we where to suspend (meaning that it is externally supported by something other then the outter flask) a flask full of air inside of larger evacuated flask. would the weight of the suspended flask contribute to the weight of the outer?

Unless the outer flask is some how supporting the inner the answer must be no.
 
I think a better way to think about this is to say that air is actually pushing "up" on the evacuated flask. Let's look at the equation of hydrostatic equilibrium:

\frac{dP}{dr}=-\rho g

If g is assumed to be roughly constant, this can be simplified to the Physics 101 equation:

\Delta P=-\rho g \Delta r

Now, for simplicity, let's imagine a cylindrical vial or cup, closed on the top. The particles outside the cup will be pushing down on the lid and up on the base (yes, there's air underneath the cup). The difference between the force pushing up and that pushing down is given by:

\Delta F=-\rho ghA

where A is the area of the lid/base and h is the height of the cup. In other words, there is a net force upwards. Since the sides of the cup are distributed identically in height, there will be no net lateral force from the air outside the cup.

What about inside the cup? Well, if there's air in it, then the internal pressure will push up on the lid and down on the base with the same forces that the outside air is pushing, so it will exactly balance the force given above. In other words, the air won't add to the cup's weight. If the cup is evacuated, however, there will be no pressure from inside the cup to balance the air pressure outside. How does all this relate to the weight of the air? Well, we can rewrite the equation above:

\Delta F = -\rho ghA=-\rho gV=-m_{air}g

where V is the volume of the cup. This is just the "missing" weight of the air that was inside the cup!

So, long story short, if there's no air inside, then the atmosphere will exert a net upward force on the flask/cup/vial. If there is air inside, then its pressure will cancel that of the air outside and you will get only the weight of the solid material. What we've just done is inadvertantly rederived a special case of Archimedes' Principle, which says that a body immersed in a fluid will experience an upward force equal to the weight of the displaced fluid.
 
So to boil it all down: the pressure in a closed container will be very slightly higher at the bottom of the container than at the top and that difference is equal to the weight of the air inside the flask (pressure times surface area, actually).
 
  • #10
here's a related question.

If an inflated balloon is weighed in air, does it weigh more, less, or the same as it weighs when its deflated?
 
  • #11
jdavel said:
If an inflated balloon is weighed in air, does it weigh more, less, or the same as it weighs when its deflated?

If the air inside the balloon is the same as outside, it will weigh approximately the same in either case...though the stretching of the balloon material may complicate things a bit.
 
  • #12
Integral said:
It is not so clear to me that you can ignore what is happening on the BOTTOM of the container. Suppose that we where to suspend (meaning that it is externally supported by something other then the outter flask) a flask full of air inside of larger evacuated flask. would the weight of the suspended flask contribute to the weight of the outer?

Unless the outer flask is some how supporting the inner the answer must be no.

I think you were referring to my post, which was supposed to address this exact concept. The added weight is due to the air pressure on the bottom of the flask.
 
  • #13
jdavel said:
here's a related question.

If an inflated balloon is weighed in air, does it weigh more, less, or the same as it weighs when its deflated?
Well, it depends on what the question is asking, it can weigh more or stay the same: If you mean the weight of the balloon, then it will of course stay the same. If you mean the weight of the balloon and its contents, then it will weigh more, because there is more matter there.
 
  • #14
Mk,

"...then it will weigh more, because there is more matter there."

Careful! If it's full of He there's more matter, but it weighs less. Remember, we're weighing the balloon in air.
 
  • #15
wow! thanks for all the replies, u've cleared that problem up for me :D
 
  • #16
jdavel said:
Careful! If it's full of He there's more matter, but it weighs less. Remember, we're weighing the balloon in air.
Weight is the force exerted upon an object by virtue of its position in a gravitational field. It is equal to the mass of the object multiplied by the magnitude of the gravitational field. The balloon still weighs more, just because it's floating, or even going up doesn't mean it doesn't have weight! Clouds have weight, dust has weight. Though the balloon's apparent weight is ≤0.
 
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  • #17
Mk said:
Weight is the force exerted upon an object by virtue of its position in a gravitational field. It is equal to the mass of the object multiplied by the magnitude of the gravitational field. The balloon still weighs more, just because it's floating, or even going up doesn't mean it doesn't have weight! Clouds have weight, dust has weight. Though the balloon's apparent weight is ≤0.

So an object in free fall isn't weightless? How about an object in orbit around the earth? Aren't astronauts weightless in space?

I think a better definition of weight is what a scale reads when you stand on it!
 
  • #18
The things you describe have ≤0 apparent weight. And your definition is the definition of apparent weight. In space there is microgravity, so they also have apparent weight.
 
  • #19
hey! this was just starting to get interesting! don't stop now!
 
  • #20
lets go back to the balloons... and evualate three senerios...three balloons of equal volume balloon 1 is filled with He2
balloon 2 is filled with H2
balloon 3 is unique and retains the same volume as 1 &2 but holds a perfect
vacuum
all these balloons are at STP what would be the difference in their 'bouancy' or rather their lifting capability?

thanks


frank MR, P
 
  • #21
Spacetiger you seem quite adept at these types of abstracts...in the scenario above if all three balloons were restrained at sea level what would be the rate of acceleration of each balloon and what would be the ceiling of each also assuming the mass of the balloons are equal...I am curious about this relationship ...I know intuitively how the balloons would respond however , mathematically I'm an idiot...also intuitively doesn't help when considering balloon 3 since its' volume will not change through the ascension phase also i find it hard to evaluate its' final velocity since the impeding forces diminish with altitude and it would appear that we have discovered a means of achieving NEO without anything...


.where physics starts and intuition ends


frank MR. P
 
  • #22
MR. P said:
...three senerios...three balloons of equal volume balloon

1 is filled with He2 balloon
2 is filled with H2 balloon
3 is unique and retains the same volume as 1 &2 but holds a perfect vacuum

all these balloons are at STP what would be the difference in their 'bouancy' or rather their lifting capability?

This all boils down to the ideal gas law:

PV=N_mRT

where Nm is the number of molecules in the balloon. I hate that form of it, however, so I'm going to define:

n=\frac{N_mN_A}{V}

where n is the number density and NA is Avogadro's number. So we have:

P=nkT

where k is Boltzmann's constant. Anyway, let's look at this. In the hydrogen and helium balloons, we know that the internal pressure must equal the outside pressure. If it didn't, then the molecules would push on the balloon, making it expand or contract until the pressures were equal. Likewise, we can treat the temperatures as being equal because we'll assume that the gaseous contents were exposed to the external environment and reached thermal equilibrium with it. This means:

n=\frac{P}{kT}

is a constant as well. However, any number of hydrogen or helium molecules has a smaller total mass than the same number of air molecules (mainly diatomic nitrogen). To see this, just look on the periodic table. Atomic hydrogen and helium have masses of about 1 amu and 4 amu, respectively, while nitrogen has a mass of about 14 amu. By Archimedes principle, the buoyancy force is given by:

F=-m_{air}g

where mair is the mass of air that would be in the balloon if it weren't filled with hydrogen or helium. The total weight of the balloon is given by:

F=m_{balloon}g

If we neglect the weight of the elastic balloon material, this gives a total force of

F=(m_x-m_{air})g=-m_{air}(1-\frac{m_x}{m_{air}})g

For the cases you listed:

\frac{m_{He_2}}{m_{air}}\sim\frac{4}{14},\ \frac{m_{H_2}}{m_{air}}\sim\frac{1}{14},\ \frac{m_{vac}}{m_{air}}=0

Thus, the ratios of the upward forces are:

\frac{F_{He_2}}{F_{H_2}}\sim\frac{10}{13},\ \frac{F_{H_2}}{F_{vac}}\sim\frac{13}{14}

This was done on-the-fly and I have no means of checking it, so please let me know if I made any errors.

NOTE: If the balloon were made of an elastic material, it couldn't maintain a vacuum at the same volume (the external pressure would squash it), but the above calculation assumes that it does anyway. For this case, one can instead imagine that the "balloon" is made of a light rigid material.
 
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  • #23
Tiger thank you are a genius!

indeed if volume 3 were an ideal restraint of equal mass as 1& 2 what would be the final velocity of 3.

in real life balloons are allowed to expand until they pop or leak from their confining medium however 3 is still purplexing in that its' density or volume to mass ratio would or should be lower than 1 & 2 but the ascension or acceleration from restraint should be quite powerfull in as much the entirety of the Earth's atmosphere would be acting upon it with a 2500 lb./ft^2 pressure so perhaps it would be easier to evualate assuming a 1 ft^3 volume . evualating this with the above insight is still beyond my ability ...i can ask the question maybe even build the restraint but analyze beyond me ...
thank you tiger that was quick, too...sorry I couldn't come up with something that actually challenged you

humbled

frank mr. p
 
  • #24
MR. P said:
in real life balloons are allowed to expand until they pop or leak from their confining medium however 3 is still purplexing in that its' density or volume to mass ratio would or should be lower than 1 & 2

I would imagine that the primary reasons they sink are

1) The balloon material still adds some weight that is much denser than air.
2) The outside air is leaking in to the balloon, increasing its interior mass.

The above treatment is idealized in the fact that it neglected the weight of the elastic material. A truly weightless balloon filled with air should feel no net force from pressure + gravity. Of course, you would still have wind and such.
 
  • #25
one cubic foot and a mass of one hundredth of a pound. also I can see why 3 ==0 however the real world sees that mass and acts upon it vacuum or not
 
  • #26
wouldn't all three accelerate coming out of the hole?ok let's assume you and I are going heads up in a verticle drags race where the winner gets the prize for reaching the highest altitude and for the rate of getting there for maybe $1,000,000.00. choice of an H2 baloon with a mass = to the vacuum "balloon?' regardless both our masses will be = with ballast or whatever. wouldn't your choice be the vacuum vessel?


humbled
 
  • #27
MR. P said:
wouldn't your choice be the vacuum vessel?

Yes, the point of the last pair of equations was to show the ratios of the different upward forces. It shows that the upward force on hydrogen is greater than that on helium and the upward force on the "vacuum" balloon is greater than that on hydrogen.
 
  • #28
it also shows that the difference is greater between hydrogen and helium than hydrogen hydrogen and a vacuum so from an engineering standpoint it'd be mo pragmatic to design around a hydrogen based system than a vacuum system. correct?
 
  • #29
MR. P said:
it also shows that the difference is greater between hydrogen and helium than hydrogen hydrogen and a vacuum so from an engineering standpoint it'd be mo pragmatic to design around a hydrogen based system than a vacuum system. correct?

Well, an obvious disadvantage of a vacuum "balloon" is that you need the rigid material I mentioned earlier. Without it, the balloon will implode as soon as the air is sucked out of it. From what I've heard, however, gaseous hydrogen is much more expensive and hard to find than gaseous helium, so that would be something else to consider. The combination of the above is probably why you usually only hear about helium balloons. If, for some reason, you need that extra buoyancy from the hydrogen, then maybe it would be worth the money. I don't see why one would need that, though.
 
  • #30
tiger... thank you for your time and analysis the purpose of the H2 is the greater lifting capability over helium and also greater ceiling over helium. Pursuing a vacuum vessel would provide an even greater ceiling than the other two. Actually hydrogen is easily accessible in fact we produce our own we're in the process of developing an electrodeless hydralyzer which promises a greater yield/efficiency over a polarized electrode based process...in fact it appeares to be close to a MHD in that we are getting a pumping action in a supposedly static medium it could also be from differential heating of the sea water when entering and exiting the 'reactor'...thanks again for the exercise

frank MR. P
 
  • #31
If you are dealing with "real" rubber ballons you will find that a He filled balloon will relativly quickly (24hrs) sink, where a balloon made of mylar will float for days or even weeks. He is small enough that it will pass through the pores of a rubber ballloon, thus the loss of buoyancy. A similar balloon filled with H would loose bouancy even faster then He.

There is also the fun part of H, that is its love affair with O2.
 
  • #32
So... if you want a balloon that will stay up forever you get a mylar one and fill it up with krypton! :biggrin:
 
  • #33
ok what volume would a vacuum have to have in order to lift a 200 pound person assuming a weightless container 100 feet above sea level?




frank
 
  • #34
what if this air in the first place in the jar is by some method changed into a macromolecular colloid,should we not be taking the force resulting from the collisions
 
  • #35
MR. P said:
ok what volume would a vacuum have to have in order to lift a 200 pound person assuming a weightless container 100 feet above sea level?

You'd need to displace 200 lbs of air:

V=\frac{W}{g\rho_{air}}

where W is 200 lbs, g is the gravitational accleration, and \rho_{air} is the mass density of air at that height above sea level. It's about 100,000 liters.
 
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  • #36
thanks spacetiger i'll mull that for awhile ,got to go to work now...do you know much about light?




frank
 
  • #37
MR. P said:
thanks spacetiger i'll mull that for awhile

Keep in mind that it was thought of long ago that buoyancy could be used to carry human beings. It's the same principle behind hot air balloons. Why is it the same? Consider the ideal gas law again:

P=nkT

If you fill a balloon with normal air, it will have the same density as its surroundings and not go anywhere. If you heat it, however, then in order to maintain pressure balance with its surroundings, the above equation says that the number density must go down. If the number density is going down, then Archimedes' principle says that there must be a buoyancy force.

I would expect this means of lifting oneself would be much easier than trying to create a controlled vacuum (you'd want to change its density in flight) inside of a solid object.


,got to go to work now...do you know much about light?

A good bit. I am an astronomer, remember? :wink:
 
  • #38
The most important piece of advice [for aspiring physicists] is to keep your sense of wonderment alive - Dr. Michio Kaku

ST I would have thought you would be interested in any means available to view the cosmos from 150,000 feet...think of the discoveries awaiting your eye...or adaptive array..at 150,000 feet that'd be almost like the opportunities that existed for Gallieo...re: your assumption of a rigid structure for isolating a vacuum , good for a quickie evaluation , however the premiss yields myriad opportunities for taming the impractical and the impossible, even more exciting , the ultimate solution for 'bouyancy'
or completing the logic sequence:

question...What is lighter than Helium?
answer...Hydrogen.
question...What is lighter than Hydrogen?
answer...Nothing.
question...What is another way of describing 'nothing'?
answer...A vacuum or the absence of something.
question...Is a vacuum the lightest?
answer...YES!
Therefore , since 'vacuum' is the lightest, then it appears that confining 'vacuum' is merely an 'engineering' problem!

To that end , the premiss does not have to be predicated upon a 'rigid body' confinement mechanism. and when 'on station' maintaining a 'vacuum' in a rareified environment , as exists in the Stratosphere, would be the most energy efficient option of all other possibilities, intuitively.
 
  • #39
somehow that got posted before i could edit it...Anyway ST , that's what has been driving those elementary questions...I have been building/experimenting with 'tensegral' structures and for the last ten or twelve years specifically 'tetrahedrons' or more affectionately 'TETS' and most recently my latest configuration I call my 'TET Offensive'. An extreme volume whose boundries (amorphic) are defined by the mass to be managed. This structure is closely analoguous to a lung or a dendritic neural form. I will be posting pictures on our site as we continue to build/present our different pursuits...

What you have thought or believed to be a lack of focus has always been the denial of BOREDOM and the pursuit of enlightenment...fap

If you can ask the question then you 'beg' the answer...ukn

frank MR. P
 
  • #40
MR. P said:
ST I would have thought you would be interested in any means available to view the cosmos from 150,000 feet...

That's quite a height. Assuming an exponential drop in density with a 7 km scale height, the density there should be less than 1% of its surface value. That means that, in order to get the same buoyancy force, you're going to have to make your volume at least 100 times larger than the above number.
 
  • #41
Indeed, ST, not an insurmountable engineering problem. At CalTech they are investigating 'intelligent' algorythms or optimizing algorythms for 'Chain Linked' 'nanobots'.In the case of an amorphic vacuum confining structure the algorythm would be optimizing for volume to mass emphasizing volume over mass. In all of these cases the barrier 'thickness' is undefined to facilitate optimization of the physical properties of the structural elements. For example..if the physical properties favor compressional strength over tensile strength then the adaptive algorythm would create a structure totally different in appearance from one composed of tensile elements. Arguably, I am inclined to favor a tensile archecture over a compressional form primairly because tensile forms tend to be more delicate/beautiful in my opinion especially for the environments I'm looking toward.
I do appreciate the repartee...

frank
 

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