Why doesn't a barometer with vacuum get crushed by the atmosphere?

In summary: The test tube is strong enough to withstand pressure because the pressure is distributed evenly over the surface of the test tube. If your weight was concentrated on the much smaller area of the test tube, and the pressure was much higher than atmospheric pressure, then you would break the test tube.
  • #1
tarekatpf
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Why doesn't a mercury barometer containing vacuum get crushed by the atomospheric pressure?

Here is what I think might be the reason.

Although there is vacuum inside a mercury barometer, that vacuum is pressurized by the atmosphere that pushes mercury from the reservoir. That pressure is canceled out by the pressure exerted by the atmosphere from outside onto the barometer tube containing the vacuum.

Did I get it right?

Additional question:

Suppose I take a test-tube that can contain only 700 mm of mercury.

Then, I fill this test-tube up with mercury, and place it in the reservoir.

Now, since the atmosphere from outside is putting pressure on the reservoir at 1 atmospheric pressure, should this pressure make the mercury kept in the reservoir try to rise the level of the mercury inside the test-tube, and having failed to do so, expand the volume of the test-tube or break it apart?
 
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  • #2
tarekatpf said:
Why doesn't a mercury barometer containing vacuum get crushed by the atomospheric pressure?

The shell of the barometer is strong enough to stand up to the force of atmospheric pressure.

If it were made of some more flimsy material, it would be crushed. For example, a thin-walled plastic bottle will collapse if you suck the air out of it but a glass or metal bottle will not.
 
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  • #3
Nugatory said:
The shell of the barometer is strong enough to stand up to the force of atmospheric pressure.

If it were made of some more flimsy material, it would be crushed. For example, a thin-walled plastic bottle will collapse if you suck the air out of it but a glass or metal bottle will not.

Thank you very much. So, glass is pretty strong then.

But I have a question. Isn't the vacuum under pressure by the mercury inside the tube ( which is pushed above by the atmosphere outside? ) Because if it was not, wouldn't then the mercury inside the tube keep falling down util totally emptying the tube?
 
  • #4
You can't put pressure on a vacuum. It's either empty space or it's not a vacuum.

The mercury column doesn't fall down completely because of the atmospheric pressure holding it up, remember? That's why barometers were developed in the first place.
 
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  • #5
SteamKing said:
You can't put pressure on a vacuum. It's either empty space or it's not a vacuum.

The mercury column doesn't fall down completely because of the atmospheric pressure holding it up, remember? That's why barometers were developed in the first place.

Yes, now I think there is no pressure on the vacuum too. Because if there was any pressure, there wouldn't be any static level of vacuum, which would then rise instead.

Thank you very much for your answer.
 
  • #6
I thought the glass isn't strong enough, because I head that there was a scientist ( the inventor of air pump, I think ) who pumped air out of a metal sphere that was made up of two hemispheres joined together. The hemispheres couldn't be separated even with a number of horses trying to pull them apart. I thought, if atmospheric pressure was so much that even a number of horses' strength was relatively weaker, the glass should easily get crushed.
 
  • #7
Turns out a thick layer of glass can be made strong enough to hold it
 
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  • #8
dauto said:
Turns out a thick layer of glass can be made strong enough to hold it

Thank you very much.

It's interesting that although even a brick kept on a glass tube can break it ( I haven't done any experiment though. But even if a brick cannot break the glass tube, I think standing on a test-tube surely will ), 1 atmospheric pressure can not. I heard somewhere that the weight of an elephant is less than 1 atmospheric pressure. So, if weight of a little brick or a person can break the glass, why can't 1 atmospheric pressure?
 
  • #9
If your weight was distributed uniformly over the whole surface of the glass pointing inwards as is the case for the atmospheric pressure, than you wouldn't break the glass either.
 
  • #10
Pressure is force divided by area. Elephants have enormous feet; if they stand on flat ground, the pressure is less than atmospheric pressure. If an elephant stood on a tiny test tube, its weight would be concentrated on the much smaller area of the test tube, and the pressure would be much higher than atmospheric pressure.

A lot of laboratory glassware is strong enough to withstand 1 atmosphere of pressure, so that it can be used in procedures conducted under low pressure. It doesn't actually have to be that thick. You can still break this glassware by dropping it or standing on it, since the resulting pressure is much more than 1 atmosphere.
 
  • #11
I have read through this thread and can't find any reference to the fact that a tube with circular cross section is, inherently, very strong. If you wanted a square section tube, it would need to be made of very much thicker glass.
Also, a tube is much stronger in compression than if you pumped it up to + 1 Atmosphere, internal pressure.
 
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  • #12
Also keep in mind that a cylindrical or spherical chamber is extremely strong against a completely uniform compressive load. The air pressure is uniform - it pushes inwards on all sides equally. If you stand on it however, the force might be smaller, but it is also not uniform. A cylinder is much weaker when loaded on one side than it is when loaded on all sides equally.
 
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  • #13
sophiecentaur said:
Also, a tube is much stronger in compression than if you pumped it up to + 1 Atmosphere, internal pressure.
It does depend on the material though.
 
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  • #14
cjl said:
Also keep in mind that a cylindrical or spherical chamber is extremely strong against a completely uniform compressive load. The air pressure is uniform - it pushes inwards on all sides equally. If you stand on it however, the force might be smaller, but it is also not uniform. A cylinder is much weaker when loaded on one side than it is when loaded on all sides equally.

Thank you very much for your answer. But sorry as I didn't get it. When you try to crush an empty can of pepsi with your hand, isn't it easier if you try to crush the can by pressing on it from all sides?
 
  • #15
sophiecentaur said:
I have read through this thread and can't find any reference to the fact that a tube with circular cross section is, inherently, very strong. If you wanted a square section tube, it would need to be made of very much thicker glass.
Also, a tube is much stronger in compression than if you pumped it up to + 1 Atmosphere, internal pressure.

Thank you very much for your answer.

So the credit goes to the cylindrical-ness of the tube?

I'm sorry as I did not get the part ''Also, a tube is much stronger in compression than if you pumped it up to + 1 Atmosphere, internal pressure.'' Would you please care to explain what you said in layman terms?
 
  • #16
tarekatpf said:
Thank you very much for your answer.

So the credit goes to the cylindrical-ness of the tube?

I'm sorry as I did not get the part ''Also, a tube is much stronger in compression than if you pumped it up to + 1 Atmosphere, internal pressure.'' Would you please care to explain what you said in layman terms?

When a cylindrical tube is subjected to a high external pressure, the forces are all in a direction which compresses the material (strongest mode). When you 'pump up' the internal pressure, the forces are all tending to stretch the material (weaker mode).

Many materials are much stronger when you are pressing against them than when you try to pull them apart. Concrete is a great example of this. A block will withstand many tons of weight on top of it but will crack quite easily on the outside edge if you try to 'bend it'. Pre-stressed concrete beams use steel bars with plates, pulling the ends together, to ensure that, even when used as cantilevers (with overhang), the net forces over all of the the beam are still compressive. Lightweight arches are much better engineering than massive horizontal beams. Try breaking a chicken's egg by pressing it together (longways) between the palms of your hand - it's unbelievably strong.

Re the pepsi can: it's hard to set up an even pressure around the sides of a can but if you take a loop of string and pass it round the sides of a can, then tighten it by twisting round a stick (a tourniquet) and you will find the can is really pretty strong compared with when you just poke it with a finger. There is a party trick in which you can stand on a light drinks can and it will support you (all your weight applied over a very small cross sectional area of metal and the forces are all compressive). Bend down (balancing requires practice) and tap the sides of the can, to form a dimple, and the can collapses because the forces are no longer just compressive but can bend the material.
 
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  • #17
tarekatpf said:
Yes, now I think there is no pressure on the vacuum too. Because if there was any pressure, there wouldn't be any static level of vacuum, which would then rise instead.

Air pressure is essentially caused by the molecules of gas that make up air (Nitrogen, oxygen etc)bouncing off each other and the surface of the vessel.
A true vacuum contains no molecules so can't create a pressure or be pressurised.
 
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  • #18
CWatters said:
Air pressure is essentially caused by the molecules of gas that make up air (Nitrogen, oxygen etc)bouncing off each other and the surface of the vessel.

A true vacuum contains no molecules so can't create a pressure or be pressurised.

Thank you very much. Yes, I was wrong to assume that.
 
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  • #19
sophiecentaur said:
When a cylindrical tube is subjected to a high external pressure, the forces are all in a direction which compresses the material (strongest mode). When you 'pump up' the internal pressure, the forces are all tending to stretch the material (weaker mode).

Many materials are much stronger when you are pressing against them than when you try to pull them apart. Concrete is a great example of this. A block will withstand many tons of weight on top of it but will crack quite easily on the outside edge if you try to 'bend it'. Pre-stressed concrete beams use steel bars with plates, pulling the ends together, to ensure that, even when used as cantilevers (with overhang), the net forces over all of the the beam are still compressive. Lightweight arches are much better engineering than massive horizontal beams. Try breaking a chicken's egg by pressing it together (longways) between the palms of your hand - it's unbelievably strong.

Re the pepsi can: it's hard to set up an even pressure around the sides of a can but if you take a loop of string and pass it round the sides of a can, then tighten it by twisting round a stick (a tourniquet) and you will find the can is really pretty strong compared with when you just poke it with a finger. There is a party trick in which you can stand on a light drinks can and it will support you (all your weight applied over a very small cross sectional area of metal and the forces are all compressive). Bend down (balancing requires practice) and tap the sides of the can, to form a dimple, and the can collapses because the forces are no longer just compressive but can bend the material.

Thank you very much for your explanation.

Though I did not understand what you said about compressive force, concrete beams, arched beams etc, since I am not familiar with these engineering terms; I would love to know the basics required to understand this kind of stuff. Can you suggest me any book in which these are explained in easy language?

I am sorry that I did not understand the procedure ''take a loop of string and pass it round the sides of a can, then tighten it by twisting round a stick (a tourniquet)'', possibly due to my poor ability to form image from words, but I really appreciate your efforts to explain it. Thanks a lot for that.

I will definitely try crushing an egg, and doing that pepsi can trick.

Thank you very much, again.
 
  • #20
tarekatpf said:
Though I did not understand what you said about compressive force, concrete beams, arched beams etc,
Think of a thin plastic pipe. It's easy to break it by bending. But it's difficult to crush it by compressing it from all sides uniformly.
 
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  • #21
A.T. said:
Think of a thin plastic pipe. It's easy to break it by bending. But it's difficult to crush it by compressing it from all sides uniformly.

Thank you very much. That's an excellent example. Can a brick be an example of an object that's difficult to break by bending, but easy by crushing?

I wonder why a ''cylindrical or spherical chamber is extremely strong against a completely uniform compressive load'' as cjl and said. Is it possible for me to understand despite having almost zero knowledge about the principles of physics?
 
  • #22
It's possible to engineer submersibles that can withstand many atmospheres of pressure.

"On 23 January 1960, the Swiss-designed bathyscaphe Trieste, originally built in Italy and acquired by the U.S. Navy, descended to the ocean floor in the trench manned by Jacques Piccard (who co-designed the submersible along with his father, Auguste Piccard) and USN Lieutenant Don Walsh. Their crew compartment was inside a spherical pressure vessel, which was a heavy-duty replacement (of the Italian original) built by Krupp Steel Works of Essen, Germany. Their descent took almost five hours and the two men spent barely twenty minutes on the ocean floor before undertaking the three-hour-and-fifteen-minute ascent. Their early departure from the ocean floor was due to their concern over a crack in the outer window caused by the temperature differences during their descent.[23] The measured depth at the bottom was measured with a manometer at 10,916 m (35,814 ft) ±5 m (16 ft).[11][24]"

Wikipedia: "Challenger Deep"

Allowing 10 meters of water for each atmosphere of pressure (atm), this craft withstood almost 1100 atm. The decent was into the Mariana Trench on the floor of the western Pacific Ocean.
 
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  • #23
tarekatpf said:
Can a brick be an example of an object that's difficult to break by bending, but easy by crushing?
No. It's easier to break a brick by bending, than by pressing uniformly from all sides.

tarekatpf said:
I wonder why a ''cylindrical or spherical chamber is extremely strong against a completely uniform compressive load'' as cjl and said. Is it possible for me to understand despite having almost zero knowledge about the principles of physics?
You can ask yourself: Where would the uniform pressure create the first dent in a round wall? Since the shape is symmetrical, it has the same stability at each point. It doesn't have weak points. The internal compressive stresses are also distributed uniformly.

A cube box on the other hand, will have strong bending moments at the edges due to the forces on the sides. Non uniform curvature creates non uniform loading, that concentrates in some areas where the material gives in first.
 
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  • #24
tarekatpf said:
Thank you very much. That's an excellent example. Can a brick be an example of an object that's difficult to break by bending, but easy by crushing?

I wonder why a ''cylindrical or spherical chamber is extremely strong against a completely uniform compressive load'' as cjl and said. Is it possible for me to understand despite having almost zero knowledge about the principles of physics?

Quite the reverse. Brick arches can take enormous loads even when made of really sub-standard bricks, which you can almost break apart with your hands by pulling and bending. Read what I wrote about pre-stressed concrete.

Consider a dry stone wall, as an extreme example. You can just lift of the stones but they will support tons and tons.
 
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  • #25
Since the shape is symmetrical, it has the same stability at each point. It doesn't have weak points.
Non uniform curvature creates non uniform loading, that concentrates in some areas where the material gives in first.

So whether a thing would break under uniformly distributed compressive force depends on its shape, regardless of what material it is composed of. Did I get it right?

Could you please tell me how can I predict where the weak points are from knowing shape of an object? Such as, we do know that a spherical object has no weak point on its surface. But we know it from our experience. But what's the intrinsic property of that object that has made it like that? And what is intrinsic about a cubic object that has made it weaker at its edges?
 
  • #26
sophiecentaur said:
Quite the reverse. Brick arches can take enormous loads even when made of really sub-standard bricks, which you can almost break apart with your hands by pulling and bending. Read what I wrote about pre-stressed concrete.

Consider a dry stone wall, as an extreme example. You can just lift of the stones but they will support tons and tons.

But what could be an example of an object that is easier to break by crushing and difficult to break by bending?
 
  • #27
tarekatpf said:
So whether a thing would break under uniformly distributed compressive force depends on its shape, regardless of what material it is composed of. Did I get it right?

Could you please tell me how can I predict where the weak points are from knowing shape of an object? Such as, we do know that a spherical object has no weak point on its surface. But we know it from our experience. But what's the intrinsic property of that object that has made it like that? And what is intrinsic about a cubic object that has made it weaker at its edges?
You may be looking for an over-simple answer. Materials science and structural engineering design are very complex subjects.
 
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  • #28
tarekatpf said:
So whether a thing would break under uniformly distributed compressive force depends on its shape, regardless of what material it is composed of. Did I get it right?
No. Every material will be crushed if the pressure is large enough, even if you distribute the load uniformly (which is not possible in the imperfect real world anyway). And different materials will be crushed at different pressures.

tarekatpf said:
Could you please tell me how can I predict where the weak points are from knowing shape of an object? Such as, we do know that a spherical object has no weak point on its surface. But we know it from our experience.
It's not experience, but the symmetry of a sphere that makes all points on it equivalent, so there are no areas weaker than others.

tarekatpf said:
But what's the intrinsic property of that object that has made it like that? And what is intrinsic about a cubic object that has made it weaker at its edges?

There is no simple general property. Problems like this are investigated numerically.
http://en.wikipedia.org/wiki/Finite_element_method
 
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  • #29
Is it possible to show mathematically that the edges of a cubic block is weaker?
 
  • #30
tarekatpf said:
Is it possible to show mathematically that the edges of a cubic block is weaker?

Yes. There are good mathematical models of materials and structures but, from what you say about your technical knowledge, you may find them hard to follow. Perhaps, if you googled terms like ' strength of a beam' you could see if you find the maths in that example accessible.
This is non-trivial stuff and needs to be approached from basic principles and not jumped into, half way through.
 
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  • #31
Atmospheric pressure exerts a 14.7 pounds per square inch at sea level. Making 1 sq inch of glass withstand 14.7 pounds isn't very hard (Or 1/4 inch per side = less than 1 lb)

Say you have 2 shallow cylinders of 1 foot diameter = 113 square inches with a vacuum between them. That means it will take 113x14.7 = 1661 lbs to separate them.
 
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  • #32
sophiecentaur said:
Yes. There are good mathematical models of materials and structures but, from what you say about your technical knowledge, you may find them hard to follow. Perhaps, if you googled terms like ' strength of a beam' you could see if you find the maths in that example accessible.
This is non-trivial stuff and needs to be approached from basic principles and not jumped into, half way through.

Thank you very much for your suggestions.
 
  • #33
meBigGuy said:
Atmospheric pressure exerts a 14.7 pounds per square inch at sea level. Making 1 sq inch of glass withstand 14.7 pounds isn't very hard (Or 1/4 inch per side = less than 1 lb)

Say you have 2 shallow cylinders of 1 foot diameter = 113 square inches with a vacuum between them. That means it will take 113x14.7 = 1661 lbs to separate them.

Thank you very much. That was an excellent use of mathematics.
 

1. Why doesn't a barometer with vacuum get crushed by the atmosphere?

A barometer with a vacuum does not get crushed by the atmosphere because the air pressure inside the barometer is equal to the air pressure outside. The vacuum inside the barometer creates a balance between the atmospheric pressure pushing down and the lack of pressure pushing up.

2. How does a barometer with vacuum measure atmospheric pressure?

A barometer with a vacuum measures atmospheric pressure by utilizing the principle of balancing forces. The vacuum inside the barometer creates a balance between the atmospheric pressure pushing down and the lack of pressure pushing up. This balance is then measured and displayed on the barometer.

3. Can a barometer with vacuum be used to measure altitude?

No, a barometer with a vacuum is not an accurate tool for measuring altitude. While it can measure changes in atmospheric pressure, it cannot accurately determine the exact altitude because there are other factors that can affect atmospheric pressure, such as weather conditions.

4. Why is a barometer with vacuum more accurate than a regular barometer?

A barometer with a vacuum is more accurate than a regular barometer because it eliminates the potential for the air trapped inside the barometer to affect the measurement. The vacuum inside the barometer creates a perfect balance between the atmospheric pressure pushing down and the lack of pressure pushing up, resulting in a more precise measurement.

5. How does a barometer with vacuum work?

A barometer with a vacuum works by utilizing the principle of balancing forces. The vacuum inside the barometer creates a balance between the atmospheric pressure pushing down and the lack of pressure pushing up. This balance is then measured and displayed on the barometer, providing an accurate measurement of atmospheric pressure.

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