Which Exerts More Pressure: Heated Air or Water?

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SUMMARY

Heating water to 100°C results in significant pressure changes due to phase transition, while heated air experiences a lesser pressure increase. The pressure in a sealed jar of water can reach approximately 13,900 PSI, which is sufficient to break standard glass jars, while the pressure in a jar of heated air is calculated to be around 18.71 PSI. The calculations utilize the ideal gas law (PV=nRT) for air, while noting that this law does not apply to liquids like water. The presence of headspace and the thermal expansion of the jar material are critical factors influencing the final pressure outcomes.

PREREQUISITES
  • Understanding of the ideal gas law (PV=nRT)
  • Knowledge of phase transitions, specifically boiling points
  • Familiarity with pressure units (PSI, bar)
  • Basic concepts of thermal expansion in materials
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  • Research the effects of thermal expansion on glass containers under pressure
  • Explore calculations for pressure changes in liquids during heating
  • Study the principles of vacuum sealing in canning processes
  • Learn about the properties of water at varying temperatures and pressures
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Xilus
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Lets say you have a jar of water, and a jar of air.
You heat both of them 100C

will either of them explode?

ok just kidding.

which one exerts more pressure, and is hence more likely to explode?

did heating the substance turn heat into force? (force per unit area)
 
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Xilus said:
Lets say you have a jar of water, and a jar of air.
You heat both of them 100C

will either of them explode?

100 C is the boiling point of water, so it's very likely to explode when the water boils into steam. As for the jar of air, it may or may not, depending on the strength of the jar. I wouldn't try it at home, that's for sure.

Xilus said:
did heating the substance turn heat into force? (force per unit area)

No, but it does increase the force on the jar since the molecules are moving about faster.
 
Why not try to work out what the pressure rises would actually be for some sample problems ?
 
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PV=nRT
 
the constant R doesn't work with a liquid like water.
we could calculate the pressure for the air though! that's awesome.
 
Is the jar initially full of water, or is the headspace. If the latter, is there air in the head space, or just water vapor?
 
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No headspace. One Jar broke. but 6 made it!
IMG_0331_compressed.jpg
 

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The effect with a totally full bottle would depend both on the expansion coefficient of the water and the glass of the bottle.
 
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The apples were cooked in boiling water. so they probably absorbed a lot of water. that's why i chose water. of course there is lots of other biomass in the applesauce.
 
  • #10
Xilus said:
The apples were cooked in boiling water. so they probably absorbed a lot of water. that's why i chose water. of course there is lots of other biomass in the applesauce.
How did you determine that there is absolutely no heat space and that you got all the air out when you put the lid on?
 
  • #11
Xilus said:
There was a little air at the top. not much.
How much? The volume of liquid water only increases by about 4% when heated from 20 C to 100 C.
 
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  • #12
I'm guessing that, in this typical canning operation, there actually is a small amount of head space to begin with, and that the liquid in the jar is fairly hot when the lid goes on, rather than being cold. What is the temperature at filling? I would like to estimate the pressure of the jar contents when the temperature is at 100 C? I have done this kind of calculation before when the company I was at was working on the development of plastic soup cans for use by a food manufacturer.
 
  • #13
I have seen canning done by boiling the apples in an open kettle, separately boiling (to sterilize) the jars and lids, then filling the jars hot and immediately putting on the lids. The resulting vacuum sucks down the lids. The sucked down lid shows that everything was done hot, and that you have a vacuum seal.
 
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  • #14
Xilus said:
No headspace. One Jar broke. but 6 made it!
In a home canning operation, one is not supposed to tighten the rings until the jars are removed from the hot water bath. The operating principle is (I assume) based on water evaporating into the head space and displacing the air there. The excess gas should bubble out through the loose seal. As the jars are cooled, the water vapor condenses and the lids are pulled down tightly -- a "vacuum seal".

The head space gives you a nice pressure reduction without a great deal of cooling and associated volume reduction in the liquid contents.
 
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  • #15
It's easy to calculate the pressure with some simplifying assumptions:

Start at 20 deg C, heat to 100 deg C.
Jar and lid are infinitely stiff, and have zero coefficient of thermal expansion.
Zero air in the water, zero air in headspace.

Density of water at 20 deg C and 1 bar is 998.23 kg/m^3.
Density of water at 100 deg C and 950 bar is 997.85.
Density of water at 100 deg C and 1000 bar is 999.70.
Interpolate to 998.23, pressure is 960 bar.
960 bar X 14.5 = 13,900 PSI. This is an upper limit because it does not include thermal expansion of the glass jar, and elastic deformation of the jar and lid, or the effect of air in the head space.

Adding in the effect of thermal expansion of the glass, and the elastic modulus of the glass and lid, will reduce the pressure. But the pressure will still be high enough to break any normal glass jar. Air in a head space is needed to save the jar.
 
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  • #16
i computed 18.71 PSI for the jar of air at 100C
its lower than i expected.
 
  • #17
Xilus said:
i computed 18.71 PSI for the jar of air at 100C
its lower than i expected.
Huh? What are you computing?

Back of the envelope: You are increasing temperature from about 293K to about 373K. Call it an increase of 30 percent. So absolute pressure should increase by about 30 percent. In terms of gauge pressure, that's about 1/3 of an atmosphere. One atmosphere is about 15 PSI. So the gauge pressure should be about 5 PSI.
 

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