Volume vs temp vs pressure question

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In a sealed container, increasing temperature does not change the volume, but it increases pressure according to the ideal gas law (PV=nRT). The volume remains constant while the number of gas molecules (N) stays the same, meaning pressure can only increase with temperature. Confusion arises between volume and quantity, as increasing pressure does not imply more molecules but rather greater force exerted by existing molecules. The discussion also touches on the coefficient of expansion for liquids and gases in sealed containers, particularly in relation to hydraulic or vapor pressure. Overall, the principles of gas behavior under varying temperature and pressure conditions are clarified.
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So here is the question:
I have a gas contained in a volume(like a sealed can). If I increase the temperature does the volume stay the same?
If I increase the pressure, does the volume stay the same?

It seems like it would, but I think volume is confused with "quantity", which I can see changing in all of the above circumstances.

Thx for any help
 
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If you have a sealed can(none of the gas can escape) you will not see an increase in volume. I think you acn see why. If you approximate this general gas as an Ideal gas, obeying the equation of state PV=nRT, you see that if you increase the temperature in a constant volume process that the pressure must also increase (by looking at the equation PV=nRT, where V,n,R all constant)
Cheers,
Norm
 
Originally posted by Rusho

It seems like it would, but I think volume is confused with "quantity", which I can see changing in all of the above circumstances.

How is the quantity changing if you've got a sealed can?
 
hmmm.
Well if a person can pack more pressure in, then more molecules are entering, so more "quantity", but the volume is the same. So its more dense?
 
I think you are confused with what is meant by pressure. Pressure is force per unit area (F/A), so increasing the pressure does not mean increasing the number of molecules (n). It means that the force imparted on the surface has increased. You can think of this is each molecule having more momentum so when it bounces off the container, its change in momentum is greater thus making a larger force (per Newton's second law). Does that make more sense (or any at all)?
good luck,
Norm
 
Yes, I understand.
Thx!
 
The "ideal gas law" is PV= NRT.

T is the temperature (in degrees Kelvin), P is the pressure, V is volume, N the number of molecules (or mols depending on how R is taken) and R is "Boltzmann's constant". If you take a "sealed" can (so that no molecules can get in or out) then N stays the same. You can increase pressure, P, by increasing T (heat the can) while V stays constant or by decreasing V (imagine one end of the can as a plunger that can be pushed down into the can) while T remains the same (you will have to push the plunger down slowly, allowing any increase in temperature due to the energy exerted to "bleed off" to the environment around the can.
 
I have an, only peripherally, related question.

Given a container with a gas, assuming a constant internal/external pressure differential, with a hole of a particular diameter/area, what is formula to compute the rate at which the gas exits the hole.

Assume we're talking ideal gas or air and anything else that I haven't given, but are needed.
 
(P1T1)/V1=(P2T2)/V2

Nautica
 
  • #10
temp vs. Pressure

Hi All,

I like some of the answers and the direction that this discussion is headed, but let's add one more varible to the equation, that is needed for liquids in sealed containers:
" Coefficient of Expansion for Liquids and Gases"

Now, with this in mind let's think another variable related to expansion of liquids and gases in a liquid state within a sealed container ,,,, say an aerosol can filled to the top;

Electrons + heat > Coefficent of Expansion > Possible Hydraulic pressure or vapor Pressure
 
  • #11
You are 3 years too late. The ship has left the harbor.

You might want to pay attention to the DATE of the thread and the last post.

Zz.
 
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