Question about the ideal gas law

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SUMMARY

The discussion centers on the ideal gas law, specifically the relationship between pressure, volume, and temperature in gas compression scenarios. Kory questions the apparent contradiction in the equation T=PV/nR, noting that while volume reduction leads to pressure increase, temperature remains constant. Hoot clarifies that the behavior of these variables depends on the process type: isothermal or adiabatic. For adiabatic processes, the temperature increases during compression, governed by the equation T_f/T_i = (V_i/V_f)^(γ-1).

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  • Basic algebra for manipulating equations
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korneld
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Hi,

I have a question about the ideal gas law.

I have been under the impression that if volume goes down then pressure and temperature go up. But, if you look at the equation T=PV/nR, it seems that if volume, say, doubles, pressure will be halved and vice-versa. While that makes sense, it also leaves the temperature constant. Doesn’t that conflict with real life observations?


Thank you,

Kory
 
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It depends on the specific situation.

For example, if you have a cylinder of gas that is at a fixed volume then obviously V can't change. In that case when you double pressure you will double temperature because PV=nRT.
 
Last edited:
Pressure, density (n/V), and temperature are 3 quantities related by the gas law. If you change one of them, you don't know how the other two change; you need more information. So for example, if you slowly compress a gas that's in contact with a heat reservoir, then T=constant and so PV = constant. OTOH, if you do the compression while not allowing heat to escape, it's an adiabatic process, and temperature will increase. It turns out that in that case, PV^\gamma = constant, where gamma is a constant > 1 related to the specific heats.
 
Follow-up question

Thank you for your replies.

Basically, I am looking for the right way to calculate how much the temperature of a body of gas will increase in a cylinder if it’s compressed so much by a piston.

Could you point me in the right direction?

Thanks.
 
Well if you consider the compression to be adiabatic (which it is likely to be in a piston) you can use the following equation;

\frac{T_{f}}{T_{i}} = \left( \frac{V_{i}}{V_{f}} \right)^{\gamma -1} = \left( \frac{P_{f}}{P_{i}} \right)^{\frac{\gamma -1}{\gamma}}

-Hoot
 
korneld said:
if you look at the equation T=PV/nR, it seems that if volume, say, doubles, pressure will be halved and vice-versa. While that makes sense, it also leaves the temperature constant. Doesn’t that conflict with real life observations?

It depends on the situation. If the piston is in equliibrium with a constant-temperature reservoir, and heat can flow rapidly enough between the piston and the reservoir, then the temperature of the gas inside the piston remains constant. This is more likely to be possible if you compress or expand the gas slowly.

On the other hand, if you insulate the piston so as to isolate it thermally from its surroundings, or if you compress/expand the gas rapidly enough that there's not enough time for a significant amount of heat to flow in or out, then you have an adiabatic process described by Hootenanny's equation.
 

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