Thermodynamics final temperature of gas

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SUMMARY

The discussion centers on calculating the final temperature and pressure of oxygen in two thermally insulated vessels after they are connected. The final temperature is determined to be 380 K, while the final pressure is 2.06 x 105 Pa (or 2.04 atm). Two methods are presented: one using conservation of heat (teacher's method) and the other using conservation of total energy (student's method). Both methods yield the same final temperature, demonstrating the equivalence of the approaches despite initial confusion regarding the role of pressure and heat capacity.

PREREQUISITES
  • Understanding of thermodynamics principles, specifically conservation of energy and heat.
  • Familiarity with ideal gas laws and equations, including PV = nRT.
  • Knowledge of heat capacities for diatomic gases, particularly for oxygen (O2).
  • Basic concepts of kinetic theory of gases and internal energy.
NEXT STEPS
  • Study the derivation and application of the ideal gas law, PV = nRT.
  • Learn about heat capacities for different types of gases, focusing on diatomic gases like O2.
  • Explore the principles of conservation of energy in thermodynamic systems.
  • Investigate the kinetic theory of gases and its implications for temperature and pressure relationships.
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Students studying thermodynamics, physics instructors, and anyone involved in understanding gas behavior in insulated systems.

Legendon
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Homework Statement


Two thermally insulated vessels are connected by a narrow tube fitted with a valve that is initially closed. One vessel of volume 16.8 L contains oxygen at a temperature of 300 K and a pressure of 1.75 atm. The other vessel of volume 22.4 L contains oxygen at a temperature of 450 K and a pressure of 2.25 atm. When the valve is opened, the gases in the two vessels mix, and the temperature and pressure become uniform throughout. (a) What is the final temperature? (b) What is the final pressure?
(Ans. (a) 380 K , (b) 2.06 x 105 Pa or 2.04 atm)


Homework Equations





The Attempt at a Solution


The teacher used the method of
heat in=heat out
(m1)c(T-300)=(m2)c(450-T)
and obtain T=380K
I did it by
Total Energy of system is conserved.
For an ideal gas, U=KE
3/2(n1)R300+3/2(n2)R450=3/2(n1+n2)RT
T=380K
Is the method i used correct?
And how come the teachers method is correct? The pressure is different in the vessels. So shouldn't that be taken into account?
 
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well both the final temperature and final pressure of the two systems are the same at the end, which is the time you are calculating for.

you used conservation of energy, and the teacher used conservation of heat. There are two energy components to U (the total internal energy). Those two components are heat, and work. Work is only done if there is change in volume, but in this case the vessels do not grow or shrink. So the change in heat will be equal to the change in total internal energy will be equal to 0 for this case(thermally insulated). This change being 0 allows you to easily relate the final and initial energy values.

EDIT: To be more specific as to why your equations are the same, let me try to put it this way.
He used mass, you used moles. Those have a linear relationship with each other since it is oxygen that's in both tanks. You used R, he used c, both constants that will give the units of energy. Then you used temperature, and he used temperature. So as you can see, both formulas are quite similar.
 
Last edited:
Legendon said:

Homework Statement


Two thermally insulated vessels are connected by a narrow tube fitted with a valve that is initially closed. One vessel of volume 16.8 L contains oxygen at a temperature of 300 K and a pressure of 1.75 atm. The other vessel of volume 22.4 L contains oxygen at a temperature of 450 K and a pressure of 2.25 atm. When the valve is opened, the gases in the two vessels mix, and the temperature and pressure become uniform throughout. (a) What is the final temperature? (b) What is the final pressure?
(Ans. (a) 380 K , (b) 2.06 x 105 Pa or 2.04 atm)

The Attempt at a Solution


The teacher used the method of
heat in=heat out
(m1)c(T-300)=(m2)c(450-T)
and obtain T=380K
I did it by
Total Energy of system is conserved.
For an ideal gas, U=KE
3/2(n1)R300+3/2(n2)R450=3/2(n1+n2)RT
T=380K
Is the method i used correct?
And how come the teachers method is correct? The pressure is different in the vessels. So shouldn't that be taken into account?
Your method is correct but you are using the incorrect heat capacity. O_{2} is a diatomic gas and its heat capacity at constant volume is 5R/2 in this temperature range. But, since heat capacities cancel out it doesn't matter.

Your method is equivalent to your teacher's method. Your teacher is using the heat capacity per unit mass and you are using the molar heat capacity. Since the two gases are the same they all cancel out:

m1c(T-300) = m2c(450-T)
m1cT - m1c(300) = m2c(450) - m2cT
(m1+m2)T = m2(450)+m1(300)

AM
 
I am not using molar heat capacity? on my notes it says Kinetic energy=3/2nRT??. But i am confused with the teacher's method. Is heat dependent on pressure? the teachers method is i see it as putting solution1 of temp1 and solution2 of temp2 together and finding final temp. But with gas of differernt initial pressures, this method still works without considering the pressures ?
 
You're asking a good question. Yes the pressure and the heat are related, which I believe covers the missing link in your understanding. you have constant pressure, constant temperature, constant volume, and constant moles inside the whole system at its final time. You know what all of these values are, therefore you will be able to find the temperature. He didn't need to take into account pressure, just as he didn't take into account Volume because PV = nRT. He has nRT, just in the form of m.c.dT

Your teacher is saying that all of the heat lost by the hotter gas must be gained by the cooler gas. What he is doing is simply calculating the total heat inside the system, and given all of those constant parameters i mentioned in the first paragraph, he can find the final temperature.

His equation is very similar to your equation. It is like this:

(m1)c(T1) + (m2)c(T2) = (m1+m2)c(Tfinal)
 
"He didn't need to take into account pressure, just as he didn't take into account Volume because PV = nRT. He has nRT, just in the form of m.c.dT." Thank you.
 
Legendon said:
I am not using molar heat capacity? on my notes it says Kinetic energy=3/2nRT??. But i am confused with the teacher's method. Is heat dependent on pressure? the teachers method is i see it as putting solution1 of temp1 and solution2 of temp2 together and finding final temp. But with gas of differernt initial pressures, this method still works without considering the pressures ?
I thought you were using 3R/2 as the heat capacity. I see that you were using a kind of principle of conservation of translational kinetic energy. Unfortunately, there is no such principle. So your method will only work if the two gases have the same heat capacity, Cv.

For example, it will not work if one gas is He and the other is O2. The internal energy of He is stored as translational KE. However, O2 stores kinetic energy as rotational as well as translational KE. But only translational KE determines temperature. So for a given change in internal energy there will be a greater change in the temperature of He than of O2.

AM
 
Last edited:
Ok, today the lecturer started on kinetic theory of gasses, i realized jR/2 is the heat capacity. and for oxygen, j=5. Thanks.
 

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