Thermodynamics Homework: Ideal Gas Compression and Work Calculation

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Homework Help Overview

The discussion revolves around thermodynamics, specifically focusing on ideal gas behavior during isothermal compression and adiabatic expansion. Participants are exploring various aspects of work done on gases, internal energy changes, and the concept of reversible processes.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the application of equations related to pressure and volume changes in ideal gases, questioning the validity of their methods and results.
  • Some participants express uncertainty about the implications of isothermal processes on internal energy and thermal energy absorption.
  • There is a query regarding the assumptions made about the ratio of heat capacities in adiabatic processes.

Discussion Status

Some guidance has been provided regarding the equations for work done and the relationship between internal energy and temperature for ideal gases. Participants are encouraged to review concepts related to reversible processes and the properties of heat capacities.

Contextual Notes

Participants are navigating through multiple parts of the homework, with specific marks assigned to each question, indicating a structured approach to the problem set. There is an acknowledgment of uncertainty in the application of thermodynamic principles and the need for further clarification on certain topics.

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Homework Statement



i.) An ideal gas occupies a volume of 2.5 dm3 at a pressure of 0.3 MPa. If the gas is compressed isothermally by a constant external pressure, Pext, so that the final volume is 0.5 dm3, what is the smallest value that the external pressure can have? [2 marks]

ii.)How much work has been done on the gas? [4 marks]

iii.) What is the internal energy change in the gas? [1 mark]

iv.)How much thermal energy has been absorbed by the gas? [2 marks]

v.) What is meant by a reversible process involving an ideal gas? Would the work done on the gas in the above problem be greater if the process had been carried out reversibly? [2 marks]

For part i I just used the equation p1v1=p2v2 and came up with the answer 1.5MPa.

For part ii I used the equation p(Vf-Vi) and got the answer W = -0.3 MJ but I'm not sure if I used the right equation, I originally used the equation W = int pdV but my answer came out as 0. I'm just not sure on the whole on this question, really.

As the process was isothermal, am I right in thinking there was no change in the internal energy of the gas. And because of this the answer for part iv is just 0.3MJ?

Not too sure about part v either. I really need to work on this area...

If anyone could point me in the right direction i'd be thrilled, cheers.
 
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DirtyLeeds said:

Homework Statement



i.) An ideal gas occupies a volume of 2.5 dm3 at a pressure of 0.3 MPa. If the gas is compressed isothermally by a constant external pressure, Pext, so that the final volume is 0.5 dm3, what is the smallest value that the external pressure can have? [2 marks]

ii.)How much work has been done on the gas? [4 marks]

iii.) What is the internal energy change in the gas? [1 mark]

iv.)How much thermal energy has been absorbed by the gas? [2 marks]

v.) What is meant by a reversible process involving an ideal gas? Would the work done on the gas in the above problem be greater if the process had been carried out reversibly? [2 marks]

For part i I just used the equation p1v1=p2v2 and came up with the answer 1.5MPa.

For part ii I used the equation p(Vf-Vi) and got the answer W = -0.3 MJ but I'm not sure if I used the right equation, I originally used the equation W = int pdV but my answer came out as 0. I'm just not sure on the whole on this question, really.

As the process was isothermal, am I right in thinking there was no change in the internal energy of the gas. And because of this the answer for part iv is just 0.3MJ?

Part i makes sense. The smallest external pressure you could have would be if it were the case that V2 is the final gas volume ie the gas pressure is now equal to the external pressure, and hence the gas will stop compressing.

For part ii, if P is constant, thenW = \int P\,dV = P \int\,dV = P\Delta Vso there is no difference between the two methods.

For part iii, yes the internal energy of the gas is constant, because for an ideal gas, internal energy depends only on temperature. Therefore, for part iv, as you stated, all the energy injected into the gas as work must escape as heat.

For part v, you need to hit the books and review reversible processes so that you can answer the question.
 
Cheers!

An ideal gas at 0.1 MPa pressure and 298 K expands reversibly and adiabatically from 0.50 dm3 to 1.00 dm3. (For this question, take the molar heat capacity at constant volume to be: CV,m = 12.48 J K-1 mol-1).
Calculate:
(i) its final temperature, [4 marks]

I used the formula Ti/Tf = (Vf/Vi)^x-1 Where x is the ratio of heat capacities, and I assumed that x=1.4, and got the answer 225.84

However, once again I am unsure whether or not I've gone down the right road.
 
DirtyLeeds said:
I used the formula Ti/Tf = (Vf/Vi)^x-1 Where x is the ratio of heat capacities, and I assumed that x=1.4, and got the answer 225.84

However, once again I am unsure whether or not I've gone down the right road.
Why are you assuming that the ratio of heat capacities is 1.4? What is Cp? [Hint: You can determine this from the value of Cv - what is Cp-Cv?].

AM
 

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