Determining Q for Isobaric Processes: Cp or Cv?

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Homework Help Overview

The discussion revolves around determining the appropriate expression for heat transfer (Q) in isobaric processes, specifically whether to use Q = nCpΔT or Q = nCvΔT + p(Vf - Vi). Participants explore the conditions under which each expression is applicable and the implications of using one over the other.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants discuss the validity of both expressions for calculating heat transfer in isobaric processes and question how to determine which expression to use in different scenarios. There are attempts to clarify the relationship between the heat transfer, internal energy change, and work done in the context of the First Law of Thermodynamics.

Discussion Status

The discussion is ongoing, with participants providing insights and suggestions for clarifying terms and conditions in the examples presented. There is recognition of the need to specify conditions such as constant pressure and the type of gas involved, but no consensus has been reached on the best approach to take.

Contextual Notes

Participants note potential confusion arising from the use of specific terms like "monoatomic" and "insulated," which may imply limitations on the applicability of the discussed relationships. There is also mention of the need for clarity regarding the context of the heat transfer expressions.

songsteel
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Just wanted to ask why is it that for isobaric processes, when we wanted to find Q, sometimes we use Q = nCpΔT and sometimes we use Q = nCvΔT + p(Vf - Vi)?

How do we determine which should be used and when?
 
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songsteel said:
Just wanted to ask why is it that for isobaric processes, when we wanted to find Q, sometimes we use Q = nCpΔT and sometimes we use Q = nCvΔT + p(Vf - Vi)?

How do we determine which should be used and when?

They are not different things .Both of the above expressions are correct and can be used simultaneously , or separately depending on the situation.

For an isobaric process ΔQ = nCPΔT.

From First law of Thermodynamics ΔQ = ΔU+ΔW .

Now ΔU=nCVΔT applies to all kinds of processes involving an ideal gas.

So ,putting values of ΔQ and ΔU ,we have nCPΔT = nCVΔT + pΔVTo elaborate it further-

Case 1) What is the heat required to raise the temperature of 'n' moles of an ideal monoatomic gas by 'ΔT' .

You can simply use Q = nCPΔT

Case 2) How much heat is supplied to 'n' moles of an ideal monoatomic gas in a chamber fitted with a light piston , when the temperature changes by 'ΔT' and volume changes by ΔV ? Consider the process to be isobaric

Here ,use ΔQ = nCVΔT + pΔV

Case 3) What is the change in the volume of 'n' moles of an ideal monoatomic gas in a chamber fitted with a light piston , when the temperature changes by 'ΔT' ? Consider the process to be isobaric .

Now use nCPΔT = nCVΔT + pΔV

Edit:Removed the word - "insulated" and removed a typo
 
Last edited:
Tanya Sharma said:
They are not different things .Both of the above expressions are correct and can be used simultaneously , or separately depending on the situation.

For an isobaric process ΔQ = nCPΔT.

From First law of Thermodynamics ΔQ = ΔU+ΔW .

Now ΔU=nCVΔT applies to all kinds of processes involving an ideal gas.

So ,putting values of ΔQ and ΔU ,we have nCPΔT = nCVΔT + pΔV


To elaborate it further-

Case 1) What is the heat required to raise the temperature of 'n' moles of an ideal monoatomic gas by 'ΔT' .

You can simply use Q = nCPΔT

Case 2) How much heat is supplied to 'n' moles of an ideal monoatomic gas in an insulated chamber fitted with a light piston , when the temperature changes by 'ΔT' and volume changes by ΔU ? Consider the process to be isobaric

Here ,use ΔQ = nCVΔT + pΔV

Case 3) What is the change in the volume of 'n' moles of an ideal monoatomic gas in an insulated chamber fitted with a light piston , when the temperature changes by 'ΔT' ? Consider the process to be isobaric .

Now use nCPΔT = nCVΔT + pΔV
Hi Tanya. You need to "lose" the word insulated from cases 2 and 3. If Q is not equal to zero, the chamber is not insulated. In all three cases, you need to lose the word monoatomic, and in case 1 you need to add the words at "at constant volume". Also, in item 2 there is a typo: replace ΔU with ΔV.

Chet
 
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Hi Chet...

Chestermiller said:
Hi Tanya. You need to "lose" the word insulated from cases 2 and 3. If Q is not equal to zero, the chamber is not insulated.

Yes you are right :redface: .I have edited my post.

Chestermiller said:
In all three cases, you need to lose the word monoatomic,

Why? These are just examples i have taken using monoatomic ideal gas.

Chestermiller said:
and in case 1 you need to add the words at "at constant volume".

Why ? The heat supplied at constant pressure is nCPΔT
 
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Tanya Sharma said:
Hi Chet...

Why? These are just examples i have taken using monoatomic ideal gas.
It might give the impression that the relationship applies only to a monoatomic ideal gas.

Why ? The heat supplied at constant pressure is nCPΔT
Oh, sorry. I misread the Cp as Cv. I think it would be worthwhile adding the words "at constant pressure" to Case 1.

Chet
 
Chestermiller said:
It might give the impression that the relationship applies only to a monoatomic ideal gas.

Well..these are just random questions/cases I formed .But...you may be correct.

Chestermiller said:
Oh, sorry. I misread the Cp as Cv. I think it would be worthwhile adding the words "at constant pressure" to Case 1.

Chet

Right.

Thanks for your valuable suggestions :smile: .I very much like reading your posts .They are full of insight.
 
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