Work and Volume in Adiabatic Expansion

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Discussion Overview

The discussion revolves around a homework problem involving the adiabatic compression of a gas, specifically 1.60 mol of H2, where participants are tasked with calculating the final volume and work associated with the process. The conversation includes attempts to apply relevant thermodynamic equations and principles, with a focus on the first law of thermodynamics and the characteristics of adiabatic processes.

Discussion Character

  • Homework-related
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant attempts to calculate the initial volume using the ideal gas law but expresses uncertainty about the correctness of their approach.
  • Another participant questions whether the process is isothermal or adiabatic, confirming it is adiabatic.
  • There is a discussion about the validity of the equation p1v1=p2v2 for adiabatic processes, with participants expressing doubt about its correctness.
  • Participants discuss the first law of thermodynamics and its application to adiabatic processes, with one suggesting that energy equals work in this context.
  • There is an attempt to derive equations involving differentials and the relationship between pressure, volume, and temperature, with some participants expressing confusion about the integration process.
  • One participant expresses concern about their understanding of calculus in relation to the problem, indicating a struggle with the mathematical aspects of the derivation.

Areas of Agreement / Disagreement

Participants generally agree that the process is adiabatic, but there is disagreement regarding the correct equations to use and the proper application of the first law of thermodynamics. The discussion remains unresolved as participants continue to explore different approaches and clarify their understanding.

Contextual Notes

There are limitations in the integration steps presented, and participants have not reached a consensus on the correct equations or methods to apply in this scenario. The discussion reflects various assumptions and uncertainties regarding the mathematical treatment of the problem.

ScreamingIntoTheVoid

Homework Statement


A sample of 1.60 mol H2 (Cv = 20.5 J K-1 mol-1) at 21°C and 1.50 atm undergoes a reversible adiabatic compression until the final pressure is 4.50 atm. Calculate the final volume of the gas sample and the work associated with this process. Assume that the gas behaves ideally.

Homework Equations


pv=nRT
p1v1=p2v2
ΔE=-peternalv=nCvΔT

The Attempt at a Solution


pv=nRT → (1.5 atm)(V0=(1.6 mol)(0.08206 atm mol K)(294 K)
V0=25.734016 L (tried this initially as I was given Cv, but that was wrong)
P1V1=P2V2→(1.5 atm)(25.734016 L)=(4.5 atm)(V) →8.57800533 L (which was wrong)

ΔE=-(4.5)(17.1501067)= -77.202 J (nope)
ΔE=(1.6 mol)(20.5 K mol)(294 K)= 9643.2 J (Nope)

I'm not really sure where I went wrong with this, any input would be really helpful
 
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Is the process isothermal, or is it adiabatic?
 
Chestermiller said:
Is the process isothermal, or is it adiabatic?
Adiabatic
 
ScreamingIntoTheVoid said:
Adiabatic
For an adiabatic reversible process, is this equation correct: p1v1=p2v2 ?
 
Chestermiller said:
For an adiabatic reversible process, is this equation correct: p1v1=p2v2 ?
That's what I wrote in my notes at least. I suppose not though?
 
ScreamingIntoTheVoid said:
That's what I wrote in my notes at least. I suppose not though?
You suppose correctly. Do you know the correct equation? It can be derived by applying the 1st law of thermodynamics to this adiabatic reversible compression. What would the 1st law give you for this?
 
Chestermiller said:
You suppose correctly. Do you know the correct equation? It can be derived by applying the 1st law of thermodynamics to this adiabatic reversible compression. What would the 1st law give you for this?
The first law of thermodynamics would be conservation of energy, which would be Internal Energy=Q+W. Since it's an adiabatic system, Energy would just be equal to work. E=p deltaV and nCv delta T... Right?
 
ScreamingIntoTheVoid said:
The first law of thermodynamics would be conservation of energy, which would be Internal Energy=Q+W. Since it's an adiabatic system, Energy would just be equal to work. E=p deltaV and nCv delta T... Right?
Yes! Except that, because the process is reversible, those deltas should be d’s. That is, differentials. And there should be a minus sign. Now substitute p=nRT/V into the equation. What does that give you?
 
Do you mean the volume value I calculated before or the actual equation itself?
E= -(4.5 atm) (d/dv 25.734016 L) =...
E= nRT/v x d/dv V -> E= nRT d/dv
(I'm sorry I lost momentum here I'm unsure what to do.)
 
  • #10
What I'm saying is $$nC_vdT=-\frac{nRT}{V}dV$$ Does this equation make sense to you?
 
  • #11
Chestermiller said:
What I'm saying is $$nC_vdT=-\frac{nRT}{V}dV$$ Does this equation make sense to you?
I thought I did but based on what I came up with it seems I've shamed my calculus teacher

∫nCvdt=-∫nRT/v dV → nCvT1-nCvT2=-(nRT)ln(V1)-(nRTln(V2)
So if I plug what I know
(1.6 mol)(20.5 J K-1 mol-1)(294K) - (1.6 mol)(20.5 J K mol)(T2)=-[(1.6)(8.315)(294)ln(25.734016 L)-(1.6)(8.315)(294)(lnV2)]

-3060.220545=(1.6 mol)(20.5 J K mol)(T) - (319.296)(ln (25.734016 L/ V2)

So I'm assuming this is super wrong?
 
  • #12
This is not integrated correctly. And, please stop substituting numbers. Do it all algebraically.
 

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