Adiabatic expansion at constant pressure.

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SUMMARY

The discussion centers on the thermodynamic principles governing adiabatic expansion of a gas, specifically 4.00 mol of oxygen at 270K in a 20L vessel, expanding against a constant external pressure of 600 torr. The key equations used include U=q+w and H=U+PV, leading to the conclusion that ΔH=0 under the conditions of constant external pressure, despite the internal pressure changing. The participants clarify that ΔH=q only holds when the system pressure remains constant, and they resolve confusion regarding the relationship between Δ(PV) and Δ(nRT).

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  • Understanding of thermodynamic concepts such as adiabatic processes and enthalpy.
  • Familiarity with the ideal gas law and the properties of perfect gases.
  • Knowledge of the first law of thermodynamics and its application in calculating work and internal energy.
  • Ability to differentiate between system pressure and external pressure in thermodynamic equations.
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LogicX
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Homework Statement



A sample of 4.00mol of oxygen is originally confined in a 20L vessel at 270K and then undergoes adiabatic expansion against a constant pressure of 600torr until the volume has tripled. Find q, W, dT, dU, dH.

Homework Equations



U=q+w
H=U+PV

The Attempt at a Solution



q=0 (Adiabatic)

w=-pexΔV

U=w

ΔT= ΔU/Cv

ΔH=0The reason I'm posting this is because I believe that all of the above is correct, but my friend claims that ΔH is not zero. First of all, ΔH=q for a constant pressure expansion, and q=0, so ΔH=0, right?

Also:

ΔH=ΔU+Δ(PV)=w+ PΔV= -PΔV+PΔV=0

I believe oxygen is considered a perfect gas in this question, because we are expected to calculate C(v) from C(p)-C(v)=nR

So, am I right, does ΔH=0?

EDIT:

So, I get different answers depending on whether I use ΔH=ΔU+Δ(PV) or ΔH=ΔU+Δ(nRT)

Shouldn't they be the same? shouldn't Δ(PV)=Δ(nRT) ?

I've been obsessing over problems like this for weeks now. Every time I figure one thing out another thing pops up that just confuses everything for me.
 
Last edited:
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LogicX said:
The reason I'm posting this is because I believe that all of the above is correct, but my friend claims that ΔH is not zero. First of all, ΔH=q for a constant pressure expansion, and q=0, so ΔH=0, right?

No, ΔH = q only if the pressure of the system stay constant. Although the external pressure is constant in this problem, the pressure of the system is not.
 
Ygggdrasil said:
No, ΔH = q only if the pressure of the system stay constant. Although the external pressure is constant in this problem, the pressure of the system is not.

Are you talking about a reversible vs. irreversible change here?

So why does Δ(PV) not equal Δ(nRT)? Is it because to use Δ(PV), the P that you use has to be constant for the whole system? I didn't see that anywhere in my textbook.

So the P in the work equation is p(external) and in the enthalpy equation it is the pressure of the system?

EDIT: Ok, I see see that my last statement is correct, and Δ(PV) does indeed equal Δ(nRT), but since P is changing Δ(PV)≠PΔV because P is the pressure of the system. So we just use nRΔT because we know all those quantities.

I'm glad I finally cleared this up.
 
Last edited:

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