Work Done on N2 Gas in Isothermal Expansion: Irreversible vs Reversible

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The discussion focuses on calculating the work done on nitrogen gas (N2) during isothermal expansion from an initial pressure of 5 atm to a final pressure of 1 atm. For the irreversible process, the work done is calculated using the formula w' = p(ext) (Vf - Vi), resulting in -4040 J. In contrast, the reversible process uses the equation w' = nRT ln(Vf / Vi), yielding -1625 J. The results confirm that the work done in the reversible process is less negative, indicating that maximum work occurs in reversible conditions, as expected.

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2 litres of N2 held in a piston at a pressure of 5 atm initially held at
T=273K expands isothermally until the final pressure is 1 atm. What is
the work done on the gas in this expansion under (i) irreversible and (ii)
reversible conditions? Comment on the magnitude of your answers to
(i) and (ii). (You may assume that N2 behaves as an ideal gas.)

My attempt:

for irreversible we have : w' = p(ext) (Vf -Vi)

I've taken p(external) to be 5 atm = 5.05x10^5 Pa

V (initial) is 2 litres = 0.002 m^3

to find Vfinal i used V = P x V (initial)/ P final

to get V final = 0.01

Putting these numbers into w' = p(ext) (Vf -Vi) to get 4040 J, but for the work done on the system this is -4040j

For reversible is used w' = nRT ln (Vf / Vi) to get 1625 J, so for work done on the system = -1625 J

But the Reversible process should be higher as maximum work occurs so the value for the irreversible should be lower.

Where have I gone wrong?
 
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Any ideas?
 
has anyone had a go at this?
 

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