Question Details

Consider a fully adiabatic piston-cylinder arrangement as shown in the figure. The piston is massless and cross-sectional area of the cylinder is 𝐴. The fluid inside the cylinder is air (considered as a perfect gas), with Ξ³ being the ratio of the specific heat at constant pressure to the specific heat at constant volume for air. The piston is initially located at a position 𝐿1. The initial pressure of the air inside the cylinder is 𝑃1 ≫ 𝑃0, where 𝑃0 is the atmospheric pressure. The stop S1 is instantaneously removed and the piston moves to the position 𝐿2, where the equilibrium pressure of air inside the cylinder is 𝑃2 ≫ 𝑃0.

What is the work done by the piston on the atmosphere during this process?


Options

A

0

B

𝑃0𝐴(𝐿2 βˆ’ 𝐿1 )

C

𝑃1𝐴𝐿1 ln( 𝐿1/ 𝐿2)

D

(𝑃2𝐿2 βˆ’ 𝑃1𝐿1)𝐴 /(1 βˆ’ Ξ³)

Show Answer

Correct Answer :

Option B

𝑃0𝐴(𝐿2 βˆ’ 𝐿1 )

Solution :

The correct option is 𝑃0𝐴(𝐿2 βˆ’ 𝐿1).

Analysis of the Figure:
From the provided diagram, we can identify the following labels and parameters:
1. The cylinder contains air at pressure 𝑃1, and the piston is at the "Initial position of the piston" at a distance 𝐿1 from the left wall.
2. A stop S1 prevents the piston from moving further right initially.
3. When the stop S1 is removed, the piston moves to the "Final position of the piston" at a distance 𝐿2, where it is stopped by S2.
4. The space outside the cylinder is labeled "Atmosphere, pressure 𝑃0".

Step-by-Step Explanation:
The work done by the piston on the atmosphere is the work done against the constant external atmospheric pressure 𝑃0.
The constant force exerted by the atmosphere on the piston of cross-sectional area 𝐴 is:

Fatm=P0A

During the process, the piston moves from position 𝐿1 to position 𝐿2. The displacement of the piston is:

Ξ”x=L2βˆ’L1

Since the atmospheric pressure remains constant at 𝑃0 throughout this movement, the work done by the piston to push back the atmosphere is the product of the atmospheric force and the displacement:

W=FatmΓ—Ξ”x

Substituting the force and displacement into the equation, we get:

W=P0A(L2βˆ’L1)

Thus, the work done by the piston on the atmosphere during this process is indeed 𝑃0𝐴(𝐿2 βˆ’ 𝐿1).

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