Starting with the same initial conditions an ideal gas expands from volume V1 to V2 in three different ways. The work done by the gas is W1 if the process is purely isothermal, W2 if purely isobaric and W3 if purely adiabatic. Then

Process - 2 IsobaricProcess - 1 IsothermalProcess - 3 AdiabaticIn a thermodynamics process, work done by the gas = Area under P-V diagram.

Starting with the same initial conditions an ideal gas expands from volume V1 to V2 in three different ways. The work done by the gas is W1 if the process is purely isothermal, W2 if purely isobaric and W3 if purely adiabatic. Then

Process - 2 IsobaricProcess - 1 IsothermalProcess - 3 AdiabaticIn a thermodynamics process, work done by the gas = Area under P-V diagram.

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Starting with the same initial conditions an ideal gas expands from volume V₁ to V₂ in three different ways. The work done by the gas is W₁ if the process is purely isothermal, W₂ if purely isobaric and W₃ if purely adiabatic. Then

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W₂ > W₁ > W₃

W₁ > W₂> W₃

W₁ > W₃ > W₂

W₂ > W₃ > W₁

answer is A.

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Process - 2 $\large \to$ Isobaric

Process - 1 $\large \to$ Isothermal

Process - 3 $\large \to$ Adiabatic

In a thermodynamics process, work done by the gas = Area under P-V diagram.

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Starting with the same initial conditions an ideal gas expands from volume V1 to V2 in three different ways. The work done by the gas is W1 if the process is purely isothermal, W2 if purely isobaric and W3 if purely adiabatic. Then

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Starting with the same initial conditions an ideal gas expands from volume V₁ to V₂ in three different ways. The work done by the gas is W₁ if the process is purely isothermal, W₂ if purely isobaric and W₃ if purely adiabatic. Then