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Starting with the same initial conditions, an ideal gas expands from volume `V_1 to V_2` in three different ways. The work done by the gas is W_1 if the process is purely isothermal, `W_2`if purely isobaric and `W_3` if purely adiabatic. Then

A

`W_(1) lt W_(2) lt W_(3)`

B

`W_(2) lt W_(3) lt W_(1)`

C

`W_(3) lt W_(1) lt W_(2)`

D

`W_(2) lt W_(1) lt W_(3)`

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