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Question: The work done during adiabatic expansion or compression of an ideal gas is given by: (the question...

The work done during adiabatic expansion or compression of an ideal gas is given by:
(the question has multiple correct options)
(A) nCvΔTn{{C}_{v}}\Delta T
(B) nRγ1(T2T1)\dfrac{nR}{\gamma -1}({{T}_{2}}-{{T}_{1}})
(C)nRPext[T2P1T1P2P1P2]-nR{{P}_{ext}}[\dfrac{{{T}_{2}}{{P}_{1}}-{{T}_{1}}{{P}_{2}}}{{{P}_{1}}{{P}_{2}}}]
(D) 2.303RTV2V1-2.303RT\dfrac{{{V}_{2}}}{{{V}_{1}}}

Explanation

Solution

In thermodynamics, the subject which is under investigation or collection of matter is being studied is called a system, which is surrounded by a boundary is a closed surface. Through the system and surroundings, the energy and mass changes may be entered or leave.

Complete step by step solution:
According to the thermodynamics in system and surrounding, there are three types of systems,
(1) open system: A system can change both energy and matter with surroundings.
(2) closed system: A system can exchange only energy, not matter with surroundings
(3) isolated system: the system either energy or matter with surroundings.
When an ideal gas compressed adiabatically (Q=0) temperature increases and work is done.
Similarly, adiabatic expansion, the temperature drops with work done.
In the adiabatic process of expansion, with Q=0, and W = 0, according to the first law of thermodynamics, there is no change in the internal energy of the system.
The work is done by the adiabatic expansion, dW=pdV where dQ=0
Therefore, apply the first law of thermodynamics, work done during adiabatic expansion is
W=nCvΔTW=n{{C}_{v}}\Delta T
From the ideal gas law, the temperature of the mixture after the adiabatic compression is
T2=(P2V2P1V1)T1{{T}_{2}}=(\dfrac{{{P}_{2}}{{V}_{2}}}{{{P}_{1}}{{V}_{1}}}){{T}_{1}}
Then the work done by the mixture during the adiabatic compression is,
W=V2V1pdVW=\int{{{^{{{V}_{2}}}}_{{{V}_{1}}}}pdV}
Then W = 2.303RTV2V1-2.303RT\dfrac{{{V}_{2}}}{{{V}_{1}}}
When an ideal gas in a quasi-static adiabatic process, PVγ1=constantP{{V}^{\gamma -1}}=cons\tan t
A reversible adiabatic expansion of an ideal gas, the work done is,
Wext=nRPext[T2P1T1P2P1P2]{{W}_{ext}}=-nR{{P}_{ext}}[\dfrac{{{T}_{2}}{{P}_{1}}-{{T}_{1}}{{P}_{2}}}{{{P}_{1}}{{P}_{2}}}]

Hence, the options A, C, and D are correct answers.

Note: Most materials expand when heated expect water between 0oC4oC{{0}^{o}}C-{{4}^{o}}C , which with increasing temperature decreases volume. Cp>Cv{{C}_{p}}>{{C}_{v}} , then expansion occurs under constant pressure with work on surroundings.