The work done in an adiabatic change in an id | vedclass

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(D) For an adiabatic process,the heat exchange $Q = 0$. According to the first law of thermodynamics,$\Delta Q = \Delta U + \Delta W$. Since $\Delta Q

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change in its temperature

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(D) For an adiabatic process,the heat exchange $Q = 0$. According to the first law of thermodynamics,$\Delta Q = \Delta U + \Delta W$. Since $\Delta Q = 0$,we have $\Delta W = -\Delta U$. The change in internal energy for an ideal gas is given by $\Delta U = nC_{v} \Delta T$. Therefore,the work done is $\Delta W = -nC_{v} \Delta T$. This shows that the work done in an adiabatic process depends only on the change in temperature $\Delta T$.

The work done in an adiabatic change in an ideal gas depends upon only

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