For an isothermal reversible change of the system, the work function is (a) (left(frac{partial A}{partial V} ight)_{T}=P)
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For an isothermal reversible change of the system, the work function is
(a) \(\left(\frac{\partial A}{\partial V}\right)_{T}=P\)
(b) \(\left(\frac{\partial A}{\partial U}\right)_{T}=-P\)
(c) \(\left(\frac{\partial A}{\partial V}\right)_{T}=-P\)
(d) \(\left(\frac{\partial A}{\partial V}\right)_{T}=-P-1\).
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