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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