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In an irreversible process taking place at constant \( \mathrm{T} \) and \( \mathrm{P} \) and in which only pressure-volume work is being done, the change in Gibbs free energy (dG) and change in entropy (dS), satisfy the criteria
(a) \( (\mathrm{dS})_{\mathrm{V}, \mathrm{E}}0,(\mathrm{dG})_{\mathrm{T}, \mathrm{P}}0 \)
(b) \( (\mathrm{dS})_{\mathrm{V}, \mathrm{E}}=0,(\mathrm{dG})_{\mathrm{T}, \mathrm{P}}=0 \)
- (c) \( (\mathrm{dS})_{\mathrm{V}, \mathrm{E}}=0,(\mathrm{dG})_{\mathrm{T}, \mathrm{P}}0 \)
-(d) \( (\mathrm{dS})_{\mathrm{V}, \mathrm{E}}0,(\mathrm{dG})_{\mathrm{T}, \mathrm{P}}0 \)
\( \mathrm{P} \)
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