Show that, for a pure substance, [left(frac{partial s}{partial T} ight)_{p}=left(frac{partial s}{partial T} ight)_{v}+left(frac{partial s}{partial v} ight)_{T}left(frac{partial v}{partial
Question:
Show that, for a pure substance,
\[\left(\frac{\partial s}{\partial T}\right)_{p}=\left(\frac{\partial s}{\partial T}\right)_{v}+\left(\frac{\partial s}{\partial v}\right)_{T}\left(\frac{\partial v}{\partial T}\right)_{p}\]
and from this, prove that
\[c_{p}-c_{v}=T\left(\frac{\partial p}{\partial T}\right)_{v}\left(\frac{\partial v}{\partial T}\right)_{p} .\]
The following table gives values of the specific volume of water, in cubic metres per kilogram. A quantity of water is initially at \(30^{\circ} \mathrm{C}, 20 \mathrm{bar}\) and occupies a volume of \(0.2 \mathrm{~m}^{3}\). It is heated at constant volume to \(50{ }^{\circ} \mathrm{C}\) and then cooled at constant pressure to \(30^{\circ} \mathrm{C}\). Calculate the net heat transfer to the water.
[438 kJ]
Step by Step Answer:
Advanced Thermodynamics For Engineers
ISBN: 9780080999838
2nd Edition
Authors: D. E. Winterbone, Ali Turan