(i) Work done on the copper, W :
Work done during isothermal compression is given by
W = \(\int_1^2pdv\)
The isothermal compressibility is given by
![](https://www.sarthaks.com/?qa=blob&qa_blobid=14766214475745321370)
Since v and K remain essentially constant
![](https://www.sarthaks.com/?qa=blob&qa_blobid=17192413391235003028)
The negative sign indicates that the work is done on the copper block.
(ii) Change in entropy :
The change in entropy can be found by using the following Maxwell relation :
![](https://www.sarthaks.com/?qa=blob&qa_blobid=12984012415255083252)
Integrating the above equation, assuming v and β remaining constant, we get
s2 – s1 = – vβ (p2 – p1)T
= – 0.114 × 10–3 × 5 × 10–5 [800 × 105 – 20 × 105]
= – 0.114 × 10–3 × 5 (800 – 20) = – 0.446 J/kg K.
(iii) The heat transfer, Q :
For a reversible isothermal process, the heat transfer is given by :
Q = T(s2 – s1) = (15 + 273)(– 0.4446) = – 128 J/kg
(iv) Change in internal energy, du :
The change in internal energy is given by :
du = Q – W
= – 128 – (– 3.135) = – 124.8 J/kg.
(v) cp – cv :
The difference between the specific heat is given by :
cp – cv = \(\cfrac{\beta^2Tv}K\)
= \(\cfrac{(5\times10^{-5})^2\times(15+273) \times0.114 \times10^{-3}}{8.6\times10^{-12}}\)
9.54 J/kg K