For any pure substance, the difference between (C_{P}) and (C_{V}) can be expressed in terms of the
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For any pure substance, the difference between \(C_{P}\) and \(C_{V}\) can be expressed in terms of the isothermal compressibility \(\alpha\) and volume expansivity \(\beta\) as
(a) \(C_{P}-C_{V}=\frac{T V \beta}{\alpha^{2}}\)
(b) \(C_{P}-C_{V}=\frac{T V \beta^{2}}{\alpha}\)
(c) \(C_{P}-C_{V}=\frac{T V \alpha}{\beta^{2}}\)
(d) \(C_{P}-C_{V}=\frac{T V \alpha^{2}}{\beta}\).
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