For a thermodynamic system, the coefficient of volume expansion \(\beta=\frac{1}{V}(\frac{βV}{βT})_P\) and compressibility \(K=-\frac{1}{V}(\frac{βV}{βP})_T\) , where V, T, and P are respectively the volume, temperature, and pressure. Considering that \(\frac{dV}{V}\) is a perfect differential, we get