In a classical gas of hard spheres (of diameter σ), the spatial distribution of the particles is no longer uncorrelated. Roughly speaking, the presence of n particles in the system leaves only a volume (V−nv0) available for the (n+1)th particle; clearly, v0 would be proportional to σ3. Assuming that Nv0≪V, determine the dependence of Ω(N,V,E) on V [cf. eqn. (1.4.1)] and show that, as a result of this, V in the gas law (1.4.3) gets replaced by (V−b), where b is four times the actual space occupied by the particles.