Using the free-particle eigenstates and density of states previously applied in Fermi-Dirac thermodynamics the spin = 0 (no spin degeneracy) BE grand potential (see Eq.16.6) is
Using the free-particle eigenstates and density of states previously applied in Fermi-Dirac thermodynamicsthe spin = 0 (no spin degeneracy) BE grand potential (see Eq.16.6) is