At ordinary temperature, the molecules of an ideal gas have only translational and rotational kinetic energies. At high temperatures they may also have vibrational energy. As a result of this at higher temperatures (Cv = molar heat capacity at constant volume) :–
(a) Cv = 3R/2 for a monoatomic gas
(b) Cv > 3R/2 for a monoatomic gas
(c) Cv > 5R/2 for a diatomic gas
(d) Cv = 5R/2 for a diatomic gas