Answer: \(C_V = \dfrac{3}{2}R\); kinetic energy \(\approx 607.8\) J.
(i) Molar specific heat at constant volume: A molecule of a monoatomic gas has only three translational degrees of freedom (along x, y and z). By the law of equipartition of energy, each degree of freedom has average energy \(\frac{1}{2}k_BT\), so the average energy per molecule is
\[\bar{E} = 3\times\frac{1}{2}k_BT = \frac{3}{2}k_BT\]
The internal energy of one mole (\(N_A\) molecules) is
\[E = \frac{3}{2}N_Ak_BT = \frac{3}{2}RT\qquad (R = N_Ak_B)\]
At constant volume no work is done, so all the heat supplied increases the internal energy. Hence
\[C_V = \frac{dE}{dT} = \frac{3}{2}R\]
Also \(C_P = C_V + R = \dfrac{5}{2}R\) and \(\gamma = \dfrac{C_P}{C_V} = \dfrac{5}{3}\).
(ii) Numerical: \(V = 4000\) cc \(= 4\times10^{-3}\) m\(^3\), \(P = 1.013\times10^5\) N/m\(^2\).
From kinetic theory, \(P = \dfrac{2}{3}\dfrac{E}{V}\), so the total kinetic energy is
\[E = \frac{3}{2}PV = \frac{3}{2}\times1.013\times10^5\times4\times10^{-3} = 6\times101.3 = 607.8\ \mathrm{J}\]