The entropy change due to a change in the number of available states is given by:
\[
S = k_B \ln W
\]
For two possible arrangements (CO and OC), the thermodynamic probability \( W \) is:
\[
W = 2 \text{(since there are two arrangements)}
\]
Thus, the entropy is:
\[
S = k_B \ln 2
\]
Where \( k_B = 1.38 \times 10^{-23} \, \text{J/K} \) is Boltzmann's constant.
For 1 mol of CO:
\[
S = 1.38 \times 10^{-23} \times \ln 2 \times N_A
\]
Where \( N_A = 6.022 \times 10^{23} \) (Avogadro's number).
\[
S \approx 5.76 \, \text{J K}^{-1} \, \text{mol}^{-1}
\]
Final Answer:
\[
\boxed{5.76 \, \text{J K}^{-1} \, \text{mol}^{-1}}
\]