The molar excess Gibbs free energy ($g^E$) of a liquid mixture of $A$ and $B$ is given by
\[
\frac{g^E}{RT} = x_A x_B [C_1 + C_2(x_A - x_B)]
\]
where $x_A$ and $x_B$ are the mole fraction of $A$ and $B$, respectively, the universal gas constant, $R = 8.314$ J K$^{-1}$ mol$^{-1}$, $T$ is the temperature in K, and $C_1, C_2$ are temperature-dependent parameters. At 300 K, $C_1 = 0.45$ and $C_2 = -0.018$. If $\gamma_A$ and $\gamma_B$ are the activity coefficients of $A$ and $B$, respectively, the value of
\[
\int_{0}^{1} \ln\left(\frac{\gamma_A}{\gamma_B}\right)\,dx_A
\]
at 300 K and 1 bar is \(\underline{\hspace{2cm}}\) (rounded off to the nearest integer).