Brewster's angle \( \theta_B \) is the angle of incidence at which light with a particular polarization is perfectly transmitted through a transparent dielectric surface, with no reflection. The relationship for Brewster's angle is given by:
\[
\tan \theta_B = \frac{n_2}{n_1}
\]
Where:
- \( n_1 \) is the refractive index of the first medium (usually air),
- \( n_2 \) is the refractive index of the second medium.
Since the refractive index of air is less than most other materials, Brewster's angle usually lies between \( 45^\circ \) and \( 90^\circ \) depending on the relative refractive indices.
Thus, Brewster's angle generally lies between \( 45^\circ \) and \( 90^\circ \).