\(0< i b < 30\)
\(30< i_b < 45\)
\(45< i_b < 90\)
\(i_b = 90\)
Brewster's angle is the angle at which light with a specific polarization passes through a dielectric surface without any reflection. When unpolarized light hits the surface at this angle, the reflected light is completely polarized.
At the interface, Brewster's angle \(i_b\) is given by: \(μ=tani_b \ (1)\)
Here, \(\mu\) is the refractive index of the material, which ranges from 1 to ∞: \(1 < \mu < \infty\)
Substituting equation (1) into this range, we get: \(1 < \tan i_b < \infty\)
Therefore, the polarization angle \( i_b\) falls within: \(\tan^{-1}(1) < i_b < \tan^{-1}(\infty)\)
\(\Rightarrow 45^\circ < i_b < 90^\circ\)
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec: 