\(0< i b < 30\)
\(30< i_b < 45\)
\(45< i_b < 90\)
\(i_b = 90\)
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 sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :