We start by noting that:
\( 1 \sin 60^\circ = \frac{\sqrt{3}}{2} r \)
Thus, \( r = 45^\circ \).
Next, we compute:
\( \frac{\sqrt{3}}{2} \sin 45^\circ = \sqrt{3} \sin r_2 \)
which gives \( r_2 = 30^\circ \).
Finally, we solve for:
\(\left( \frac{1}{\sqrt{3}} + \frac{\sqrt{3} - 1}{2 \sqrt{3}} + \frac{\sqrt{3} - 1}{2 \sqrt{3}} \right) \times n\)
\(= \frac{8}{\sqrt{3}} \quad \Rightarrow \quad n = 4.\)
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 :
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
The major products obtained from the reactions in List-II are the reactants for the named reactions mentioned in List-I. Match each entry in List-I with the appropriate entry in List-II and choose the correct option.
Moment of inertia is defined as the quantity expressed by the body resisting angular acceleration which is the sum of the product of the mass of every particle with its square of a distance from the axis of rotation.
In general form, the moment of inertia can be expressed as,
I = m × r²
Where,
I = Moment of inertia.
m = sum of the product of the mass.
r = distance from the axis of the rotation.
M¹ L² T° is the dimensional formula of the moment of inertia.
The equation for moment of inertia is given by,
I = I = ∑mi ri²
To calculate the moment of inertia, we use two important theorems-