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 :
Let $ S $ denote the locus of the point of intersection of the pair of lines $$ 4x - 3y = 12\alpha,\quad 4\alpha x + 3\alpha y = 12, $$ where $ \alpha $ varies over the set of non-zero real numbers. Let $ T $ be the tangent to $ S $ passing through the points $ (p, 0) $ and $ (0, q) $, $ q > 0 $, and parallel to the line $ 4x - \frac{3}{\sqrt{2}} y = 0 $.
Then the value of $ pq $ is
Let $ y(x) $ be the solution of the differential equation $$ x^2 \frac{dy}{dx} + xy = x^2 + y^2, \quad x > \frac{1}{e}, $$ satisfying $ y(1) = 0 $. Then the value of $ 2 \cdot \frac{(y(e))^2}{y(e^2)} $ is ________.
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-