Given that the velocity of the center of mass (VCM) is:
\( V_{\text{CM}} = 2R \omega \)
At the point of contact, we have:
\( V_{\text{CM}} = \omega_0 R \Rightarrow \omega_0 = 2 \omega \)
Now, the angular momentum of disk B with respect to the center of disk A is calculated as:
\( L = \left( \frac{MR^2}{2} \right) (\omega_0) + M (2R \omega) (2R) \)
Substitute the values of \( \omega_0 \) and simplify:
\( L = \left( \frac{MR^2}{2} \right) (2\omega) + 4MR^2 \omega \)
\( L = 5MR^2 \omega \) and hence, \( n = 5 \).
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 ________.
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: