Given:
\[ T = 3.14 = \frac{2\pi}{\omega}. \]
Solving for \( \omega \):
\[ \omega = 2 \, \text{rad/s}. \]
The displacement \( x \) is given by:
\[ x = 10 \sin\left(\omega t + \frac{\pi}{3}\right). \]
To find the velocity \( v \), differentiate \( x \) with respect to \( t \):
\[ v = \frac{dx}{dt} = 10\omega \cos\left(\omega t + \frac{\pi}{3}\right). \]
At \( t = 0 \):
\[ v = 10\omega \cos\left(\frac{\pi}{3}\right) = 10 \times 2 \times \frac{1}{2} = 10 \, \text{m/s}. \]
Answer: 10 m/s
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity):
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: