Given:
The period \( T \) is \( T = 3.14 = \frac{2\pi}{\omega}. \)
Solving for \( \omega \):
The angular frequency is \( \omega = 2 \, \text{rad/s}. \)
The displacement \( x \) is described by:
\( x = 10 \sin\left(\omega t + \frac{\pi}{3}\right). \)
To determine the velocity \( v \), differentiate \( x \) with respect to \( t \):
\( v = \frac{dx}{dt} = 10\omega \cos\left(\omega t + \frac{\pi}{3}\right). \)
At \( t = 0 \):
The velocity is \( v = 10\omega \cos\left(\frac{\pi}{3}\right) = 10 \times 2 \times \frac{1}{2} = 10 \, \text{m/s}. \)
Result: 10 m/s
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is: