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:
Given:
\( x_1 = \sqrt{7} \sin 5t \), \quad \( x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \)
Representing the displacements using phasors, we have:
Magnitudes: \( \sqrt{7} \) and \( 2 \sqrt{7} \). Phase difference: \( 60^\circ \).
The amplitude of the resultant simple harmonic motion (SHM) is \( 7 \).
The phase angle \( \phi \) is calculated as: \( \phi = \tan^{-1} \left( \frac{2 \sqrt{7} \times \frac{\sqrt{3}}{2}}{\sqrt{7} + 2 \sqrt{7} \times \frac{1}{2}} \right) = \tan^{-1} \left( \frac{\sqrt{3}}{2} \right) = \tan^{-1} \left( \sqrt{3} \right) \).
The resultant SHM is given by: \( X_R = 7 \sin \left( 5t + \phi \right) \).
The acceleration of the resultant SHM is: \( a_R = 7 \times 25 \sin \left( 5t + \phi \right) \).
The maximum acceleration is: \( a_{\text{max}} = 175 \, \text{cm/sec} = 175 \times 10^{-2} \, \text{m/sec} \).