The problem is addressed by first analyzing the relationship between oscillation frequency and attached mass, defined by the mass-spring system frequency formula: \( f = \frac{1}{2\pi}\sqrt{\frac{k}{m}} \). Here, \( k \) represents the spring constant, and \( m \) denotes the mass.
With mass \( m \), the frequency is \( f_1 = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \).
For mass \( 9m \), the frequency is \( f_2 = \frac{1}{2\pi} \sqrt{\frac{k}{9m}} \). This simplifies to \( f_2 = \frac{1}{2\pi} \frac{1}{3} \sqrt{\frac{k}{m}} \), which is equivalent to \( f_2 = \frac{1}{3} \cdot f_1 \).
Consequently, the ratio \(\frac{f_1}{f_2}\) is calculated as \(\frac{f_1}{\frac{1}{3}f_1} = 3\).
Therefore, the value of \(\frac{f_1}{f_2}\) is \( 3 \), which is within the specified range of 3 to 3.
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: