To determine the time period of a particle executing simple harmonic motion (SHM), given its maximum acceleration \( \alpha \) and maximum velocity \( \beta \), we need to understand the SHM equations and relationships.
- For SHM, the displacement \( x(t) \) in terms of angular frequency \( \omega \) and amplitude \( A \) is given by:
x = A \sin(\omega t).
- The maximum velocity \( v_{\text{max}} \) of a particle in SHM is given by:
\(\beta = \omega A\).
- The maximum acceleration \( a_{\text{max}} \) is given by:
\(\alpha = \omega^2 A\).
- We can express the amplitude \( A \) in terms of \( \beta \) and \( \alpha \) using:
A = \frac{\beta}{\omega}
- Using the maximum acceleration expression, we have:
A = \frac{\alpha}{\omega^2}
- Equating both expressions for \( A \), we get:
\frac{\beta}{\omega} = \frac{\alpha}{\omega^2},
- Solving for \( \omega \), we find:
\omega = \frac{\alpha}{\beta}.
- The time period \( T \) of SHM is related to angular frequency by:
T = \frac{2\pi}{\omega}.
- Substituting the expression for \( \omega \), we get:
T = \frac{2\pi \beta}{\alpha}.
Thus, the correct time period of the vibration is provided by the formula:
\(\frac{2\pi \beta}{\alpha}\).
Therefore, the correct option is:
\(\frac{2\pi \beta}{\alpha}\).