
To find the angular frequency of the oscillations for this system, we can use the formula for the angular frequency of a mass-spring system:
\(\omega = \sqrt{\frac{k}{m_{\text{eff}}}}\)
where:
Given values from the diagram:
Because both blocks move together, they contribute to the system's effective mass. Therefore, the effective mass \(m_{\text{eff}}\) is the reduced mass given by:
\(m_{\text{eff}} = \frac{m_1 \cdot m_2}{m_1 + m_2}\)
Substituting the known values:
\(m_{\text{eff}} = \frac{2 \times 3}{2 + 3} = \frac{6}{5} = 1.2 \, \text{kg}\)
Now, substitute \(k\) and \(m_{\text{eff}}\) into the angular frequency formula:
\(\omega = \sqrt{\frac{150}{1.2}}\)
\(= \sqrt{125}\)
\(= 5\sqrt{5}\)\)
This means the angular frequency of the system is \(5\sqrt{5}\).
Conclusion: The correct answer is \(\boxed{5\sqrt{5}}\).

Using a variable frequency ac voltage source the maximum current measured in the given LCR circuit is 50 mA for V = 5 sin (100t) The values of L and R are shown in the figure. The capacitance of the capacitor (C) used is_______ µF.
