As shown in the figure, a spring is kept in a stretched position with some extension by holding the masses \(1\,\text{kg}\) and \(0.2\,\text{kg}\) with a separation more than spring natural length and then released. Assuming the horizontal surface to be frictionless, the angular frequency (in SI unit) of the system is _______. (Given \(k=150\,\text{N/m}\)) 
\(30\)
\(20\)
To find the angular frequency of the system, we use the formula for the angular frequency of a simple harmonic oscillator, which is given by:
\(\omega = \sqrt{\frac{k}{\mu}}\)
where \(\omega\) is the angular frequency, \(k\) is the spring constant, and \(\mu\) is the reduced mass of the system.
The reduced mass \(\mu\) for two masses \(m_1\) and \(m_2\) is calculated as:
\(\mu = \frac{m_1 \cdot m_2}{m_1 + m_2}\)
Given:
First, calculate the reduced mass \(\mu\):
\(\mu = \frac{1 \cdot 0.2}{1 + 0.2} = \frac{0.2}{1.2} = \frac{1}{6}\,\text{kg}\)
Now, substitute the values into the angular frequency formula:
\(\omega = \sqrt{\frac{150}{\frac{1}{6}}} = \sqrt{150 \times 6} = \sqrt{900}\)
\(\omega = 30\,\text{rad/s}\)
However, it seems there is an error in the calculated value. Let's re-evaluate:
\(\omega = \sqrt{\frac{150}{\frac{1}{6}}} = \sqrt{150 \times 6} = \sqrt{900} = 30\,\text{rad/s}\)
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 