

For Particle to be in equilibrium,
\(mg\,sin \theta = mx\,\omega^2cos\theta\)
⇒ \(tan \theta =\frac{\omega^2x}g\)
Also, \(y=4 c x^{2}\)
⇒ \(\frac{dy}{dx} = 8cx =\) Slope at point P = \(tan \theta\)
Equating both values of \(tan\theta\) we get,
\(\frac{\omega^2x}g = 8cx\)
⇒ \(\omega^2 = 8cg\)
⇒ \(\omega = \sqrt{8cg} = 2\sqrt{2cg}\)
Therefore, The correct option is (B): \(2\sqrt{2cg}\)

A string of length \( L \) is fixed at one end and carries a mass of \( M \) at the other end. The mass makes \( \frac{3}{\pi} \) rotations per second about the vertical axis passing through the end of the string as shown. The tension in the string is ________________ ML.
For a short dipole placed at origin O, the dipole moment P is along the X-axis, as shown in the figure. If the electric potential and electric field at A are V and E respectively, then the correct combination of the electric potential and electric field, respectively, at point B on the Y-axis is given by:

If A and B are two events such that \( P(A \cap B) = 0.1 \), and \( P(A|B) \) and \( P(B|A) \) are the roots of the equation \( 12x^2 - 7x + 1 = 0 \), then the value of \(\frac{P(A \cup B)}{P(A \cap B)}\)
A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is: