The general solution of $ 2 \cos 4x + \sin^2 2x $= 0 is

To solve the equation \(2 \cos 4x + \sin^2 2x = 0\), we start by rewriting it using trigonometric identities.
We know that \(\sin^2 \theta = 1 - \cos^2 \theta\). Hence, \(\sin^2 2x = 1 - \cos^2 2x\). Substituting in the equation gives:
\(2 \cos 4x + 1 - \cos^2 2x = 0\)
Rearranging terms, we obtain:
\(2 \cos 4x = \cos^2 2x - 1\)
Using the double angle formula, \(\cos 4x = 2 \cos^2 2x - 1\), we equate:
\(2(2 \cos^2 2x - 1) = \cos^2 2x - 1\)
Simplifying, we get:
\(4 \cos^2 2x - 2 = \cos^2 2x - 1\)
Thus:
\(3 \cos^2 2x = 1\)
\(\cos^2 2x = \frac{1}{3}\)
Taking the square root, we find:
\(\cos 2x = \pm \frac{\sqrt{3}}{3}\)
The general solution for \( \cos 2x = \pm \frac{\sqrt{3}}{3} \) is:
\(2x = 2n\pi \pm \cos^{-1}\left(\frac{\sqrt{3}}{3}\right)\)
Therefore, the solution for \(x\) is:
\(x = n\pi \pm \frac{1}{2} \cos^{-1}\left(\frac{\sqrt{3}}{3}\right)\)
Since \(\cos^{-1}\left(\frac{\sqrt{3}}{3}\right) = \sin^{-1}\left(\pm \frac{\sqrt{2}}{3}\right)\):
The equation simplifies to:
\(x = \frac{\pi}{4} + (-1)^n \sin^{-1}\left(\pm \frac{\sqrt{2}}{3}\right)\)
This matches the option \(x = \frac{\pi}{4} + (-1)^n \sin^{-1}\left(\pm \frac{\sqrt{2}}{3}\right)\).

The number of solutions of the equation $ \cos 2\theta \cos \left( \frac{\theta}{2} \right) + \cos \left( \frac{5\theta}{2} \right) = 2 \cos^3 \left( \frac{5\theta}{2} \right) $ in the interval \(\left[ -\frac{\pi}{2}, \frac{\pi}{2} \right ]\) is:
If $ \theta \in [-2\pi,\ 2\pi] $, then the number of solutions of $$ 2\sqrt{2} \cos^2\theta + (2 - \sqrt{6}) \cos\theta - \sqrt{3} = 0 $$ is:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure. 
The angular velocity of the system after the particle sticks to it will be: