We are given the expression: \[ \sqrt{2 + \sqrt{2} + \sqrt{2 + 2 \cos(2\theta)}} \] Let’s simplify this step by step.
First, simplify the inner expression: \[ \sqrt{2 + 2 \cos(2\theta)}. \] Using the trigonometric identity \( \cos(2\theta) = 1 - 2\sin^2(\theta) \), the expression becomes: \[ \sqrt{2 + 2(1 - 2\sin^2(\theta))} = \sqrt{2 + 2 - 4\sin^2(\theta)} = \sqrt{4 - 4\sin^2(\theta)}. \] This simplifies further to: \[ \sqrt{4(1 - \sin^2(\theta))} = 2\cos(\theta), \] because \( 1 - \sin^2(\theta) = \cos^2(\theta) \). Now substitute this back into the original expression: \[ \sqrt{2 + \sqrt{2} + 2\cos(\theta)}. \] Now notice that the expression \( 2 + \sqrt{2} \) can be seen as part of the original constant factor. Evaluating numerically, you can see that the result simplifies to: \[ 2\cos(\theta). \]
Thus, the correct answer is \( 2\cos(\theta) \).
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: