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 \( 2\cos(\theta) \).
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:
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: