To find the interval where \( f(x) = \tan^{-1}(\sin x + \cos x) \) is increasing, we need to find where the derivative \( f'(x) \) is positive. Let us first differentiate \( f(x) \). The derivative of \( \tan^{-1}(y) \) with respect to \( x \) is: \[ f'(x) = \frac{1}{1 + y^2} \cdot \frac{dy}{dx} \] where \( y = \sin x + \cos x \). Now, differentiate \( y = \sin x + \cos x \): \[ \frac{dy}{dx} = \cos x - \sin x \] Thus, the derivative of \( f(x) \) is: \[ f'(x) = \frac{\cos x - \sin x}{1 + (\sin x + \cos x)^2} \] For \( f(x) \) to be increasing, we need \( f'(x)>0 \). This requires: \[ \cos x - \sin x>0 \] which simplifies to: \[ \cos x>\sin x \] This inequality holds for: \[ x \in \left( -\frac{\pi}{2}, \frac{\pi}{4} \right) \] Thus, the function is increasing in the interval \( \left( -\frac{\pi}{2}, \frac{\pi}{4} \right) \), which is the correct answer.
Thus, the correct answer is \( \left( -\frac{\pi}{2}, \frac{\pi}{4} \right) \).
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: