The given function is: \[ f(x) = a - (x - 3)^{8/9} \] where \( a \) is a constant, and \( (x - 3)^{8/9} \) represents a fractional power of \( x - 3 \).
To find the maxima or minima of \( f(x) \), we need to first find the derivative \( f'(x) \) and set it equal to zero. The derivative of \( f(x) = a - (x - 3)^{8/9} \) is: \[ f'(x) = - \frac{8}{9} (x - 3)^{-1/9} \]
Set the derivative equal to zero to find critical points: \[ f'(x) = - \frac{8}{9} (x - 3)^{-1/9} = 0 \] This equation will never be equal to zero because \( (x - 3)^{-1/9} \) is never zero for any \( x \neq 3 \). Therefore, the function does not have any critical points where the derivative is zero.
The function involves a fractional power, so we need to check the behavior of \( f(x) \) near \( x = 3 \), where the term \( (x - 3)^{8/9} \) becomes zero. - For \( x = 3 \), we have: \[ f(3) = a - (3 - 3)^{8/9} = a - 0 = a \] - As \( x \to 3^+ \) (approaching 3 from the right), \( (x - 3)^{8/9} \) increases as \( x \) increases slightly from 3. - As \( x \to 3^- \) (approaching 3 from the left), \( (x - 3)^{8/9} \) also increases. Therefore, \( f(x) \) is decreasing for both \( x > 3 \) and \( x < 3 \), and the maximum occurs at \( x = 3 \).
The maximum value of \( f(x) \) occurs at \( x = 3 \), and the maximum value is \( f(3) = a \).
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: