Given:
Mass of the flywheel, \( m = 20 \, {kg} \)
Radius, \( r = 100 \, {mm} = 0.1 \, {m} \)
Angular velocity, \( \omega = 600 \, {rpm} = \frac{600 \times 2\pi}{60} = 62.83 \, {rad/s} \)
Time to stop, \( t = 3.14 \, {s} \)
Coefficient of friction, \( \mu = 0.1 \)
Step 1: Calculate the angular deceleration (\( \alpha \)) The flywheel comes to rest in 3.14 s, so the angular deceleration is: \[ \alpha = \frac{\Delta \omega}{t} = \frac{0 - 62.83}{3.14} = -20 \, {rad/s}^2 \] The magnitude of angular deceleration is \( 20 \, {rad/s}^2 \).
Step 2: Calculate the torque (\( \tau \)) The torque required to stop the flywheel is: \[ \tau = I \alpha \] where \( I \) is the moment of inertia of the flywheel. For a solid disk: \[ I = \frac{1}{2} m r^2 = \frac{1}{2} \times 20 \times (0.1)^2 = 0.1 \, {kg m}^2 \] Thus, the torque is: \[ \tau = 0.1 \times 20 = 2 \, {Nm} \] Step 3: Calculate the frictional force (\( F \)) The torque is also given by: \[ \tau = F \cdot r \] Solving for \( F \): \[ F = \frac{\tau}{r} = \frac{2}{0.1} = 20 \, {N} \] However, considering the coefficient of friction \( \mu = 0.1 \), the normal force \( N \) required to produce this frictional force is: \[ F = \mu N \implies N = \frac{F}{\mu} = \frac{20}{0.1} = 200 \, {N} \] Thus, the force to be applied against the flywheel is 200 N.
Final Answer: 200 N
A force of 49 N acts tangentially at the highest point of a sphere (solid) of mass 20 kg, kept on a rough horizontal plane. If the sphere rolls without slipping, then the acceleration of the center of the sphere is
If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: