Question

FIGURE 2 shows a constant force, F of magnitude 20N pulled a light cord wrapped around a pulley to lift a bucket of mass 1.53kg. The radius and the moment of inertia of the pulley are 0.330m and 0.385kg m² respectively. If the frictional torque is 1.10Nm calculate the

(a) angular acceleration of the pulley. (b) linear acceleration of the bucket​

Answer 1

(a) $14.3 rad/s^2$

The angular acceleration of the pulley can be found by using the equivalent of Newton's second law for rotational motions:

$\tau = I \alpha$ (1)

where

$\tau$ is the net torque on the pulley

$I=0.385 kg m^2$ is the moment of inertia of the pulley

$\alpha$ is the angular acceleration

First, we need to find the net torque. The torque exerted by the force F (forward) is:

$\tau_t = F r = (20 N)(0.330 m)=6.6 Nm$

While the frictional torque (backward) is $\tau_f = 1.1 Nm$. So, the net torque is

$\tau = \tau_t - \tau_f=6.6 - 1.1 = 5.5 Nm$

Now, re-arranging eq.(1), we find the angular acceleration:

$\alpha = \frac{\tau}{I}=\frac{5.5}{0.385}=14.3 rad/s^2$

(b) $4.72 m/s^2$

Assuming that the string holding the bucket is inextensible, the bucket should have the same linear acceleration of a point on the edge of the pulley, which is given by

$a= \alpha r$

where

$\alpha=14.3 rad/s^2$ is the angular acceleration

r = 0.330 m is the radius of the pulley (the distance of a point at the edge from the centre)

Substituting into the equation, we find

$a=(14.3)(0.330)=4.72 m/s^2$