To determine the work required to halt a solid circular disc rolling on a surface, we must account for its linear and angular kinetic energies. The total kinetic energy (\(KE\)) is given by:
Here, \(m = 50 \, \text{kg}\) represents the disc's mass, \(v = 0.4 \, \text{m/s}\) is the speed of its center of mass, \(I\) denotes the moment of inertia, and \(\omega\) is the angular velocity.
For a solid disc, the moment of inertia is \(I = \frac{1}{2} m r^2\). Assuming no-slip rolling, the angular velocity is related to linear velocity by \(\omega = \frac{v}{r}\).
Substituting these expressions yields:
The total kinetic energy is the sum of these two components:
\(KE = \frac{1}{2}mv^2 + \frac{1}{4}mv^2 = \frac{3}{4}mv^2\)
Plugging in the given values:
\(KE = \frac{3}{4} \times 50 \times (0.4)^2 = 6 \, \text{J}\)
Therefore, the work done to stop the disc, equivalent to the change in its total kinetic energy, is \(6 \, \text{J}\). This result falls within the expected range of \([6,6]\).
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).