To solve the problem of finding the work done to stop a solid circular disc rolling on a floor, we need to consider both its translational and rotational kinetic energy. The total kinetic energy \(KE\) of the disc can be expressed as:
where \(m = 50 \, \text{kg}\) is the mass of the disc, \(v = 0.4 \, \text{m/s}\) is the speed of the center of mass, \(I\) is the moment of inertia, and \(\omega\) is the angular velocity.
For a solid disc, \(I = \frac{1}{2} m r^2\), and since the disc rolls without slipping, \(\omega = \frac{v}{r}\).
Substituting \(\omega\) and \(I\), we find:
The total kinetic energy is the sum of translational and rotational components:
\(KE = \frac{1}{2}mv^2 + \frac{1}{4}mv^2 = \frac{3}{4}mv^2\)
Substituting the known values:
\(KE = \frac{3}{4} \times 50 \times (0.4)^2 = 6 \, \text{J}\)
Hence, the work done to stop the disc (which is equal to the reduction in total kinetic energy) is \(6 \, \text{J}\). This value matches the expected range \([6,6]\).
Using the work-energy theorem:
\[ W = \Delta KE = 0 - \left( \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2 \right) \]
Since the disc rolls without slipping, we use:
\[ I = \frac{K^2}{R^2} \]
Thus:
\[ W = 0 - \frac{1}{2}mv^2 \left( 1 + \frac{K^2}{R^2} \right) \]
Substituting the values:
\[ W = -\frac{1}{2} \times 50 \times 0.4^2 \left( 1 + \frac{1}{2} \right) = -6J \]
Therefore, the absolute value of work is:
\[ |W| = 6J \]
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).

Nature of compounds TeO₂ and TeH₂ is___________ and ______________respectively.