To determine the velocity of the center of mass of the sphere, we start by noting the following: For a solid sphere rolling without slipping, the total kinetic energy is the sum of translational and rotational kinetic energy. Given the kinetic energy \(K = 2240 \, \text{J}\), we can express it as:
\(K = \frac{1}{2}mv^2 + \frac{1}{2}I\omega^2\)
For a solid sphere, the moment of inertia \(I\) about its center is \(\frac{2}{5}mr^2\). Also, for pure rolling, the relation between linear velocity \(v\) and angular velocity \(\omega\) is \(v = r\omega\).
Thus, the rotational kinetic energy can be rewritten as:
\(\frac{1}{2}I\omega^2 = \frac{1}{2} \times \frac{2}{5}mr^2 \times \left(\frac{v}{r}\right)^2 = \frac{1}{5}mv^2\)
Substituting these into the kinetic energy equation, we get:
\(K = \frac{1}{2}mv^2 + \frac{1}{5}mv^2 = \frac{7}{10}mv^2\)
Given \(K = 2240 \, \text{J}\) and \(m = 2 \, \text{kg}\), we solve for \(v\):
\(2240 = \frac{7}{10} \times 2 \times v^2\)
\(2240 = \frac{14}{10}v^2\)
\(2240 \times \frac{10}{14} = v^2\)
\(v^2 = 1600\)
\(v = \sqrt{1600} = 40 \, \text{ms}^{-1}\)
Thus, the velocity of the center of mass of the sphere is \(40 \, \text{ms}^{-1}\). This solution is consistent with the expected range of 40 to 40, confirming its accuracy.