The moment of inertia \(I\) for a solid cone with mass \(M\) and base radius \(R\) about its central axis of symmetry is \( I = \frac{3}{10}MR^2 \). This result from classical mechanics is obtained by integrating the moments of inertia of constituent infinitesimal circular disks, where a disk of mass \(dm\) and radius \(r\) has a moment of inertia of \(\frac{1}{2}r^2 dm\).