1. | \(5:2\) | 2. | \(3:5\) |
3. | \(5:3\) | 4. | \(2:5\) |
1. | \(1:\sqrt{2}\) | 2. | \(2:1\) |
3. | \(\sqrt{2}:1\) | 4. | \(4:1\) |
The ratio of the moments of inertia of two spheres, about their diameters, having the same mass and their radii being in the ratio of \(1:2\), is:
1. | \(2:1\) | 2. | \(4:1\) |
3. | \(1:2\) | 4. | \(1:4\) |
From a circular ring of mass \({M}\) and radius \(R\), an arc corresponding to a \(90^\circ\)sector is removed. The moment of inertia of the remaining part of the ring about an axis passing through the centre of the ring and perpendicular to the plane of the ring is \(K\) times \(MR^2\). The value of \(K\) will be:
1. | \(\dfrac{1}{4}\) | 2. | \(\dfrac{1}{8}\) |
3. | \(\dfrac{3}{4}\) | 4. | \(\dfrac{7}{8}\) |
Point masses \(m_1\) and \(m_2\), are placed at the opposite ends of a rigid rod of length \(L\) and negligible mass. The rod is set into rotation about an axis perpendicular to it. The position of point \(P\) on this rod through which the axis should pass so that the ork required to set the rod rotating with angular velocity is minimum is given by:
1. | \(x = \frac{m_1L}{m_1+m_2}\) | 2. | \(x= \frac{m_1}{m_2}L\) |
3. | \(x= \frac{m_2}{m_1}L\) | 4. | \(x = \frac{m_2L}{m_1+m_2}\) |
Three identical spherical shells, each of mass \(m\) and radius \(r\) are placed as shown in the figure. Consider an axis \(XX'\), which is touching two shells and passing through the diameter of the third shell. The moment of inertia of the system consisting of these three spherical shells about the \(XX'\) axis is:
1. | \(\frac{11}{5}mr^2\) | 2. | \(3mr^2\) |
3. | \(\frac{16}{5}mr^2\) | 4. | \(4mr^2\) |
The moment of inertia of a uniform circular disc is maximum about an axis perpendicular to the disc and passing through:
1. \(C\)
2. \(D\)
3. \(A\)
4. \(B\)