A rigid body rotates about a fixed axis with a variable angular velocity equal to \(\alpha\) \(-\) \(\beta t\), at the time t, where \(\alpha , \beta\) are constants. The angle through which it rotates before it stops is:

1.	\(\frac{\left(\alpha\right)^{2}}{2 \beta}\)	2.	\(\frac{\left(\alpha\right)^{2} - \left(\beta\right)^{2}}{2 \alpha}\)
3.	\(\frac{\left(\alpha\right)^{2} - \left(\beta\right)^{2}}{2 \beta}\)	4.	\(\frac{\left(\alpha-\beta\right) \alpha}{2}\)

For the uniform T shaped structure, with mass 3M, the moment of inertia about an axis normal to the plane and passing through O would be

1.  $\frac{2}{3}{\mathrm{MI}}^2$

2.  ${\mathrm{MI}}^2$

3.  $\frac{{\mathrm{MI}}^2}{3}$

4.  None of these

A rigid body rotates with an angular momentum L. If its rotational kinetic energy is made 4 times, its angular momentum will become

1.  4L

2.  16L

3.  $\sqrt{2} \mathrm{L}$

4.  2L

Four particles of mass m₁ = 2m, m₂ = 4m, m₃ = m, and m₄ are placed at the four corners of a square. What should be the value of ${\mathrm{m}}_4$ so that the center of mass of all the four particles is exactly at the center of the square?

Angular momentum of a body is defined as the product of

1.  Mass and angular velocity

2.  Centripetal force and radius

3.  Linear velocity and angular velocity

4.  Moment of inertia and angular velocity

Two masses ${\mathrm{m}}_1 \mathrm{and} {\mathrm{m}}_2, {\mathrm{m}}_1 > {\mathrm{m}}_2$ are connected to the ends of massless rope and allowed to move as shown in the figure. The acceleration of the centre of mass assuming pulley is massless and frictionless, is

1.  $\frac{{\mathrm{m}}_1 - {\mathrm{m}}_2}{{\mathrm{m}}_1 + {\mathrm{m}}_2}\mathrm{g}$

2.  0

3.  ${\left(\frac{{\mathrm{m}}_1 - {\mathrm{m}}_2}{{\mathrm{m}}_1 + {\mathrm{m}}_2}\right)}^2\mathrm{g}$

4.  ${\left(\frac{{\mathrm{m}}_1 + {\mathrm{m}}_2}{{\mathrm{m}}_1 - {\mathrm{m}}_2}\right)}^2\mathrm{g}$

The speed of a uniform spherical shell after rolling down an inclined plane of vertical height h from rest is:

1.  \(\sqrt{\frac{10   g h}{7}}\)

2.    \(\sqrt{\frac{6   g h}{5}}\)

3.  \(\sqrt{\frac{4   g h}{5}}\)

4.  \(\sqrt{2   g h}\)

A uniform rod of mass m is bent into the form of a semicircle of radius R. The moment of inertia of the rod about an axis passing thorugh A and Perpendicular to the plane of paper is

1. $\frac{2}{3}M{R}^2$

2. $M{R}^2$

3. 2$M{R}^2$

4. $\frac{3}{2}M{R}^2$

A thin circular ring of mass M and radius r is rotating about its axis with a constant angular velocity $\omega$. Four objects each of mass m, are kept gently to the opposite ends of two perpendicular diameters of the ring. The angular velocity of the ring will be

1. $\frac{M\omega }{M+4m}$

2.$\frac{(M+4m)\omega }{M}$

3. $\frac{(M-4m)\omega }{M+4m}$

4. $\frac{M\omega }{4m}$

Let g be acceleration due to gravity on the surface of earth and T be the rotational kinetic energy of the earth. Suppose the earth's radius decreases by 2%. Keeping all other quantities same (even $\omega$)

1.  g decreases by 2% and T decreases by 4%

2.  g decreases by 4% and T decreases by 2%

3.  g increases by 4% and T decreases by 4%

4.  g decreases by 4% and T increases by 4%