To determine which cylinder will reach the bottom of an inclined plane first, we need to consider the rotational dynamics of both the solid cylinder and the hollow cylinder, both of which roll down without slipping.
The time it takes for each cylinder to reach the bottom of the incline depends on its moment of inertia and how it converts its potential energy into translational and rotational kinetic energy. The potential energy at the top is entirely converted to kinetic energy at the bottom.
The moment of inertia I for each cylinder type is as follows:
Using the principle of conservation of energy:
Potential energy at the top = Total kinetic energy at the bottom
mgh = \frac{1}{2} mv^2 + \frac{1}{2} I \omega^2
Where \omega = \frac{v}{r} is the angular velocity and v is the linear velocity.
For the solid cylinder, substituting the value of I:
mgh = \frac{1}{2} mv^2 + \frac{1}{2} \left(\frac{1}{2} m r^2\right) \left(\frac{v}{r}\right)^2
Simplifying, we find:
mgh = \frac{3}{4} mv^2
Thus, v = \sqrt{\frac{4}{3}gh}
For the hollow cylinder:
mgh = \frac{1}{2} mv^2 + \frac{1}{2} (m r^2) \left(\frac{v}{r}\right)^2
Simplifying, we find:
mgh = mv^2
Thus, v = \sqrt{gh}
Comparing the two results, the linear velocity of the solid cylinder (\sqrt{\frac{4}{3}gh}) is greater than that of the hollow cylinder (\sqrt{gh}). Therefore, since the solid cylinder has a greater acceleration and hence velocity, it will reach the bottom of the incline first.
Conclusion: The solid cylinder will reach the bottom of the inclined plane before the hollow cylinder.
The center of mass of a thin rectangular plate (fig - x) with sides of length \( a \) and \( b \), whose mass per unit area (\( \sigma \)) varies as \( \sigma = \sigma_0 \frac{x}{ab} \) (where \( \sigma_0 \) is a constant), would be 