To solve this problem, we need to determine the distance travelled by a solid cylinder rolling up an inclined plane. We'll take the following steps:
Step 1: Calculate Initial Kinetic Energy
The total initial kinetic energy for the rolling cylinder is the sum of its translational and rotational kinetic energy.
Translational kinetic energy, T_{KE} = \frac{1}{2} m v^2
Rotational kinetic energy, R_{KE} = \frac{1}{2} I \omega^2
For a solid cylinder, the moment of inertia, I = \frac{1}{2} m r^2 and the angular speed v = r \omega gives us \omega = \frac{v}{r}
Substituting these in, the total initial kinetic energy becomes:
E_{\text{initial}} = \frac{1}{2} m v^2 + \frac{1}{2} \left(\frac{1}{2} m r^2\right) \left(\frac{v}{r}\right)^2 = \frac{1}{2} m v^2 + \frac{1}{4} m v^2 = \frac{3}{4} m v^2
Given, m = 2 \text{ kg}, v = 4 \text{ m/s}, thus:
E_{\text{initial}} = \frac{3}{4} \times 2 \times 4^2 = \frac{3}{4} \times 2 \times 16 = 24 \text{ J}
Step 2: Equate Initial Energy to Potential Energy at the Highest Point
The potential energy at the highest point is U = mgh. Here, h is the height the cylinder reaches, and can be related to the distance d travelled along the incline by h = d \sin(\theta).
Equating gives us:
24 = 2 \times 10 \times d \sin(30^\circ)
The value of \sin(30^\circ) = \frac{1}{2}, so:
24 = 2 \times 10 \times d \times \frac{1}{2}
24 = 10d
Solve for d:
d = \frac{24}{10} = 2.4 \text{ m}
Thus, the distance travelled by the cylinder on the incline surface is 2.4 m.
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 