To solve this problem, we need to determine the tension in the string that produces an angular acceleration of 2 revolutions per second squared in the solid cylinder.
\text{Angular acceleration, } \alpha = 2 \times 2\pi = 4\pi \, \text{rad/s}^2
I = \frac{1}{2} m r^2
Where:
Substituting the values, we get:
I = \frac{1}{2} \times 50 \times (0.5)^2 = \frac{1}{2} \times 50 \times 0.25 = \frac{1}{2} \times 12.5 = 6.25 \, \text{kg m}^2
\tau = I \alpha
Substitute the values:
\tau = 6.25 \times 4\pi = 25\pi \, \text{Nm}
\tau = T \cdot r
Solving for tension (T), we have:
T = \frac{\tau}{r} = \frac{25\pi}{0.5} = 50\pi \, \text{N}
Approximating \pi \approx 3.14, the tension becomes:
T \approx 50 \times 3.14 = 157 \, \text{N}
The correct answer is therefore 157 N.
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 