To solve this problem, we need to consider the physics of rotational motion and the relationship between the tension, radius, and kinetic energy of the rotating mass.
First, let's understand the mechanics involved:
According to the principle of conservation of angular momentum:
m v_1 r_1 = m v_2 r_2
Here, when the radius r is reduced to half, r_2 = \frac{r_1}{2}, we have:
v_2 = \frac{v_1 r_1}{r_2} = \frac{v_1 r_1}{\frac{r_1}{2}} = 2v_1
This means that the new tangential velocity becomes twice the original velocity.
Substituting this into the kinetic energy formula gives us:
K_2 = \frac{1}{2} m (2v_1)^2
K_2 = 2^2 \times \frac{1}{2} m v_1^2 = 4 K_1
This results in the kinetic energy increasing by a factor of 4.
Thus, the correct answer is: increase by a factor of 4.
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 