The radius \( r \) of the circular path of a charged particle moving in a magnetic field is given by:
\[
r = \frac{mv}{qB}
\]
where \( m \) is the mass of the particle, \( v \) is its velocity, \( q \) is the charge, and \( B \) is the magnetic field.
When the particle loses half of its kinetic energy, its velocity \( v \) changes because kinetic energy \( K.E. = \frac{1}{2} mv^2 \). If the kinetic energy is halved, then the new velocity \( v' \) will be:
\[
v' = \frac{v}{\sqrt{2}}
\]
Since the radius is directly proportional to the velocity, the new radius \( r' \) is:
\[
r' = \frac{m v'}{qB} = \frac{m}{qB} \cdot \frac{v}{\sqrt{2}} = \frac{r}{\sqrt{2}}
\]
Thus, the radius of the path decreases by a factor of \( \sqrt{2} \).
The time period \( T \) of revolution is given by:
\[
T = \frac{2 \pi r}{v}
\]
Since the radius decreases by a factor of \( \sqrt{2} \) and the velocity also decreases by a factor of \( \sqrt{2} \), the time period will not change because both the radius and the velocity decrease by the same factor. Therefore, the time period remains the same.
Thus:
1. The radius of the path decreases by a factor of \( \sqrt{2} \).
2. The time period of revolution remains unchanged.