91Ó°ÊÓ

Time spent by the particle is $130\text{ }ns=1.30×{10}^{−7}\text{ }s$

We have to use the formula for magnetic force and centrifugal force to find the magnetic field.Also, we need to express the period in terms of the magnetic field to determine the time spent by a particle in the region.

Formula:

$F_m=qVB$

$F_c=\frac{m{v}^2}{r}$

The particle is pointing downward while entering the magnetic field, and the direction of the magnetic field is out of the page, as shown in the figure. So, according to the right-hand rule,$\stackrel{→}{v}×\stackrel{→}{B}$

points towards the left. As this is the direction of a charged particle, we can conclude that the particle has a positive charge. Hence, it is a proton.

Now, we have:

$\begin{array}{c}qvB=\frac{m{v}^2}{r}\\ qB=m\mathrm{Ó\neg }\\ \mathrm{Ó\neg }=\frac{qB}{m}\\ \frac{2\mathrm{Ï€}}{T}=\frac{qB}{m}\end{array}$

So,

$B=\frac{2\mathrm{Ï€}m}{qT}$

Here, T is the period given by:

,

$T=2×t=2×1.30×{10}^{−7}\text{ s}$

So, Magnetic force can be calculated as:

$\begin{array}{c}B=\frac{2\mathrm{π}×1.67×{10}^{−27}}{2×1.6×{10}^{−19}×1.30×{10}^{−7}}.\\ =0.252\text{ }T\end{array}$

Thus, the magnitude of the magnetic field is $0.252T$.

We have the equation for the time period as follows:

$T=\frac{2\mathrm{Ï€}m}{qB}$

This shows that period does not depend on speed, so it will remain thesame even though kinetic energy is double.

Therefore, time spent in the magnetic field region will remain .$130\text{ }ns$$130\text{ }ns$