Answer:
[tex]v=\frac{2K}{RqB}[/tex]
[tex]m=\frac{(RqB)^2}{2K}[/tex]
Explanation:
The formula for kinetic energy K of a particle of mass m moving at velocity v is [tex]K=\frac{mv^2}{2}[/tex] and the formula for the Lorentz force F experimented by a particle of charge q and velocity v under a magnetic field B is (asuming v and B are perpendicular) [tex]F=qvB[/tex].
Since the particle would be moving in circles, this force would be a centripetal force given by [tex]F_{cp}=ma_{cp}=\frac{mv^2}{R}[/tex], where R is the radius of the trajectory.
Then we have (q, K, R and B would be what we know):
[tex]F=F_{cp}[/tex]
[tex]qvB=\frac{mv^2}{R}=\frac{2K}{R}[/tex]
[tex]v=\frac{2K}{RqB}[/tex]
And:
[tex]m=\frac{2K}{v^2}=\frac{2K(RqB)^2}{(2K)^2}=\frac{(RqB)^2}{2K}[/tex]