Answer: a) (2)^1/2*rp; b) ra= (2)^1/2*rp
Explanation: In order to explain this problem we have to consirer a circular motion for charged particles with velocity in a magnetic field.
The we know that:
the Ek=q*V=1/2*m*v^2 then
v=(2*q*V/m)^1/2
The magnetic force when v is perpendicular to B, is equal
Fm=q*v*B
when the charged particle is moving a circular motion, we have:
Fm=m*ac where ac is the centripetal acceleration which is equal,
ac=v^2/R where R is the radius of the circular trajectory.
Finally we obtain;
q*v*B=m*v^2/R
R=m*v/(q*B) using that v= (2*q*V/m)^1/2
we have; R=(1/B)*(2*V*m/q)^1/2
For a proton we have
rp=(1/B)* (2*V*mp/e)^1/2
For a deuteron ( charge +e and mass 2mp)
rd=(1/B)* (2*V*2*mp/e)^1/2=(1/B)*(4*V*mp/e)^1/2=(2)^1/2*rp
For a alpha particle ( charge +2e, mass 4mp) =
ra=(1/B)*(2*V*4*mp/2*e)^1/2=(1/B)*(4*V*mp/e)^1/2=(2)^1/2*rp