
Since the path of the proton (positive charge) curves to the left, the magnetic force is directed toward the center of curvature. Using the right-hand rule with velocity tangents, we find:
Since: \[ r = \frac{mv}{qB} \Rightarrow B \propto \frac{1}{r} \] The smaller the radius of curvature, the stronger the magnetic field.
Looking at the image:
A proton (positive charge) moves with velocity $\vec v$ in a non-uniform magnetic field and its path (always in the plane of the paper) is curved. Magnetic force is the centripetal force that bends the proton’s path: $$\vec F = q(\vec v\times\vec B).$$
For a charged particle moving perpendicular to a magnetic field the radius of curvature $r$ is $$r=\dfrac{mv}{qB}\quad\Rightarrow\quad B=\dfrac{mv}{q\,r}.$$ With the proton’s mass $m$, charge $q$ and speed $v$ (given) essentially the same at those nearby points, the magnetic field strength is inversely proportional to the local radius of curvature: $B\propto 1/r$.
From the figure the curvature radii satisfy (smallest curvature radius at Q, larger at R, largest at P) — therefore $$B_Q > B_R > B_P.$$
Direction: $\vec B$ is into the page at P, Q and R.
Relative magnitudes: $\displaystyle B_Q > B_R > B_P.$

“One of these days you’re going to talk yourself into a load of trouble,” her father said aggressively. What do you learn about Sophie’s father from these lines? (Going Places)
Write a letter to the editor of a local newspaper expressing your concerns about the increasing “Pollution levels in your city”. You are an environmentalist, Radha/Rakesh, 46, Peak Colony, Haranagar. You may use the following cues along with your own ideas: 