Question

(a) Show that the period of the circular orbit of a charged particle moving perpendicularly to a uniform magnetic field is $T = \dfrac{2 \pi m}{qB}$. (b) What is the frequency $f$? (c) What is the angular velocity $\omega$ ? Note that these results are independent of the velocity and radius of the orbit and, hence, of the energy of the particle. (Figure 22.64.)

Final Answer

- Please see the solution video.
- $\dfrac{qB}{2 \pi m}$
- $\dfrac{qB}{m}$

### Solution video

# OpenStax College Physics for AP® Courses, Chapter 22, Problem 80 (Problems & Exercises)

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Video Transcript

This is College Physics Answers with Shaun Dychko. In a cyclotron, a charged particle starts in the center with a little bit of velocity and then this magnetic field will cause it to go into a curve and then it gets accelerated across this gap between the Dees by this electric field so if it's a positively charged particle, it will get accelerated down here and then it will encounter this region where there is magnetic field causing it to move in a circular path again and then once it crosses this gap, it gets accelerated again but once it reaches here, the direction of this magnetic field or sorry the electric field in blue here will change because this is an alternating current voltage and so it gets accelerated upwards once it gets to this point and then it goes in a circle again and then the AC switches at the exact moment when the charged particle reaches this edge of the Dee and then the field will be pointing down, it gets accelerated faster still and its radius is increasing due to its increasing energy but its period and its frequency are remaining the same as we are going to derive here. So we are going to show that the period of one complete circle for a charged particle is 2

*π*times the particle's mass divided by its charge times the magnetic field strength. So speed of the particle is the distance it travels divided by time so period is the time it takes to travel one complete circle and so we have the circumference of a circle here— 2*π*times radius—divided by period and we can solve this for period then by multiplying both sides by period divided by speed. So period then is 2*πr*over*v*. And we can use this Lorentz Force formula for figuring out what*v*is. So the Lorentz force is providing the centripetal force, which is*mv squared*over*r*for any particle moving in a circle with no tangental acceleration. So we have mass of the particle times its speed squared divided by*r*is the charge times its speed times magnetic field strength and we can solve this for*v*by multiplying both sides by*r*over*m*and then also divide both sides by*v*. So we have*v*to the power of 1 on the left equals*qBr*over*m*and that we can substitute in for*v*here and so we are having 2*πr*divided by this fraction but dividing by a fraction I find more easy to express as multiplying by its reciprocal because I don't like to have fractions within fractions. So we have 2*πr*multiplied by the flipped version of this it's the reciprocal in other words,*m*over*qBr*, the*r*'s cancel leaving us with 2*π*times mass divided by charge times magnetic field strength and this is what we wanted to show that the period of making one complete circle for a charge particle in this cyclotron is 2*π*times its mass divided by its charge times magnetic field. Frequency is the reciprocal of period so we just flip this fraction*qB*over*2πm*and then in part (c), we are asked to find the angular velocity and so it does one complete circle, which has 2*π*radians in an amount of time equal to the period because that's what period is in this case, the time it takes to do one complete cycle, which is a circle. And so we have 2*π*divided by period and that is 2*π*times the reciprocal of this so 2*π*times*qB*over 2*πm*and this works out to*qB*over*m*. So the angular velocity depends only on the charge, the magnetic field strength and the mass.