Magnetic Fields and Proton Beam therapy

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SUMMARY

Proton Beam therapy utilizes high-energy proton beams to target tumors, with protons traveling at a speed of 1.8 x 10^8 m/s. The magnetic field required to deflect these protons by 90 degrees in a circular arc of radius 4.0 m can be calculated using the formula B = uI/2(pi)r. The torque measured on a square coil of side 0.2 m, which was parallel to the magnetic field, was found to be 0.15 N.m, indicating the need to determine the current flowing through the coil to complete the analysis.

PREREQUISITES
  • Understanding of Proton Beam therapy and its applications in cancer treatment.
  • Familiarity with magnetic fields and their role in particle acceleration.
  • Knowledge of torque calculations in magnetic fields.
  • Basic principles of centripetal force and its relation to circular motion.
NEXT STEPS
  • Learn how to calculate magnetic fields using the Lorentz force equation F = BIL.
  • Research the principles of centripetal force in the context of charged particles in magnetic fields.
  • Study the effects of relativistic speeds on particle behavior in magnetic fields.
  • Explore the design and function of proton accelerators used in medical applications.
USEFUL FOR

Medical physicists, engineers involved in proton therapy systems, and students studying advanced physics concepts related to magnetism and particle acceleration.

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Proton Beam therapy is an advanced technique to destroy tumors by concentrating a high energy beam of protons to a specific depth inside the body of a patient. These proton beams are produced by accelerators and steered to the patient-treatment rooms by magnets. In a particular cancer treatment center, the speed of the protons is 1.8 x 10^8 m/s. In a particular arrangement, the proton beam is deflected by 90 degrees with respect to its initial direction by a constant magnetic field.

a) If the radius of the circular arc of the trajectory is 4.0 m, find the magnitude of the constant magnetic field.

b) The engineers who installed these magnets tested the magnetic field by inserting a single square coil of side .2 m. The plane of the coil was made parallel to the field lines. They measured the torque on this coil when it carried a current. They found th torque to be .15 N.m for the magnetic field you found in part (a). What was the current in the square coil?

For part A, I know I can use the equation:

B = uI/2(pi)r

Plug in what I know, I end up with :

B = 4(pi)x10^-7 (I) / 2(Pi)(4.0m)

or

2 (pi) x 10^-7 (I) / 4.0 m

However I am unsure what the current is and therefore, do not know what to plug in for I.
 
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B = uI/2(pi)r only applies to an infinitely long current-carrying wire. Here, you have to derive the equation yourself. What's the centripetal force equal to? What is it applied by? Also, since 1.8E8 m/s is more than half the speed of light, do you need to take into consideration relativistic effects?
 
We've never talked about centripetal force in class so I doubt that the answer is related to that.

I do not believe we have to take into consideration relativistic effects.

Would a formula like F= BIL be more effective? The current seems to be the missing link in all the magnetic field equations given.

Thank you for your reply.
 

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