Solve Cyclotron Question: Calculate Magnetic Field & Time to Exit

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In summary, a cyclotron with a maximum chamber radius of 110 cm can accelerate ##_{4}^{2+}He## (alpha particles) up to an energy of 140 MeV. To calculate the required magnetic field, the relativistic calculation should be used as the speed of the particle is close to 30% of the speed of light. The calculated magnetic field of 1.55T is quite high and not easy to produce uniformly over the cyclotron. To determine the time from emission from the source to exiting the cyclotron, the number of half turns can be calculated, which is approximately 22666 turns. This results in a time on the order of a millisecond, which seems very fast.
  • #1
CAF123
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Homework Statement



If a cyclotron with a maximum chamber radius of 110 cm can accelerate ##_{4}^{2+}He##, (alpha particles) up to a energy of 140 MeV, calculate

A) The magnetic field and comment on your answer.

If the accelerating voltage is 3 kV and the source of alpha particle is from a radioactive source that emits alpha particles with an energy of 4MeV, calculate

B) time from emission from the source to exiting the cyclotron.

The Attempt at a Solution


A)Max energy of the alpha particles: 140 MeV, which means ##v = \sqrt{2E/m} \approx 8.2 \times 10^{7}m/s > 0.1c## Should I be doing a relativistic calculation?

The cyclotron moves a particle in a circular fashion, so F points towards the centre and v tangential => B is into the page with magnitude mv/qR = 1.55T.

It says I should comment on this - perhaps something like the B field is strong enough that the particle is accelerated to a speed closer than 10% of the speed of light?

B) Total energy: 4Mev + qV = E => v ≈ 1.4 x 107m/s > 0.1c. Proceeding gives ##T = 2 \pi R/v = 4.9 \times 10^{-7} s##. I feel this may be incorrect because I don't think I have taken into account how a cyclotron actually works.

Many thanks.
 
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  • #2
CAF123 said:
A)Max energy of the alpha particles: 140 MeV, which means ##v = \sqrt{2E/m} \approx 8.2 \times 10^{7}m/s > 0.1c## Should I be doing a relativistic calculation?
With a speed close to 30% c, I would do the relativistic calculation. I think it will make about a 4% difference in your answer.
The cyclotron moves a particle in a circular fashion, so F points towards the centre and v tangential => B is into the page with magnitude mv/qR = 1.55T.
If you want to include relativistic effects, then mv should be replaced by the relativistic momentum. [EDIT: Looks like you're off by a factor of 2 somehow in the calculation, but the formula is basically correct except for using the relativistic momentum.] [Edit #2: My mistake, you're not off by a factor of 2.]
B) Total energy: 4Mev + qV = E => v ≈ 1.4 x 107m/s > 0.1c. Proceeding gives ##T = 2 \pi R/v = 4.9 \times 10^{-7} s##. I feel this may be incorrect because I don't think I have taken into account how a cyclotron actually works.
You'll need to read up a bit on how the cyclotron works. T is the time for one orbit, but the ion will make many orbits before reaching 140 MeV. See http://en.wikipedia.org/wiki/Cyclotron
 
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  • #3
Hi TSny,

So the angular frequency of the particle is ##\omega = 2 \pi f \Rightarrow T = \frac{2 \pi}{\omega} = 2 \pi \frac{m}{qB}##.

The ion starts with an initial energy of 4 MeV and every half turn it is accelerated by 3kV. We want to know how many times the particle has to go around the circle until its energy is 140MeV. So I then set up a linear eqn:$$4MeV + x(3kV q) = 140MeV \Rightarrow x = 45333 $$ This is the approximate number of half turns. To get the number of full turns, divide by 2 to get approx 22666 turns.

So I should multiply the result above for T by 22666 and I attain an answer of the order of a millisecond. This seems very fast!

Many thanks.
 
  • #4
That all looks good. (It was my mistake earlier when I thought you were off by a factor of 2 in B.)
 
  • #5
Thanks TSny,
For part 1), I was asked to comment about my answer of 1.55T. What can I say? The only thing I can think of is that we are nearing the case where we would have to apply relativistic calculations. (since a particle in a B field producing that strength of teslas has an energy such that it's ejection speed is close to c).
 
  • #6
I'm not sure what the question is getting at here. The energy of the ion depends on both B and R, so a large B doesn't necessarily imply large energy if R is small. Perhaps they just want you to note that 1.55 T is a large magnetic field that is not easy to produce uniformly over the cyclotron. I don't know. [See http://en.wikipedia.org/wiki/Magnetic_field#Measurement for largest B field produced in lab.]
 
  • #7
Maybe they just want us to note that 1.55T is quite a high strength field.
Thank you TSny.
 

FAQ: Solve Cyclotron Question: Calculate Magnetic Field & Time to Exit

1. What is a cyclotron?

A cyclotron is a type of particle accelerator that uses a magnetic field and an electric field to accelerate charged particles. It is commonly used in scientific research to study the properties and behavior of particles.

2. How do you calculate the magnetic field in a cyclotron?

The magnetic field in a cyclotron can be calculated using the formula B = mv/(qR), where B is the magnetic field, m is the mass of the particle, v is the velocity, q is the charge of the particle, and R is the radius of the cyclotron.

3. What factors affect the time it takes for a particle to exit a cyclotron?

The time it takes for a particle to exit a cyclotron is affected by the strength of the magnetic field, the velocity of the particle, and the radius of the cyclotron. It is also influenced by the mass and charge of the particle being accelerated.

4. How can I use the calculated magnetic field and time to exit to optimize the performance of a cyclotron?

By accurately calculating the magnetic field and time to exit, scientists can adjust the strength of the magnetic field and the size of the cyclotron to optimize the performance of the cyclotron. This allows for efficient and precise acceleration of particles.

5. What are some real-world applications of cyclotrons?

Cyclotrons have a wide range of applications in scientific research, medical imaging, and cancer treatment. They are used to produce and study radioactive isotopes for medical imaging and in the production of radiopharmaceuticals for cancer treatment. They are also used in particle physics experiments to study the fundamental properties of particles.

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