Diverting a beam of charged particles using M.F.

In summary, the problem involves a beam of charged particles with a kinetic energy of 1keV and a charge of 1.6 x 10^-19 C. The particles, with masses of 8 x 10^-22kg and 16 x 10^-27kg, are emitted from an accelerator tube and strike a plate at a distance of 1cm from the end of the tube. The smallest magnetic field that can prevent the beam from striking the plate is given by Bmin = √(2mK.E.)/qr, where r = 1cm. On solving, the value of Bmin is found to be √(m x 1.1 x 10^13). However,
  • #1
zorro
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Homework Statement


A beam of charged particles of K.E. = 1keV and q=1.6 x 10-19 C and 2 masses 8 x 10-22kg and 16 x 10-27kg come out of an accelerator tube and strike a plate at a distance of 1cm from the end of the tube, where the particles emerge perpendicularly. Find the value of the smallest magnetic field which can prevent the beam from striking the plate.


The Attempt at a Solution



Bmin = √(2mK.E.)/qr where r=1cm

On solving, I got
Bmin as √m x 1.1 x 1013
Now the min. value of magnetic field will be the one which can just divert the heavier particles.
So m = 8 x 10-22kg which gives Bmin as 311.1 T

The answer given is 1.414 T which is found by substituting m as 16 x 10-27kg
I don't understand how this is possible.
Is the answer wrong?
Please help!
 
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  • #2
Your method looks good, though the question is not all that clear without a diagram. It sure looks like the masses got garbled when the question was typed. 8 x 10^-27kg and 16 x 10^-27kg would make a lot more sense and lead to the given answer.
 
  • #3
Yes you are right. Thanks!
 

1. How does diverting a beam of charged particles using M.F. work?

Diverting a beam of charged particles using M.F. (magnetic field) involves applying a magnetic field to the path of the beam, causing the charged particles to change direction due to the Lorentz force. The strength and direction of the magnetic field can be manipulated to control the trajectory of the particles.

2. What are the applications of diverting a beam of charged particles using M.F.?

The ability to manipulate charged particle beams using M.F. has many applications in various fields of science and technology. Some examples include particle accelerators for high-energy physics research, ion implantation in semiconductor manufacturing, and focusing and steering of electron beams in cathode ray tubes.

3. Are there any challenges in diverting a beam of charged particles using M.F.?

Yes, there are several challenges in diverting a beam of charged particles using M.F. One of the main challenges is maintaining a stable and uniform magnetic field, as any fluctuations or variations can affect the trajectory of the particles. Additionally, controlling and adjusting the magnetic field to precisely guide the particles can be a complex task.

4. Can different types of charged particles be diverted using M.F.?

Yes, M.F. can be used to divert a wide range of charged particles, including electrons, protons, ions, and even heavier particles such as alpha particles. The strength and direction of the magnetic field may need to be adjusted for different types of particles to ensure proper diversion.

5. Are there any safety concerns when working with M.F. to divert charged particles?

Yes, there are potential safety concerns when working with M.F. to divert charged particles. The magnetic fields used can be very strong, so precautions must be taken to avoid any harm to individuals or equipment. Additionally, the charged particles themselves can be hazardous, so proper handling and containment measures should be in place to ensure safety.

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