Cathode Ray Tube Magnetic Question

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SUMMARY

The discussion focuses on the behavior of an electron in a cathode ray tube subjected to a magnetic field of 6.0 x 10-4 tesla. The magnetic force acting on the electron is calculated using the formula F = qvBsinθ, where θ is determined to be 90 degrees, resulting in a force of 1.92 x 10-16 N. The radius of curvature of the electron's path is found to be 0.1898 m using the formula r = (mv)/(qB). To achieve no deflection, an electric field must be established in the opposite direction, which can be calculated as E = F/q.

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  • Understanding of electromagnetism principles, specifically Lorentz force.
  • Familiarity with the right-hand rule for determining magnetic field direction.
  • Knowledge of basic physics equations related to force and motion.
  • Ability to perform calculations involving electric and magnetic fields.
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  • Learn about the Lorentz force and its applications in particle physics.
  • Study the relationship between electric and magnetic fields in electromagnetic theory.
  • Explore the concept of centripetal force in the context of charged particles in magnetic fields.
  • Investigate the design and function of cathode ray tubes in electronic devices.
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Homework Statement



The figure from the link below shows a cross section of a cathode ray tube. An electron in the tube initially moves horizontally in the plane of the cross section at a speed of 2.0 x 107 meters per second. The electron is deflected upward by a magnetic field that has a field strength of 6.0 x 10-4 tesla.
a. What is the direction of the magnetic field?
b. Determine the magnitude of the magnetic force acting on the electron.
c. Determine the radius of curvature of the path followed by the electron while it is in the magnetic field.

An electric field is later established in the same region as the magnetic field such that the electron now passes through the magnetic and electric fields without deflection.
d. Determine the magnitude of the electric field.
e. What is the direction of the electric field?

I found the picture at this link on page 6: harmonphys.info/magnetism%20problems.doc

Homework Equations


F = qvBsin\theta

r = (mv)/(qB)

The Attempt at a Solution



a) It is directed out of the page by the right hand rule. (Did I do this properly?)

b) F = qvBsin\theta
F = (1.60*10^(-19) C)(2.0*10^7 m/s)(6.0*10^(-4))sin\theta

How do I determine \theta?

c) r = (mv)/(qB)
r = [(9.11*10^(-31) kg)(2.0*10^7 m/s)] / [(1.60*10^(-19) C)(6.0*10^(-4) T)
r = .1898 m

d) Would the electrical and magnetic fields cancel? How do I set this up?
e) Would this be the opposite of (a)? [i.e., into the page?]
 
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Homework Equations


F = qvBsin\theta

r = (mv)/(qB)

The Attempt at a Solution



a) It is directed out of the page by the right hand rule. (Did I do this properly?)

b) F = qvBsin\theta
F = (1.60*10^(-19) C)(2.0*10^7 m/s)(6.0*10^(-4))sin\theta

How do I determine \theta?

v and B are perpendicular. Therefore θ is 90 degrees.

c) r = (mv)/(qB)
r = [(9.11*10^(-31) kg)(2.0*10^7 m/s)] / [(1.60*10^(-19) C)(6.0*10^(-4) T)
r = .1898 m

d) Would the electrical and magnetic fields cancel? How do I set this up?
e) Would this be the opposite of (a)? [i.e., into the page?][/QUOTE]

Due to magnetic field B, the centripetal force mv^2/r bends the electron beam in the upward direction. To nullify this deflection an electric force Eq should act in the downward direction.
 
Thank you, rl.bhat!
 

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