Charge passing through a magnetic field of uniform magnetic flux density

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Homework Help Overview

The discussion revolves around the behavior of a charged particle moving through a magnetic field, specifically examining the forces acting on the charge and the conditions required for it to move in a straight line rather than in a circular path due to the magnetic force.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between magnetic and electric forces on a charge, particularly how to compute the necessary electric field to counteract the circular motion induced by the magnetic field. There are questions regarding the net force on the charge when it moves in a straight line at constant speed.

Discussion Status

Participants have confirmed aspects of the reasoning presented, particularly regarding the nature of the forces involved and the conditions for straight-line motion. There is ongoing exploration of the implications of constant speed and the necessary electric field configuration.

Contextual Notes

There are mentions of constraints related to the velocity of the charge and the complexity introduced by variable speeds, which may affect the analysis of forces acting on the charge.

3OPAH
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upload_2015-4-5_11-42-42.png


My reasoning:

The magnetic force on charge q is

Fm = qv x B

B does not change |v|. Therefore, |Fm| is constant at time t > 0 and Fm is always perpendicular to the direction of movement of charge q. Fm behaves as a centripetal force, and thus the charge moves along the circumference of a circle.

Here is my drawing depicting what I think is happening:
upload_2015-4-5_11-47-25.png


Now, knowing that an electric charge q either at rest or in motion, experience an electric force Fe in the presence of an electric field E, that is,


Fe = qE

Then if we have a charge q moving with velocity v in the presence of both an electric field E and a magnetic flux density B, the total force exerted on the charge is therefore

F
= Fe + Fm = q(E + v x B)

which is the Lorentz force equation.

I am having trouble using what I have done so far and what I know about the magnetic force and electric force to compute the necessary electric force needed to make charge q move in a straight line. If the charge is moving in a circular path about the xy-plane under the influence of a magnetic field in the positive z direction, then the necessary electric field needed to counteract the circular movement of the charge and make it move in a straight line will be a combination of x and y coordinates, correct?
 
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3OPAH said:
then the necessary electric field needed to counteract the circular movement of the charge and make it move in a straight line will be a combination of x and y coordinates, correct?
Correct.

What is the net force on the charge if it moves in a straight line at constant speed*?

*this is not required, but if you allow a variable speed things get really messy
 
mfb said:
Correct.

What is the net force on the charge if it moves in a straight line at constant speed*?

*this is not required, but if you allow a variable speed things get really messy

If a charge experiences no net force, then its velocity is constant; the charge is either at rest (if its velocity is zero), or it moves in a straight line with constant speed. So the net force is zero.
 
mfb said:
Right.

So we are given the initial velocity of v = aex + bey. The magnitude of the velocity vector has to be the same, but opposite in direction. So the necessary electric field is (with the magnetic flux density in there as well):

E = -bB_0ex + aB_0ey

correct?
 

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