Motion of charged particles in E and B fields

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Homework Help Overview

The discussion revolves around the motion of photoelectrons emitted from a parallel-plate capacitor in the presence of an electric field and a magnetic field. The problem involves determining the conditions under which an electron can reach the positive plate of the capacitor based on the potential difference and the magnetic flux density.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore the forces acting on the electrons, including electric and magnetic forces, and discuss the relationship between acceleration and centripetal motion. Questions arise regarding the appropriate expressions for velocity and the implications of energy conservation.

Discussion Status

Participants have provided various approaches to relate the forces and energies involved. Some have suggested using energy conservation principles, while others have pointed out the need to consider centripetal acceleration due to the magnetic field. There is an ongoing exploration of the conditions under which electrons can reach the positive plate.

Contextual Notes

There is a focus on the specific charge of the electron and the implications of the potential difference in relation to the magnetic field. Participants are also considering the scenario of electrons that do not reach the positive plate, which adds complexity to the discussion.

georgia
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Homework Statement



Photoelectrons are emitted with negligible initial velocity from one plate of a parallel-plate capacitor which is at zero potential. The other plate is held at a potential +V and the capacitor is in a uniform magnetic field of flux density B parallel to the plane of the plates. Show that no electron can reach the positive plate if V is less than e(DB)^2/2m where D is the separation of the plates and e/m is the specific charge of the electron.

Homework Equations



F=q(vxB)
E=V/D
F=qE

The Attempt at a Solution



Ok well I've found the force due to the electric field created by the capacitor by saying:

F=qE and E=V/D
so F=qV/D
The charge of the electron is e/m so:
F=eV/mD

Then you've got the force due to the magnetic field which is trying to pull the electron in a circle. I'm not sure where you go from here. All I know is that:

F=evB but what do I use for v as obviously it's accelerating?
 
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Pointing out that specific charge is NOT charge of the electron.
So F/m = eV/mD
F=ma
So accleleration towads the plate by the electric force is = eV/mD

Try relating it with centripetal acceleration caused by the magnetic field.
 
georgia said:

Homework Statement



Photoelectrons are emitted with negligible initial velocity from one plate of a parallel-plate capacitor which is at zero potential. The other plate is held at a potential +V and the capacitor is in a uniform magnetic field of flux density B parallel to the plane of the plates. Show that no electron can reach the positive plate if V is less than e(DB)^2/2m where D is the separation of the plates and e/m is the specific charge of the electron.

Homework Equations



F=q(vxB)
E=V/D
F=qE

The Attempt at a Solution



Ok well I've found the force due to the electric field created by the capacitor by saying:

F=qE and E=V/D
so F=qV/D
The charge of the electron is e/m so:
F=eV/mD

Then you've got the force due to the magnetic field which is trying to pull the electron in a circle. I'm not sure where you go from here. All I know is that:

F=evB but what do I use for v as obviously it's accelerating?

It might be best to use potential energy/kinetic energy relation for a particle that just grazes the plate, eg 1/2mv^2=eV. What else must v be? (use quantums idea about centripetal force from the magnetic field)
 
Ok so at the plate with zero potential the photoelectron has negligible kinetic energy and potential energy of eV. At the other plate the photoelectron has no potential energy and all kinetic energy?

So: 1/2mv^2=eV Is this correct?

The radius of the circle if the photoelectron just grazes the plate will be D so I can say that the centripetal force is mv^2/D and this is equal to the force due to the magnetic field (?)

So mv^2/D=evB
and so v=eBD/m

Substituting into: 1/2mv^2=eV gives:

V=e(DB)^2/2m so have I done it?!

If this is right then thanks everyone for your help :smile:
 
Last edited:
methinks so. But remember this is for particle that never makes it. so for particle that reaches other side, v> that quantity as asked for in statement in problem.
 

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