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Motion of a Charge Particle in
Uniform Magnetic Field
By Syed Mudassir Zaidi
Example: an electron travels at 2x107 m/s in a plane
perpendicular to a 0.01 T magnetic field. Describe its path.
Motion of a charged particle
in a uniform magnetic field
Example: an electron travels at 2x107 m/s in a plane
perpendicular to a 0.01 T magnetic field. Describe its path.
The above paragraph is a
description of uniform
circular motion.
The electron will move in a circular path with a constant speed
and acceleration = v2/r, where r is the radius of the circle.
The force on the electron
(remember, its charge is -) is
always perpendicular to the
velocity. If v and B are
constant, then F remains
constant (in magnitude).
-
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

B
v
F
v
F
-
-
Motion of a proton in a uniform magnetic field
+








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

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

Bout
v
FB
+ +
v
v
FB
FB
r
The force is always in the
radial direction and has a
magnitude qvB. For circular
motion, a = v2/r so
The rotational frequency f is
called the cyclotron frequency
The period T is
2
mv
F = q vB =
r
q rB mv
v = r =
m q B
π π
2 r 2 m
T = =
v q B
π
q B
1
f = =
T 2 m
Thanks to Dr. Waddill for the use of the picture and following examples.
Remember: you can do
the directions “by hand”
and calculate using
magnitudes only.
Helical motion in a uniform magnetic field
If v and B are perpendicular, a
charged particle travels in a circular
path. v remains constant but the
direction of v constantly changes.
If v has a component parallel to B,
then v remains constant, and the
charged particle moves in a helical
path.
v
v
B
+
There won’t be any test problems on
helical motion.
*or antiparallel
Electrons confined to move in a plane
Thanks to Dr. Yew San Hor for this and the next slide.
Apply B-field perpendicular to plane
Apply B-field perpendicular to plane









Lorentz Force Law
If both electric and magnetic fields are present,  .

F = q E+v B
Applications
See your textbook for numerical calculations related the next
two slides.
If I have time, I will show the mass spectrometer today.
The energy calculation in the mass spectrometer example is
often useful in homework.

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1600207755.ppt

  • 1. Motion of a Charge Particle in Uniform Magnetic Field By Syed Mudassir Zaidi
  • 2. Example: an electron travels at 2x107 m/s in a plane perpendicular to a 0.01 T magnetic field. Describe its path. Motion of a charged particle in a uniform magnetic field
  • 3. Example: an electron travels at 2x107 m/s in a plane perpendicular to a 0.01 T magnetic field. Describe its path. The above paragraph is a description of uniform circular motion. The electron will move in a circular path with a constant speed and acceleration = v2/r, where r is the radius of the circle. The force on the electron (remember, its charge is -) is always perpendicular to the velocity. If v and B are constant, then F remains constant (in magnitude). -                                                                 B v F v F - -
  • 4. Motion of a proton in a uniform magnetic field +                                        Bout v FB + + v v FB FB r The force is always in the radial direction and has a magnitude qvB. For circular motion, a = v2/r so The rotational frequency f is called the cyclotron frequency The period T is 2 mv F = q vB = r q rB mv v = r = m q B π π 2 r 2 m T = = v q B π q B 1 f = = T 2 m Thanks to Dr. Waddill for the use of the picture and following examples. Remember: you can do the directions “by hand” and calculate using magnitudes only.
  • 5. Helical motion in a uniform magnetic field If v and B are perpendicular, a charged particle travels in a circular path. v remains constant but the direction of v constantly changes. If v has a component parallel to B, then v remains constant, and the charged particle moves in a helical path. v v B + There won’t be any test problems on helical motion. *or antiparallel
  • 6. Electrons confined to move in a plane Thanks to Dr. Yew San Hor for this and the next slide. Apply B-field perpendicular to plane
  • 7. Apply B-field perpendicular to plane         
  • 8. Lorentz Force Law If both electric and magnetic fields are present,  .  F = q E+v B Applications See your textbook for numerical calculations related the next two slides. If I have time, I will show the mass spectrometer today. The energy calculation in the mass spectrometer example is often useful in homework.