Moving electric charges produce magnetic fields.
Magnetic fields exert forces on other moving charge.
The force a magnetic field exerts on a charge q moving with velocity
v is called the magnetic
It is given by
F = qv × B.
(The SI unit of B is Ns/(Cm) = T (Tesla))
The force F is perpendicular to the direction of the magnetic field B.
It also is perpendicular to the direction of the velocity v.
F is perpendicular to the plane that contains both v and B.
(Review the vector or cross product!)
The magnitude of the Lorentz force F is F = qvB sinθ, where θ is the smallest angle between the directions of the vectors v and B.
If v and B are parallel or anti-parallel to each other, then sinθ = 0 and F = 0. If v and B are perpendicular to each other, then sinθ = 1 and F has its maximum possible magnitude F = qvB.
If a charge q is moving with uniform velocity v parallel to the direction of a uniform magnetic field B, it experiences no force. It continues to move with uniform velocity v along a straight line parallel to the field.
To find the direction of the Lorentz force, use the right-hand rule. Let the fingers of your right hand point in the direction of v. Orient the palm of your hand, so that as you curl your fingers, you can sweep them over to point into the direction of B. Your thumb points in the direction of the vector product v × B. If q is positive then this is the direction of F. If q is negative, your thumb points opposite to the direction of F.
On the surface of a pulsar, or neutron star, the magnetic field may be as strong as 108 T. Consider the electron in a hydrogen atom on the surface of the neutron star. The average distance between the electron and the proton is 0.53*10-10 m. The average speed of the electron is 2.2*106 m/s. Compare the magnitude of the electric force that the electric field of the proton exerts on the electron with the maximum magnitude of the magnetic force that the magnetic field of the neutron star exerts on the electron. Is it reasonable to expect that the hydrogen atom will be strongly deformed by the magnetic field?
Consider a charged particle with mass m and charge q
which at t = 0 has a velocity v perpendicular to
This particle experiences a force with magnitude F = qvB perpendicular
to its velocity. A force perpendicular to the velocity results in
a = F/m = v2/r. The
particle will move along a circular path. The radius of the circle
r = mv2/F = mv2/(qvB) = mv/(qB),
and the circle lies in a plane perpendicular to B. The diagram on the right shows the paths followed by two charges, one positive (red) and one negative (blue), in a magnetic field that points into the page.
Since the magnetic force is perpendicular to the velocity v = ∆r/∆t, it is, at any time, perpendicular to the displacement ∆r. The work done by the magnetic force is therefore zero, ∆W = F∙∆r = 0. The magnetic force does no work. The magnetic force changes the direction of the velocity, but it does not change the speed or the kinetic energy of the particle.
Assume a particle at t = 0 is moving
with a velocity v which has a component vperpendicular
perpendicular and a component vparallel parallel to
the magnetic field.
The path of the particle will be a spiral.
There is no acceleration parallel to B, but in the plane perpendicular to B the centripetal acceleration is a = qvperpendicularB/m, and the particle moves in a circle. The superposition of these two motions results in a spiral path.
An interactive 3D animation of the motion of a charged particle in a uniform magnetic field.
In a current carrying wire electrons move with an average velocity, called
the drift velocity vd. If the wire is placed into a
magnetic field B, a force will act on the wire.
Consider a straight section of wire of length L. The number of
moving electrons in this section is n-AL, where n-
is the electron density and A is the cross-sectional area of the wire. The
electrons move with the drift velocity vd. The force
on the section of wire is the sum of the forces on all the moving electrons,
F = -qn-ALvd × B = jAL × B = IL × B.
Here we have used that -qn-vd = ρ-vd = j, and that jA = I for a wire. Since I is not a vector and we have to preserve the directional aspects of the vector product, we assign the direction of the current density to L, which points in the direction as j.
The force on a straight section of wire in a uniform field B is
F = IL × B.
You can again use the right-hand rule to find the direction of the force. Let the fingers of your right hand point in the direction of the current flow. Orient the palm of your hand, so that as you curl your fingers, you can sweep them over to point into the direction of B. Your thumb points in the direction of the vector product F.
A wire carries a steady current of 2.4 A. A
straight section of the wire is 0.75 m long and lies along the x-axis
within a uniform field B = 1.6 T in the z-direction. If the
current is in the positive x-direction, what is the magnetic force on
the section of wire.
Link: The Lorentz force on a wire (Youtube)
A demo: We pass a current through a wire a section of which passes
between the poles of two magnets, as shown below.
Make a prediction. When we connect the power supply, which way the wire will move?
Discuss this with your fellow students on Piazza!
Review with them the Lorentz force and the right-had rule.
Two parallel wires both carry current flowing in the same direction. Do
the wires attract or repel each other?
Remember: Parallel wires carrying currents in the same direction attract each other, parallel wires carrying currents in opposite directions repel each other.
If you miss having regular lectures, consider this video lecture.Lecture 11: Magnetic field and Lorentz Force