Lorentz Force

Edited by Chris Mickas Fall 2016 Yiqiao Wu Spring 2017

Edited by Adam Schatz Fall 2017

Edited by Connor Meeds Fall 2017

The Main Idea

The Lorentz Force is a name for the entire electromagnetic force exerted on a charged particle q moving with velocity v through an electric field E and magnetic field B. In most cases studied throughout college physics courses, the Lorentz Force on a particle is merely contributed by electric and magnetic forces, where other forces acting on the particle are considered negligible.

A Mathematical Model

The electromagnetic force F on a charged particle, the Lorentz force (named after the Dutch physicist Hendrik A. Lorentz) is given by:

[math]\displaystyle{ \vec{F}_{Lorentz} = q\vec{E} + q\vec{v} ⨯ \vec{B} }[/math]

where [math]\displaystyle{ q\vec{E} }[/math] is the electric force contributed by an external electric field and [math]\displaystyle{ q\vec{v} ⨯ \vec{B} }[/math] is the magnetic force contributed by an external magnetic field. As many applications involve vectors, it is valuable to recognize the resulting directions of [math]\displaystyle{ q\vec{E} }[/math] and [math]\displaystyle{ q\vec{v} ⨯ \vec{B} }[/math] in relation to the particle's charge and velocity within the environment of applied electric/magnetic fields. The resulting electric force vector will always be towards or opposite to the applied electric field, depending on the sign of the charge. For example, an electron undergoing an electric field in the +x direction will receive an electric force in the -x direction. The magnetic force on the particle, however, has a direction perpendicular to both the velocity v of the particle and the magnetic field B, and has a value proportional to q and to the magnitude of the vector cross product [math]\displaystyle{ q\vec{v} ⨯ \vec{B} }[/math]. More specifically, the magnitude of the magnetic force equals qvBsinθ where θ is the angle between v and B.

Motion of a Charged Particle in a Uniform Magnetic Field

A noteworthy result of the Lorentz force is the motion of a charged particle within a uniform magnetic field as the angle between v and B varies. If a scenario presents a charged particle with a velocity vector v perpendicular to the applied magnetic field B (i.e. θ = 90°), the particle will follow a circular trajectory. The radius of this trajectory can easily be calculated:

[math]\displaystyle{ \vec{F}_{Mag} = \vec{F}_{Centripetal} }[/math]

[math]\displaystyle{ qvB = mv^2/R }[/math]

[math]\displaystyle{ R = mv/qB }[/math]

Suppose that for the following example, a charge is shot into a region filled with a uniform magnetic field coming out of the page:

At every instant, the external magnetic field B points out of the page and thus invokes a magnetic force on the particle perpendicular to the particle's velocity - the force needed to create circular motion. The radius R can be calculated from the equation above. In addition, it's worth noting that the particle's charge will determine where the particle veers. If the particle were positively charged, the magnetic force would cause the particle to veer downward (due to right hand rule), and vice-versa if negatively charged.

In the case that θ is less than 90°, the particle's trajectory will orbit a helix path with a central axis parallel to the field lines.

If θ is zero, that is, the magnetic field is in the same direction as the particle's velocity, the particle will experience no magnetic force and continue to move normally along the field lines.

A Computational Model

Here is a visualization on VPython of a negatively charged particle moving through a constant electric and magnetic field:

Initially, a negatively charged particle is traveling with initial velocity in the -z direction. There is a constant electric field E in the -x direction and a constant magnetic field B in the +y direction. The magnetic force on the negatively charged particle is equal to [math]\displaystyle{ q\vec{v} ⨯ \vec{B} }[/math], or the charge of the particle times the cross product of the particle’s velocity and the magnetic field it travels through. The electric force on the particle is equal to [math]\displaystyle{ q\vec{E} }[/math], or the charge of the particle times the electric field that the particle travels through. Since the magnetic force on the particle is related to the particle’s velocity v, the magnetic force changes as the the particle’s velocity changes. Conversely, the electric force on the particle is constant. Since the Magnetic force is variable, the Lorentz Force on the particle, or the net force due to magnetic and electric forces on the particle ([math]\displaystyle{ \vec{F}_{Lorentz} = q\vec{E} + q\vec{v} ⨯ \vec{B} }[/math]) is also variable, and the particle's velocity changes.

Example Problems

Simple

The electric force on a certain particle is <100,-600,300> N and the magnetic force is <-600,400,0> N. Find the Lorentz force.

Solution: Lorentz force = <-500,-200,300> N

Intermediate

The magnetic force on a proton is 100 N at an angle 30 degrees down from the +x axis. The electric force on the proton is 100 N at an angle 30 degrees up from the +z axis. What is the magnitude of the Lorentz Force on the proton?

Solution: Lorentz force = 122.5 N

Difficult

An electron is traveling with a constant velocity of <0.75c, 0, 0>. You measure the magnetic field to be <0.4, 0.3, 0.5>T everywhere. What is the electric field?

Solution: E = <0, 1.13e8, -6.75e7> N/C

Since the electron is traveling at constant velocity, the net force must be zero. Thus, the magnetic field must equal the electric field, or [math]\displaystyle{ q\vec{v} ⨯ \vec{B}= q\vec{E} }[/math]. The charge on both sides cancels out to give [math]\displaystyle{ \vec{v} ⨯ \vec{B}= \vec{E} }[/math]. Calculating [math]\displaystyle{ q\vec{v} ⨯ \vec{B} }[/math] = <0, -1.13e8, 6.75e7>, so the electric field must point in the opposite direction.

Connectedness

1. Speakers use the Lorentz force of an electromagnet to move a cone that creates sound waves in the air. When current flows through the wires in the electromagnetic in different quantities, the speakers move in unique ways to produce the different sounds that we recognize. Amplifiers for electric guitars and basses work in the same way.

2. In today's evolving world, one area of particular interest is sustainable and renewable energy. Wind turbines and hydropower plants work by harnessing the kinetic energy of wind or water and using it to induce an electrical current. The turbines rotate and move a permanent magnet that induces a current in an electromagnet placed inside of the magnet, which is shaped like a hollow cylinder. The induced current is then carried via wires to external sources to provide energy.

3. Several industries manufacture products that induce current using the Lorentz Force. For example, electric guitars and basses work by magnetizing the strings and relying on the Lorentz force to create a current in pickups that is then transmitted to an amplifier. Pickups are small electromagnet coils surrounding a magnet that are placed beneath the strings. The strings become magnetized because of the magnet inside the pickup. When they are played and vibrate, they induce current in the electromagnet. The Lorentz force causes the strings to exert forces that move mobile charges and induce the current. The current is then increased through a potentiometer and sent to an amplifier through a cable. In addition, charged particle accelerators like cyclotrons make use of the circular orbit particles experience when v and B are perpendicular to each other. For each revolution, a carefully timed electric field offers additional kinetic energy to cause the particles to move in increasingly-larger orbits until a desired energy level is met. These particles are known to be extracted and used in a number of ways, from basic studies of the properties of matter to the medical treatment of cancer.

History

The Lorentz Force is named after Hendrik Lorentz, who derived the formula in the late 19th century following a previous derivation by Oliver Heaviside in 1889. However, scientists had tried to find formulas for one electromagnetic force for over a hundred years before.Some scientists such as Henry Cavendish argued that the magnetic poles of an object could create an electric force on a particle that obeys an inverse-square law. However, the experimental proof was not enough to definitively publish. In 1784, Charles de Coulomb, using a torsion balance, was able to definitively show through experiment that this was true. After Hans Christian Ørsted discovered that a magnetic needle is acted on by a voltaic current, Andre Marie Ampere derived a new formula for the angular dependence of the force between two current elements. However, the force was still given in terms of the properties of the objects involved and the distances between, not in terms of electric and magnetic fields or forces.

Michael Faraday introduced modern ideas of magnetic and electric fields, including their interactions and relations with each other, later to be given full mathematical description by William Thomson (Lord Kelvin) and James Maxwell. From a modern perspective it is possible to identify in Maxwell's 1865 formulation of his field equations a form of the Lorentz force equation in relation to electric currents, however, it was not initially evident how his equations related to the forces on moving charged objects. J.J. Thomson was the first to attempt to derive from Maxwell's field equations the electromagnetic forces on a moving charged object in terms of the object's properties and external fields. Interested in determining the electromagnetic behavior of the charged particles in cathode rays, Thomson published a paper in 1881 wherein he gave the force on the particles due to an external magnetic field as [math]\displaystyle{ \vec{F} = q\vec{E} + \frac{q}{2}\vec{v} ⨯ \vec{B} }[/math]. Finally, Heaviside and later Lorentz were able to combine the information into the currently accepted Lorentz Force equation.

Lorentz Force

Contents

The Main Idea

A Mathematical Model

Motion of a Charged Particle in a Uniform Magnetic Field

A Computational Model

Example Problems

Simple

Intermediate

Difficult

Connectedness

History

See also

Further reading

External links

References

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