Lorentz force via electromagnetic field

The Lorentz force law states that a charged particle moving in an electromagnetic field experiences a force that depends on the values of the electric field and the magnetic field.

Notation:

  1. \(\left[ \vec a, \vec b \right]\) (cross(a, b)) is the cross product between \(\vec a\) and \(\vec b\).

Notes:

  1. This law is valid even in the relativistic case.

  2. This law works only in principle because a real particle would generate its own electromagnetic field that would interact with the external one which would alter the electromagnetic force it experiences.

Links:

  1. Wikipedia.

lorentz_force

Vector of the Lorentz force exerted on the charged particle.

Symbol:

F

Latex:

\({\vec F}\)

Dimension:

force

charge

Value of the electric charge of the test particle.

Symbol:

q

Latex:

\(q\)

Dimension:

charge

electric_field

Vector of the electric field. See electric_field_strength.

Symbol:

E

Latex:

\({\vec E}\)

Dimension:

voltage/length

velocity

Vector of the particle’s velocity. See speed.

Symbol:

v

Latex:

\({\vec v}\)

Dimension:

velocity

magnetic_flux_density

Vector of the magnetic_flux_density.

Symbol:

B

Latex:

\({\vec B}\)

Dimension:

magnetic_density

law

F = q * (E + cross(v, B))

Latex:
\[{\vec F} = q \left({\vec E} + \left[ {\vec v}, {\vec B} \right]\right)\]