Lorentz force

In physics, the Lorentz force is the force on an electrically charged particle that moves through a magnetic field and possibly also through an electric field. In the absence of an electric field, the strength of the Lorentz force is proportional to the charge q of the particle and its velocity v (a vector). The direction of the force is given by the right hand rule: put your right hand along v with the open palm toward the magnetic field B (a vector). Stretch the thumb of your right hand, the Lorentz force is along it, pointing from your wrist to the tip of your thumb.

The force is named after the Dutch physicist Hendrik Antoon Lorentz, who gave its description in 1892.<ref>H. A. Lorentz, La théorie électromagnétique de Maxwell et son application aux corps mouvants, Archives néerlandaises des Sciences exactes et naturelles, 1892, vol. 25 p. 363 (1892).<ref>

Mathematical description

The Lorentz force F_Lorentz is given by the experssion

$\mathbf {F} _{\textrm {Lorentz}}=q(\mathbf {E} +k\mathbf {v} \times \mathbf {B} ),$

here k is a constant depending on the units. In SI units k = 1; in Gaussian units k = 1/c, where c is the speed of light in vacuum (299 792 458 m s⁻¹ exactly). The quantity q is the electric charge of the particle and v is its velocity. The vector B is the magnetic induction (also referred to as the magnetic field). The product between v and B is a vector product, which obeys the right hand rule mentioned above. The electric field A is in full generality given by

$\mathbf {E} =-{\boldsymbol {\nabla }}V-k{\frac {d\mathbf {A} }{dt}}$

with the (magnetic) vector protential A

$\mathbf {B} ={\boldsymbol {\nabla }}\times \mathbf {A}$