Laplace's force
Fondamental : Case of parallelepiped conductor
This lesson uses the same notations as the lesson about Hall effect.
The following video shows the Laplace's force experimentally (Alain Le Rille, CPGE teacher at lycee Janson de Sailly, Paris)
What is the expression of the force applied by the magnetic field
to the conductor ?
The set of carrier electrons and metallic cations in the conductor is subject to the following forces due to the magnetic field
:
On the carrier electrons :
Where
is the density of charge carriers.
On metallic cations (still) :
Globally the conductor is subject to the force :

The intensity
can be expressed as:
So :
Attention : Laplace's force for a thread-like conductor
A portion of the thread-like circuit is travelled by the intensity
and put in a certain magnetic field
.

The conductor is subject to the force called Laplace's force :
By writing :
Then :
This is the expression of the Laplace's force for volume currents.
Differences between Laplace's and Lorentz's forces :
Lorentz's force is microscopic. It is applied to charge
moving carriers in a magnetic field :
Laplace's force is macroscopic. It is applied to any conductor, electrons and cations included.