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The following notation is used throughout the report:
 and
and  . Unit vectors have a hat on top of them, as
. Unit vectors have a hat on top of them, as  .
.  . The same goes for the absolute length of a vector, i.e.
. The same goes for the absolute length of a vector, i.e.  
  is
the unit vector in the radial direction.
is
the unit vector in the radial direction.  is the vector from point (current element) 1 to point (current element)
2;
is the vector from point (current element) 1 to point (current element)
2;  is the length of this vector; and
is the length of this vector; and  is the unit vector in its direction.
is the unit vector in its direction.  is
the distance from the origin. (It is used in the discussion on
surface
charges.)
is
the distance from the origin. (It is used in the discussion on
surface
charges.) Biot-Savart's law, well known from magnetostatics, gives the magnetic field from a circuit:
 
 is the magnetic field;
is the magnetic field;  the electric current;
the electric current;  is an infinitesimal section of the conductor;
is an infinitesimal section of the conductor;  the distance from
the distance from  to the point where the magnetic field is to be measured,; and
to the point where the magnetic field is to be measured,; and  the unit vector from
the unit vector from  to that point.
to that point. 
In differential form it becomes:
 
The magnetic force (  ) that moving charge experiences in a magnetic field is given by the
Lorentz
force law:
) that moving charge experiences in a magnetic field is given by the
Lorentz
force law: 
 
Here q is the charge that is moving;  its velocity; and
its velocity; and  the magnetic induction. With
the magnetic induction. With  in vacuum (and air), and noting that
in vacuum (and air), and noting that  we have:
we have: 
 
which is Grassmann's law for the force between two current elements.