Consider a thin, flat, uniform, ribbon of some conducting material which is orientated such that its flat side is perpendicular to a uniform magnetic field --see Fig. 26. Suppose that we pass a current along the length of the ribbon. There are two alternatives. Either the current is carried by positive charges moving from left to right (in the figure), or it is carried by negative charges moving in the opposite direction.

Suppose that the
current is carried by positive charges moving from left to right.
These charges are deflected
*upward* (in the figure) by the magnetic field. Thus, the upper edge of the ribbon becomes
positively charged, whilst the lower edge becomes negatively charged.
Consequently, there is a *positive* potential difference between the upper
and lower edges of the ribbon. This potential difference is called the *Hall voltage*.

Suppose, now, that the current is carried by negative charges
moving from right to left. These
charges are also deflected *upward* by the magnetic field. Thus, the upper edge
of the ribbon becomes negatively charged, whilst the lower edge becomes
positively charged. It follows that the Hall voltage (*i.e.*, the
potential difference between the upper and lower edges of the ribbon)
is *negative* in this case.

Clearly, it is possible to determine the sign of the mobile charges in a
current carrying conductor by measuring the Hall voltage. If the voltage is
positive then the mobile charges are positive (assuming that the
magnetic field and the current are orientated as shown in the
figure), whereas if the voltage is
negative then the mobile charges are negative. If we were to perform
this experiment we would discover that the the mobile charges in metals
are always negative (because they
are electrons). However, in some types of semiconductor the mobile charges
turn out to be positive. These positive charge carriers are called *holes*.
Holes are actually missing electrons in the atomic lattice of the
semiconductor, but they act essentially like positive charges.

Let us investigate the magnitude of the Hall voltage. Suppose that the mobile
charges each possess a charge and move along the ribbon with the
drift velocity . The magnetic force on a given mobile charge
is of magnitude , since the charge moves essentially
at right-angles to the magnetic field. In a steady-state, this force
is balanced by the electric force due to the build up of charges
on the upper and lower edges of the ribbon. If the Hall voltage is
, and the width of the ribbon is , then the electric
field pointing from the upper to the lower edge of the ribbon is
of magnitude . Now, the electric force on a mobile charge
is . This force acts in opposition to the magnetic force.
In a steady-state,

(169) |

Note that the Hall voltage is directly proportional to the magnitude of the magnetic field. In fact, this property of the Hall voltage is exploited in instruments, called

Suppose that the thickness of the conducting ribbon is , and that it contains
mobile charge carriers per unit volume. It follows that the total current
flowing through the ribbon can be written

(172) |