Hall Voltage (Cambridge (CIE) A Level Physics): Revision Note
Exam code: 9702
Written by: Ashika
Updated on
Hall voltage
When an external magnetic field is applied perpendicular to the direction of current through a conductor, the electrons experience a magnetic force
As a result, the electrons drift to one side of the conductor, causing it to become more negatively charged
This causes the opposite side to become more positively charged
As a result of the separation of charge, a potential difference is set up across the conductor
This is called the Hall voltage, which is defined as:
The potential difference produced across an electrical conductor when an external magnetic field is applied perpendicular to the current through the conductor
It is described by the expression:
Where:
= magnetic flux density (T)
= charge of the electron (C)
= current (A)
= number density of electrons (m-3)
= thickness of the conductor (m)
This equation shows that the smaller the electron density
of a material, the greater the magnitude of the Hall voltage
This is why a semiconducting material is often used for a Hall probe
Note: if the electrons were replaced by positive charge carriers, the direction of the Hall voltage would reverse
This happens because positive charges experience a magnetic force in the opposite direction to that experienced by electrons (provided the direction of the current is unchanged)
Hall voltage

The positive and negative charges drift to opposite ends of the conductor, producing a Hall voltage when a magnetic field is applied
Derivation of the Hall voltage equation
An equation for the Hall voltage
can be derived from the electric and magnetic forces on the charges
The voltage arises from the electrons accumulating on one side of the conductor slice
As a result of the charge separation, an electric field is set up between the two opposite sides of the conductor
The two sides can be treated as oppositely charged parallel plates, where the electric field strength
is equal to:
Where:
= Hall voltage (V)
= width of the conductor slice (m)
A single electron has a drift velocity
within the conductor
The magnetic field is into the plane of the page, so the magnetic force
on the electron acts to the right:
This is equal to the electric force
acting to the left:
Substituting
and cancelling the charge
Recall that current
is related to the drift velocity
by the equation:
Where:
= cross-sectional area of the conductor (m2)
= number density of electrons (m-3)
Rearranging this for
and substituting it into the equation gives:
The cross-sectional area
of the slice is equal to the product of the width
and thickness
:
Substituting
and rearranging for the Hall voltage
leads to the equation:
Electric and magnetic forces creating a Hall voltage

The electric and magnetic forces on the electrons are equal and opposite
Examiner Tips and Tricks
Remember to use Fleming’s left-hand rule to obtain the direction the electrons move due to the magnetic force created by the magnetic field.
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