Fundamentally the electric field
is defined as the force
per unit charge
experience by a small charge – small enough so as not to disturb the field in any way. We can write
or![]()
A electric charge or combination of electric charges produces an electric field – that is, a force is exerted on any electric charge that comes close to these charges. If a 'test charge'
– an infinitesimally small charge, so that the distribution of charges is not disturbed and the electric field does not change -is introduced, the force experienced by the test charge will be the sum of the forces exerted by each individual charge in the distribution. We can use Coulomb's Law to write
![]()
where
is the unit vector from charge
to the test charge![]()
Then![]()
Dividing by
gives![]()
The electric field at the position of
due to the charge
is
so we can also write![]()
This means that we can find the field due to each charge as a vector and add them.
The technical term is linear – the electric field and the electric force are both linear in the charges![]()