If we move a charge q from a point a to a point b, then the
charge in potential energy, Uab, of the system is
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(1) |
-
is a small displacement along the
path we choose to take from a to b.
If we define the
electric potential to be the potential energy per unit charge,
so that V=U/q, then the difference in electric potential is given by,
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(2) |
With the definition of potential given in Eq. (2) and
taking the potential at infinity to be zero, we can
calculate the potential at each position from the
electric field.
Electric potential due to a point charge
The electric field due to a point charge is
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(3) |
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(4) |
Uniform shell of charge
From the shell theorems we know that the electric
field inside a uniform shell of charge is zero.
In addition, if the electric field is zero the integral (2)
gives no contribution so
the electric potential is a constant. The electric
potential of a uniform shell of charge is
therefore a constant inside the shell of charge
and like a point charge centered at the origin
outside the shell of charge.
Conductors
Inside and on the surface of conductors, the
electrical potential is a constant. This follows
as the electric field is zero inside and
parallel to the surface of conductors.
Parallel plates
If we consider two parallel plates with
uniform charge density ,
then the electric field
between the plates has magnitude
.
Since this
is a constant, the electric potential difference between the
plates is simply E d where d is the distance
between the plates. The electric potential
is defined as the potential to move a
small positive charge between two positions.
In this case we imagine moving a small positive
charge from the negative plate to the positive
plate. This requires work and hence the electrical
potential is positive.
The electric potential of the
positively charged plate is thus higher than the electric
potential of the negatively charged plate.