Electric field due to dipole¶
The strength of the electric field set up by a dipole at a distant point on the dipole axis, which runs through both point charges comprising the dipole, is proportional to the inverse cube of the distance to the dipole and the value of the electric dipole moment.
Notation:
\(\varepsilon_0\) (
epsilon_0
) isvacuum_permittivity
.
Conditions:
\(r / d \gg 1\) where \(d\) is the distance between point charges of the dipole. This means that the point where electric field is measured must be far enough from the dipole itself.
Links:
- electric_field_strength¶
electric_field_strength
due to dipole.- Symbol:
E
- Latex:
\(E\)
- Dimension:
voltage/length
- electric_dipole_moment¶
See Electric dipole moment is charge times distance and
electric_dipole_moment
.- Symbol:
p
- Latex:
\(p\)
- Dimension:
charge*length
- distance¶
euclidean_distance
to dipole.- Symbol:
d
- Latex:
\(d\)
- Dimension:
length
- law¶
E = p / d^3 / (2 * pi * epsilon_0)
- Latex:
- \[E = \frac{1}{2 \pi \varepsilon_0} \frac{p}{d^{3}}\]