The electric field and electric potential due to a point charge are closely related concepts in electrostatics.
1. **Electric Field (E)**: This is a vector quantity that represents the force per unit charge experienced by a test charge placed in the field. For a point charge \( q \), the electric field \( \vec{E} \) at a distance \( r \) from the charge is given by:
\[
\vec{E} = \frac{k q}{r^2} \hat{r}
\]
where \( k \) is Coulomb's constant, and \( \hat{r} \) is a unit vector pointing radially away from the charge if \( q \) is positive, or towards the charge if \( q \) is negative.
2. **Electric Potential (V)**: This is a scalar quantity that represents the work done per unit charge in bringing a test charge from infinity to a point in the field. For a point charge \( q \), the electric potential \( V \) at a distance \( r \) from the charge is given by:
\[
V = \frac{k q}{r}
\]
**Relationship**: The electric field is related to the electric potential by the gradient. Specifically, the electric field is the negative gradient of the electric potential:
\[
\vec{E} = -\nabla V
\]
For a point charge, in spherical coordinates, this relationship simplifies to:
\[
E = -\frac{dV}{dr}
\]
Substituting \( V = \frac{k q}{r} \), we get:
\[
E = -\frac{d}{dr} \left( \frac{k q}{r} \right) = \frac{k q}{r^2}
\]
Thus, the electric field is the spatial rate of change of the electric potential.