Portions of this entry contributed by Leonardo Motta
The Coulomb force between two or more charged bodies is the force between them due to Coulomb's law. If the particles are both positively or negatively charged, the force is repulsive; if they are of opposite charge, it is attractive.
By the middle of eighteenth century, only the qualitative aspects of the electric force were known. Scientists started to speculate about the quantitative aspect of the force and the idea that the electric force could be similarly to the gravitational force, i.e., proportional to the inverse of the square of the distance. In 1777-1785, Charles Augustine Coulomb Eric Weisstein's World of Biography proved experimentally that indeed the electric force was proportional to the inverse of the square of the distance. Coulomb stated that the force that acts in two electrically charged bodies is proportional to the product of the module of their charges divided by the square of the distance d between them,
This called Coulomb's law and was the first attempt to understand the electric force.
Like the gravitational force, the Coulomb force is an inverse square law. Unlike the gravitational force
however, the Coulomb (or electric) force may be either attractive or repulsive, depending on the signs of the charges
and
The Coulomb force F on a charged particle due to another charge can be obtained by
multiplying the electric field caused by by the charge
Charge, Coulomb's Law, Coulomb Potential, Electric Field, Electromagnetic Force, Electromagnetism, Fundamental Forces Inverse Square Law, Lorentz Force
References
Feynman, R. P.; Leighton, R. B.; and Sands, M. The Feynman Lectures on Physics, Vol. 2. Redwood City, CA: Addison-Wesley, p. 1-2, 1989.
Whittaker, E. A History of the Theories of Aether and Electricity, Vols. 1-2. New York: Dover, 1989.