Coulombic Force = [(-e)(Ze)]/r^2 = -Ze^2/r^2
If Coulomb's force is gone , the material structure of the Cosmos would be gone. Coulomb's force hold atoms together and molecules together and matter together.
F = kq1q2/r2 where F is the coulomb force, k is coulomb's constant, q1 and q2 are the magnitudes of the charges and r is the distance between them.
The force that binds electrons to nuclei to form atoms is usually called the electrostatic force or the Coulomb force; the magnitude of the force can be calculated using Coulomb's law.
Electromotive force is not a force. It is the work performed to move one coulomb of charge.
Charles-Augustin de Coulomb (1736 - 1806) was a French physicist known for developing Coulomb's law which defines the electrostatic force of attraction and repulsion. The SI unit of charge, the coulomb, was named after him.
Force acts on charges. This is demonstrated by Coulomb's law.
Atomic structure is predominantly determined by the Coulomb force. The Coulomb force, i.e. force between charges is inversely proportional to distance, is the force of electrostatics. The Coulomb force is the force of attraction between the nucleus and the electrons and it is the force of repulsion between the electrons. Quantum mechanics is the theory which uses this force law in determining electronic structure of atoms and molecules. If one wants to get picky and look for very small influences on atomic structure that are not due to the Coulomb force, then one has to investigate the subject of special relativity and some very weak nuclear interactions.
Cool
The electrostatic force (or electric force) can be described by Coulomb's Law. See: http://www.answers.com/topic/coulomb-s-law?ff=1
It also doubles.F = kq1q2/r2 where F is the coulomb force, k is coulomb's constant, q1 and q2 are the magnitudes of the charges and r is the distance between them.
Yes, Coulomb's law is an example of a conservative force. A conservative force is one in which the energy required to move a particle (subject to this force) from one point in space to another is independent of the path taken.
Coulomb.