Did you know that the world exists mainly because of the force of attraction and repulsion? It is mainly because of these attractions and repulsions between particles that the environment remains in a well-equipped and well-balanced form. One such practical application of this theory is the Coulomb’s Law.

Do you know what Coulomb’s Law is all about? Well, in order to find out the extent of repulsion or attraction force between two particles, having some charge, Charles – Augustin de Coulomb came up with the Coulomb’s Law. We will learn about it in this chapter.

### Suggested Videos

## Coulomb’s Law

Coulomb’s Law gives an idea about the force between two point charges. By the word point charge, we mean that in physics, the size of linear charged bodies is very small as against the distance between them. Therefore, we consider them as point charges as it becomes easy for us to calculate the force of attraction/ repulsion between them.

Charles-Augustin de Coulomb**, **a French physicist in 1784, measured the force between two point charges and he came up with the theory that the force is inversely proportional to the square of the distance between the charges. He also found that this force is directly proportional to the product of charges (magnitudes only).

We can show it with the following explanation. Let’s say that there are two charges q_{1} and q_{2.} The distance between the charges is ‘r’, and the force of attraction/repulsion between them is ‘F’. Then

F ∝ q_{1}q_{2}

Or, F ∝ 1/r^{2}

F = k q_{1}q_{2}/ r^{2}

where k is proportionality constant and equals to 1/4 π ε_{0}. Here, ε_{0} is the epsilon naught and it signifies permittivity of a vacuum. The value of k comes 9 × 10^{9} Nm^{2}/ C^{2} when we take the S.I unit of value of ε_{0} is 8.854 × 10^{-12} C^{2} N^{-1} m^{-2}.

According to this theory, like charges repel each other and unlike charges attract each other. This means charges of same sign will push each other with repulsive forces while charges with opposite signs will pull each other with attractive force.

**Browse more Topics under Electric Charges And Fields**

- Conductors and Insulators
- Electric Charge
- Basic Properties of Electric Charge
- Electric Field
- Electric Field Lines
- Gauss’s Law
- Applications of Gauss’s Law
- Electric Flux
- Electric Dipole
- Dipole in a Uniform External Field

*Learn more about Gauss’s Law here in detail*

## Vector Form of Coulomb’s Law

The physical quantities are of two types namely scalars (with the only magnitude) and vectors (those quantities with magnitude and direction). Force is a vector quantity as it has both magnitude and direction. The Coulomb’s law can be re-written in the form of vectors. Remember we denote the vector “F” as F, vector r as r and so on.

Let there be two charges q_{1} and q_{2}, with position vectors r_{1} and r_{2} respectively. Now, since both the charges are of the same sign, there will be a repulsive force between them. Let the force on the q_{1} charge due to q_{2} be F_{12} and force on q_{2} charge due to q_{1 }charge be F_{21}. The corresponding vector from q_{1} to q_{2} is r_{21} vector.

r_{21 }= r_{2} – r_{1}

To denote the direction of a vector from position vector r_{1} to r_{2} , and from r_{2} to r_{1 }as:

Now, the force on charge q_{2} due to q_{1}, in vector form is:

The above equation is the vector form of Coulomb’s Law.

**Download Conductors and Insulators Cheat Sheet PDF**

## Remarks on Vector Form of Coulomb’s Law

While applying Coulomb’s Law to find out the force between two point charges, we have to be careful of the following remarks. The vector form of the equation is independent of signs of both the charges, as both the forces are opposite in nature.

The repulsive force F_{12} , that is the force on charge q_{1} due to q_{2} and another repulsive force F_{21} that is the force on charge q_{2} due to q_{1} are opposite in signs, due to change in position vector.

F_{12} = – F_{21}

This is because the position vector in case of force F_{12 }is r_{12} and position vector in case of force F_{21} is r_{21}, now

r_{21 }= r_{2} – r_{1}

r_{12} = r_{1} – r_{2}

Since both r_{21 }and r_{12 }are opposite in signs, they make forces of opposite signs too. This proves that Coulomb’s Law fits into Newton’s Third Law i.e. every action has its equal and opposite reaction. Coulomb’s Law provides the force between two charges when they’re present in a vacuum. This is because charges are free in a vacuum and don’t get interference from other matter or particles.

## Limitations of Coulomb’s Law

Coulomb’s Law is derived under certain assumptions and can’t be used freely like other general formulas. The law is limited to following points:

- We can use the formula if the charges are static ( in rest position)
- The formula is easy to use while dealing with charges of regular and smooth shape, and it becomes too complex to deal with charges having irregular shapes
- The formula is only valid when the solvent molecules between the particle are sufficiently larger than both the charges

## Solved Example for You

Question: Two charges 1 C and – 3 C are kept at a distance of 3 m. Find the force of attraction between them.

Solution: We have q_{1} = 1C, q_{2} = – 3C and r = 3m. Then using Coulomb’s Law and substituting above values we get

F = k q_{1}q_{2}/ r^{2}

Or, F = 9 × 10^{9 }× 1 × 3/ 3^{2}

F = 3 × 10^{9} Newton

Can u provide with the pdf of all the derivations of physics class 12