## What is Coulomb’s Law?

According to the Coulombs law, the force of attraction or repulsion between two charged bodies is directly proportional to the product of their charges and inversely proportional to the square of the distance between them. It acts along the line joining the two charges considered to be point charges.

### Table of Content

**According to Coulomb’s Law:** F ∝ q_{1}q_{2}/d^{2}

**where,**

**ε is absolute permittivity**,**K**or**ε**is the_{r}**relative permittivity**or**specific inductive capacity****ε**is the_{0}**permittivity of free space**.- K or
**ε**is also called a dielectric constant of the medium in which the two charges are placed._{r}

**Brief History on Coulomb’s law:** A French Physicist Charles Augustin de Coulomb in 1785 coined a tangible relationship in mathematical form between two bodies that have been electrically charged. He published an equation for the force causing the bodies to attract or repel each other which is known as Coulomb’s law or Coulomb’s inverse-square law.

### Relative Permittivity of a Material

\({{\varepsilon }_{r}}\) = \(K=\frac{force\;between\;two\;charge\;in\;air}{force\;between\;same\;charge\;in\;the\;medium\;at\;the\;same\;distance}\). \({{\varepsilon }_{r}}\) = \(=\frac{F_a}{F_m}\)- For air K = 1
- For metals K = infinity

Force between 2 charges depends upon the nature of the intervening medium, whereas gravitational force is independent of intervening medium.

For air or vacuum, \(F\text{ }=\text{ }\frac{\text{1}}{\text{4}\pi {{\varepsilon }_{\text{o}}}}.\frac{{{\text{q}}_{\text{1}}}{{q}_{2}}}{{{d}^{2}}}\) since for air or vacuum, \({{\varepsilon }_{r}}\) = K = 1

The value of \(\frac{\text{1}}{\text{4}\pi {{\varepsilon }_{\text{o}}}}\) is equal to 9 × 10^{9} Nm^{2}/C^{2}.

#### Also Read:

## What is 1 Coulomb of Charge?

A coulomb is that charge which repels an equal charge of the same sign with a force of 9×10^{9} N when the charges are one meter apart in a vacuum. Coulomb force is the conservative mutual and internal force.

The value of \({{\varepsilon }_{o}}\) is 8.8610^{–12} C^{2}/Nm^{2} (or) 8.8610^{–12} Fm^{–1}

**Note:** Coulomb force is true only for static charges.

### Coulomb’s Law – Conditions for Stability

If q is slightly displaced towards A, FqA increases in magnitude while FqB decreases in magnitude. Now the net force on q is toward A so it will not return to its original position. So for axial displacement, the equilibrium is unstable.

If q is displaced perpendicular to AB, the force FqA and FqB bring the charge to its original position. So for perpendicular displacement, the equilibrium is stable.

## Coulomb’s Law in Vector Form

\({{\vec{F}}_{12}}=\frac{1}{4\pi {{\in }_{0}}}-\frac{{{q}_{1}}{{q}_{2}}}{r_{12}^{2}}{{\hat{r}}_{12}}; \;\;{{\vec{F}}_{12}}=-{{\vec{F}}_{21}}\)Here F_{12} is force exerted by q_{1} on q_{2} and F_{21} is force exerted by q_{2} on q_{1}.

Coulomb’s law holds for stationary charges only which are point sized. This law obeys Newton’s third law

\(\left( ie\,\,\,{{{\vec{F}}}_{12}}=-{{{\vec{F}}}_{21}} \right)\)Force on a charged particle due to a number of point charges is the resultant of forces due to individual point charges i.e.

\(\vec{F}={{\vec{F}}_{1}}+{{\vec{F}}_{2}}+{{\vec{F}}_{3}}+……\)## Key Points on Coulomb’s Law

**1.** If the force between two charges in two different media is the same for different separations, \(F=\frac{1}{K}\frac{1}{4\pi {{\in }_{0}}}\frac{{{q}_{1}}{{q}_{2}}}{{{r}^{2}}}\) = constant .

**2. ** Kr^{2} = constant or K_{1}r_{1}^{2} = K_{2}r_{2}^{2 }

**3.** If the force between two charges separated by a distance ‘r_{0}’ in vacuum is same as the force between the same charges separated by a distance ‘r’ in a medium, Kr^{2} = r_{0}^{2}

**4.** Two identical conductors having charges q_{1} and q_{2} are put to contact and then separated, then each have a charge equal to \(\frac{{{q}_{1}}+{{q}_{2}}}{2}\). If the charges are q_{1} and –q_{2}, then each have a charge equal to \(\frac{{{q}_{1}}-{{q}_{2}}}{2}\).

**5.** Two spherical conductors having charges q_{1} and q_{2} and radii r_{1} and r_{2} are put to contact and then separated then the charges of the conductors after contact are

**6.** The force of attraction or repulsion between two identical conductors having charges q_{1} and q_{2} when separated by a distance d is F. If they are put to contact and then separated by the same distance the new force between them is F = \(\frac{F{{\left( {{q}_{1}}+{{q}_{2}} \right)}^{2}}}{4{{q}_{1}}{{q}_{2}}}\)

**7. **If charges are q_{1} and –q_{2} then, F =\(\frac{F{{\left( {{q}_{1}}-{{q}_{2}} \right)}^{2}}}{4{{q}_{1}}{{q}_{2}}}\).

**8.** Between two electron separated by a certain distance: Electrical force/Gravitational force = 10^{42}

**9.** Between two protons separated by a certain distance: Electrical force/Gravitational force = 10^{36}

**10.** Between a proton and an electron separated by a certain distance: Electrical force/Gravitational force = 10^{39}

**11.** The relationship between velocity of light, permeability of free space and permittivity of free space is given by the expression c = 1/\(\sqrt{({{\mu }_{o}}{{\varepsilon }_{o}})}\).

**12.** If two identical balls each of mass m are hung by silk thread of length ‘l’ from the same hook and carry similar charges q then.

- The distance between balls = \({{\left[ \frac{{{q}^{2}}2\ell }{4\pi {{\in }_{0}}mg} \right]}^{1/3}}\)
- The tension in the thread = \(\sqrt{{{\left( F \right)}^{2}}+{{\left( mg \right)}^{2}}}\)
- If total system is kept in space then angle between threads is 180° and tension in thread is given by T =\(\frac{1}{4\pi {{\in }_{0}}}\frac{{{q}^{2}}}{4{{\ell }^{2}}}\)
- A charge Q is divided into q and (Q – q). Then electrostatic force between them is maximum when \(\frac{q}{Q}=\frac{1}{2}\;\ (or) \;\;\;\frac{q}{\left( Q-q \right)}=1\)

## Limitations of Coulomb’s Law

- The law is applicable only for the point charges at rest.
- Coulomb’s Law can be only applied in those cases where the inverse square law is obeyed.
- It is difficult to implement Coulomb’s law where charges are in arbitrary shape because in such cases we cannot determine the distance’ between the charges.

## Problems on Coulombs Law

**Problem 1:** Charges of magnitude 100 microcoulomb each are located in vacuum at the corners A, B and C of an equilateral triangle measuring 4 meters on each side. If the charge at A and C are positive and the charge B negative, what is the magnitude and direction of the total force on the charge at C?

**Sol.**

The situation is shown in fig. Let us consider the forces acting on C due to A and B.

Now, from Coulomb’s law, the force of repulsion on C due to A i.e., FCA in direction AC is given by

FCA = \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q\times q}{{{a}^{2}}}\) along AC

The force of attraction on C due to B i.e., FCB in direction CB is given by

FCB = \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q\times q}{{{a}^{2}}}\) along CB

Thus the two forces are equal in magnitude. The angle between them is 120º. The resultant force F is given by

F = \(\sqrt{{{F}_{C{{A}^{2}}}}+{{F}_{C{{B}^{2}}}}+2{{F}_{CA}}\times {{F}_{CB}}\cos 120{}^\text{o}}\)

= \(\frac{{{q}^{2}}}{4\pi 6{{a}^{2}}} = \frac{9\times {{10}^{9}}\times {{(100\times {{10}^{-6}})}^{2}}}{{{4}^{2}}}\) = 5.625 Newton

This force is parallel to AB.

**Problem 2:** The negative point charges of unit magnitude and a positive point charge q are placed along the straight line. At what position and for what value of q will the system be in equilibrium? Check whether it is stable, unstable or neutral equilibrium.

**Sol.**

The two negative charges A and B of unit magnitude are shown in fig. Let the positive charge q be at a distance rA from A and at a distance rB from B.

Now, from coulombs law, Force on q due to A

FqA = \(\frac{1}{4\pi{{\varepsilon}_{0}}}.\frac{q}{{{r}_{A}}^{2}}\) towards A

Force on q due to B

FqB=\(\frac{1}{4\pi{{\varepsilon}_{0}}}. \frac{q}{{{r}_{B}}^{2}}\) towards B.

These two forces acting on q are opposite and collinear. For the equilibrium of q, the two forces must also be equal i.e.

| FqA | = | FqB |

or \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q}{{{r}_{A}}^{2}} = \frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q}{{{r}_{B}}^{2}}\) Hence rA = rB

So for the equilibrium of q, it must be equidistant from A & B i.e. at the middle of AB

Now for the equilibrium of the system, A and B must be in equilibrium.

For the equilibrium of A

Force on A by q = \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q}{{{r}_{A}}^{2}}\) towards q

Force on A by B = \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{(1)(1)}{{{({{r}_{A}}+{{r}_{B}})}^{2}}}\)

= \(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{1}{{{(2{{r}_{A}})}^{2}}}\) away from q

The two forces are opposite and collinear. For equilibrium the forces must be equal, opposite and collinear. Hence

\(\frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{q}{{{r}_{A}}^{2}}= \frac{1}{4\pi {{\varepsilon }_{0}}}. \frac{1}{{{(2{{r}_{A}})}^{2}}}\)or q = 1/4 in magnitude of either charge.

It can also be shown that for the equilibrium of B, the magnitude of q must be 1/4 of the magnitude of either charge.