# Coulomb’s law examples and problems

*“Coulomb’s law states that force of attraction or repulsion between two electric charges is directly proportional to their magnitudes and inversely proportional to the square of the distance between them”.Coulomb’s law examples are given below.*

Charles Agustin Coulomb (1736-1806) measured electrical attractions and repulsion quantitatively and deduced the law that governs them.

This figure resembles the figure given below:

If a and b are charged, the electric force on a tends to twist the suspension fiber. Coulomb canceled out this twisting effect by turning the suspension head through the angle θ needed to keep the two charges at a particular separation. The angle θ is then a relative measure of the electric force acting on charge a. The device of the above figure is a torsion balance,a similar arrangement was used latter by Cavendish to measure gravitational attractions.

## Coulomb’s Law Derivation

This relation is called coulomb’s law. Here F is called the magnitude of the mutual force that acts on each of the two charges a and b, q_{1 }and q_{2} are relative measures of the charges on spheres a and b, and r is the distance between their centers. The force on each charge due to the other acts along the line connecting the charges. The two forces point in opposite directions but have equal magnitudes, even though the charges may be different. The two forces point in opposite directions but have equal magnitudes, even though the charges may be different.

## Coulomb’s constant

To turn the above proportionality into an equation,let us introduce a constant of proportionality, which we represent for now as k .Its value depends upon the system of units and medium between the charges. For free space and in system international ‘k’ is expressed as:

## Permittivity of free space

Where ε_{0} is the permittivity of free space and its value is 8.85 × 10^{-12}C^{-2}N^{-1}m^{-2}.

we thus obtain, for the force between the charges. Coulomb’s law generally holds only for charged objects whose sizes are much smaller than the distance between them. We often say that it holds only for point charges.

Our belief in coulomb’s law does not rest quantitatively on coulomb’s experiments. Torsion balance measurements are difficult to make to an accuracy of better than a few percent.

Coulomb law resembles Newton,s inverse square **law of gravitation**, which was already more than 100 years old at the time of Coulomb’s experiments. Both are inverse-square laws, and the charge q plays the same role in Coulomb’s law that the mass m plays in **Newton’s law of gravitation**. One difference between the two laws is that gravitational forces, as far as we know, are always attractive, while electrostatic forces can be repulsive or attractive, depending on whether the two charges have the same or opposite signs.

There is another important difference between the two laws. In using the law of gravitation, we were able to define mass from **Newton’s second law**, and then by applying the law of gravitation to know masses we could determine the constant G.in using Electrostatic force law, we take the reverse approach;we define the constant k to have a particular value, and we then use Coulomb’s law to determine the basic unit of electric charge as the quantity of charge that produces a standard unit of force.

For example, consider the force between two equal charges of magnitude q. We could adjust q until the force has a particular value, say 1 N for separation of r=1m, and define the resulting q as the basic unit of charge. It is, however, more precise to measure the magnetic force between two wires carrying equal currents, and therefore the fundamental SI electrical unit is the unit of current, from which the unit of charge is derived. The operational procedure for defining the SI unit of current , which is called the ampere.

## Coulomb’s law in vector form

Coulomb’s force is a mutual force, it means that if charge ‘q_{1}‘ exerts a force on charge ‘q_{2}‘ then q_{2} also exerts an equal and opposite force on q_{1}.

If charge q_{1 }exerts an electrostatic force “**F _{12}**“

_{ }charge q

_{2}and q

_{2}exerts electrical force F

_{21 }on charge q

_{1}.

If r_{12} represents the direction of force from charge q_{1 }to charge q_{2 }and r_{21 }is the unit vector which represents the direction of force from charge q_{2 }to q_{1}, then:

According to newton’s 3rd law:

F_{21}=-F_{12}

This expression shows that the Coulomb force is a mutual force.

## Significance of vector form of coulomb law

The vector form of coulomb law has critical importance when there is an assembly of point charges. In this case, the resultant force on any one of the charges is the vector sum of the forces due to each of the other forces. This is called the principle of superposition.

## Coulomb’s law examples in physics

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