## ▶Introduction

The study of static charges is called **electrostatics** and this complete electrostatic will be discussed in two chapters. In this chapter, we begin with a discussion of electric charge, some properties of charged bodies, and the fundamental electric force between two charged bodies.

## ▶What is Electric Charge?

** Electric Charge** is a fundamental property of a matter which is responsible for electric forces between the bodies. Two electrons placed at a small separation are found to repeal each other, this **repulsive force** (**Electric force**) is only because of the **electric charge** on electrons.

When a **glass rod** is rubbed with **silk**, the rod acquires one kind of
charge and the silk acquires the second kind of charge. This is true for any pair of objects that are rubbed to be **electrified**. Now if the electrified
glass rod is brought in contact with **silk**, with which it was rubbed, they no longer attract each other.

### Types of Electric Charge

There are two types of charges that exist in our nature.

**Positive Charge****Negative Charge**

If any object loses its electrons then they get a **positive charge**. It is denoted by (+q) sign. If any object gain electrons from another object then it gets a **negative charge**. It is denoted by (-q) sign. The charges were named as positive and negative by the American scientist **Benjamin Franklin**. If an object possesses an electric charge, it is said to be **electrified** or **charged**. When it has no charge it is said to be
**neutral**.

**Read also:** Electrostatic Potential and Capacitance Class 12 Physics Notes Chapter 2

## ▶Basic Properties of Electric Charge

The important properties and characteristics of electric charge are given below.

**(i) Attraction and Repulsion:-** Like charges repel each other while unlike charges attract each other.

**(ii) Electric Induction:-** When a charged object brings to contact with another uncharged, it gets the opposite charge of the charged object. It is called **charging by induction**.

**(iii) Charge is Quantized:-** An object that is electrically charged has an excess or deficiency of some whole number of **electrons**. Since electrons cannot be divided into **fractions** of electrons, it means that the charge of an object is a whole-number multiple of the charge of an electron. For example, it cannot have a charge equal to the charge of 0.5 or 1000.5 electrons.

Mathematically q = ± ne, Here n = 1, 2, 3
and e = 1.6 × 10^{–19} coulomb.

**(iv) Electric Charge is Conserved:-** According to this property, "An electric charge neither can be created nor can be destroyed" i.e. total net **charge** of an isolated system is always conserved. Thus, when a glass rod is rubbed with silk cloth, both glass rod, and silk cloth acquire opposite charges in the same quantity. Thus, the total amount of charge remains the same before rubbing as well as after rubbing.

**Read also:** Solid State Class 12 Chemistry Notes Chapter 1

## ▶Conductors and Insulators

Some substances easily allow the passage of **electricity** through them while others do not. Substances that allow
electricity to pass through them easily are called ‘**conductors**’. They have electrons that are free to move inside
the material. Metals, human and animal bodies, earth, etc. are examples of **conductors**. Non-metals e.g., glass,
plastic, and wood are ‘**insulators**’ because they do not easily allow the passage of electricity through them.

Most
substances are either conductors or insulators. There is a third category called ‘**semiconductors**’ which are
intermediate between conductors and insulators because they partially allow movement of charges through them.

## ▶Charging by Induction

Now as we know that two oppositely charged bodies attract each other. But it also has been our observation
that a charged body attracts a neutral body as well. This is explained on the basis of **charging by induction**.
In the induction process, two bodies (at least one body must be charged) are brought very close, but they never
touch each other.

Charging by Induction |

**Read also:** Conceptual Questions for Class 12 Physics Chapter 1 Electric Charges and Fields

Let us examine how a charged body attracts an uncharged body. Imagine a conducting or partially conducting body (sphere here) is kept on an insulating stand and a charged rod (positive, for example) is brought very close to it. It will attract electrons to its side and the farther end of the sphere will become positively charged as it is deficient in electrons.

## ▶Coulomb’s Law

In 1785 **Charles Coulomb** (1736-1806) experimentally established the fundamental law of electric force between
two stationary charged particles. He observed that An electric force between two charged particles has the following properties:

- It is directed along a line joining the two particles and is inversely proportional to the square of the separation distance r, between them.

- It is proportional to the product of the magnitudes of the charges, |q
_{1}| and |q_{2}|, of the two particles.

- It is attractive if the charges are of opposite sign and repulsive if the charges have the same sign.

From these observations, Coulomb proposed the following mathematical form for the electric force between
two charges. The magnitude of the electric force **F** between charges q_{1} and q_{2} separated by a distance **r** is given by

`F=k\frac{|q_{1}||q_{1}|}{r^{2}}`

where k is a constant called the **Coulomb constant**.
The proportionality constant k in Coulomb’s law is similar to **G** in Newton’s law of gravitation. Instead of being
a very small number like G (6.67 × 10^{–11}), the electrical proportionality constant k is a very large number. It
is approximately

k = 8.9875 × 10^{9} N-m^{2}C^{–2}

The constant k is often written in terms of another constant, ε_{0}, called the permittivity of free space. It is related
to k by

`k=\frac{1}{4\pi \epsilon_o}`

`\therefore F=\frac{1}{4\pi \epsilon_o}\frac{|q_{1}||q_{1}|}{r^{2}}`

`\epsilon_o=\frac{1}{4\pi k}=8.85\times 10^{-12}` C^{2} / Nm^{2}

## ▶Electric Field

A charge produces something
called an **electric field** in the space around it and this electric field exerts a force on any charge (except the
source charge itself) placed in it. The electric field has its own existence and is present even if there is no
additional charge to experience the force.

### ▶Intensity of Electric Field

**The intensity of the electric field** due to a charge configuration at a point is defined as the force acting on a unit positive charge at this point. Hence if a charge q experiences an electric force **F** at a point then the intensity of the electric field at this point is given as

**E** = **F** / q

It has S.I. units of newtons per coulomb (N/C).

## ▶Electric Field due to a Point Charge

To determine the direction of an **electric field**, consider a point charge q as a source charge. This charge
creates an **electric field** at all points in the space surrounding it. A test charge q_{0} is placed at point P, a distance r from the source charge. According to **Coulomb’s law**, the
force exerted by q on the test charge is

`F=\frac{1}{4πε_0}\frac{qq_0}{r^2}`

This force is directed away from the source charge q, since the electric field at P, the position of the test charge, is defined by

`E=\frac{F}{q_0}`

we find that at P, the electric field created by q is

`E=\frac{1}{4πε_0}\frac{q}{r^2}`

## ▶Electric Field Lines

**Electric field lines** are a way of pictorially mapping the electric
field around a configuration of charges. An **electric field line** is, in general, a curve drawn in such a way that the tangent to it at each
point is in the direction of the net field at that point. The field lines follow some important general properties:

- The tangent to
**electric field lines**at any point gives the direction of the electric field at that point.

- In free space, they are continuous curves that emerge from a positive charge and terminate at a negative charge

- They do not intersect each other. If they do so, then it would mean two directions of the electric field at the point of intersection, which is not possible.

- Electrostatic field lines do not form any closed loops. This follows from the conservative nature of the electric field

## ▶Electric Dipole

A configuration of two charges of the same magnitude q, but of opposite sign, separated by a small distance
(say 2a) is called an **electric dipole**.

**The dipole moment** for an electric dipole is a vector quantity directed from the negative charge to the positive charge and its magnitude is p = q × 2a (charge × separation). The SI unit of dipole moment is C-m (**coulomb-metre**).

Electric Dipole |

## ▶Electric Field Strangth due to Electric Dipole

### ▶(i) At Axial Position

The net electric field at P

`E=\vec{E_1}+\vec{E_2}`, where E_{1} and E_{2} are fields due to +q and –q respectively

`E_1=\frac{1}{4\pi\epsilon_0}\frac{q}{(r-a)^2}` .....(1)

`E_2=\frac{1}{4\pi\epsilon_0}\frac{-q}{(r+a)^2}` .....(2)

`E=E_{1}+E_{2}`

From eq. (1) and (2)

`E=\frac{q}{4\pi\epsilon_0}[\frac{1}{(r-a)^2}-\frac{1}{(r+a)^2}]`

`E=\frac{q}{4\pi\epsilon_0}[\frac{(r+a)^2-(r-a)^2}{(r^{2}-a^{2})^2}]`

`E=\frac{q}{4\pi\epsilon_0}\frac{4ar}{(r^{2}-a^{2})^2}`

`E=\frac{1}{4\pi\epsilon_0}\frac{2(2aq)r}{(r^{2}-a^{2})^2}`

`E=\frac{1}{4\pi\epsilon_0}\frac{2Pr}{(r^{2}-a^{2})^2}`

For a short dipole, a is very small in comparison

`\therefore r^{2}-a^{2}\approx r^2`

`E=\frac{1}{4\pi\epsilon_0}\frac{2P}{r^3}`

### ▶(ii) At Broad side on Position

Electric field vector due to +q is

`E_1=\frac{1}{4\pi\epsilon_0}\frac{q}{(r^{2}+a^2)}`

Electric field vector due to –q is

`E_2=\frac{1}{4\pi\epsilon_0}\frac{q}{(r^{2}+a^2)}`

Resultant field at P is,

`E=E_{1}cos\theta+E_{2}cos\theta`

`E=\frac{1}{4\pi\epsilon_0}\frac{q}{(r^{2}+a^2)}cos\theta+\frac{1}{4\pi\epsilon_0}\frac{q}{(r^{2}+a^2)}cos\theta`

`E=\frac{1}{4\pi\epsilon_0}\frac{2q}{(r^{2}+a^2)}cos\theta`

`E=\frac{1}{4\pi\epsilon_0}\frac{2q}{(r^{2}+a^2)}\frac{a}{\sqrt{r^{2}+a^2}}`

`E=\frac{1}{4\pi\epsilon_0}\frac{2aq}{(r^{2}+a^2)^{\frac{2}{3}}}`

`E=\frac{1}{4\pi\epsilon_0}\frac{P}{(r^{2}+a^2)^{\frac{2}{3}}}`

For a short dipole

`\therefore r^{2}+a^{2}\approxr^2`

`E=\frac{1}{4\pi\epsilon_0}\frac{P}{(r^{2}+a^2)^3}`

## ▶Torque of Electric Dipole in uniform Electric Field

An electric dipole is placed in a uniform electric field E

The force experienced by the dipole is

F = qE

The two forces form a couple and it tries to turn the dipole. The torque due to the couple is given by

τ = either force × perpendicular distance between the forces

τ = qE × (2a sin θ)

τ = (2aq) E sin θ

τ = pE sin θ

τ = p × E

## ▶Electric Flux

The number of electric field lines that are passing perpendicular through the unit surface of any plane is called **electric flux**. Consider an electric field that is uniform in both magnitude and direction, as in the figure.

We can write this as N ∝ **EA**, which means
that the number of **field lines** is proportional to the product of **E** and **A**. This is a measure of **electric flux**
and is represented by the symbol φ. In the above case, φ = **EA **cosθ. The SI unit of electric flux is N-m^{2}/C or V-m(volt-metre).

## ▶Solid Angle

A solid angle is defined as an angle that is made at a point in place by an area. The SI unit of solid angle is steradian, and it is expressed as 'sr'.

`sr=\frac{dA\cos\theta}{r^2}`

## ▶Gauss’s Law

It states that the **electric flux** Φ through any closed surface is equal to (1/ε_{o}) times the net charged q enclosed by the surface. That is

`\phi =\int E.dS=\frac{q}{\epsilon_o}`

**Proof:** Consider a point charge q surrounded by a spherical surface of radius r centered on the charge. The magnitude of the electric field everywhere on the surface of the sphere is

`E=\frac{1}{4πε_0}\frac{q}{r^2}` ......(1)

The electric field is perpendicular to the spherical surface at all points on the surface. The electric flux through the surface is

`\phi_{E}=\int EA\cos\theta` .....(2)

Putting the value of E from eq. (1)

`\phi_{E}=\int \frac{1}{4πε_0}\frac{q}{r^2}A\cos\theta`

`\phi_{E}=\frac{q}{4πε_0}\int \frac{A\cos\theta}{r^2}`

`\phi_{E}=\frac{q}{4πε_0}\int d\omega`

`\phi_{E}=\frac{q}{4πε_0} 4\pi`

`\phi_{E}=\frac{q}{ε_0}`

This result says that the electric flux through a sphere that surrounds a charge q is equal to the charge divided by the constant ε_{0}

Let us note some important points regarding this law:

- Gauss’s law is true for any closed surface, no matter what its shape or size.

- The term q on the right side of Gauss’s law, includes the sum of all charges enclosed by the surface.

- Gauss’s law is often useful for a much easier calculation of the electrostatic field when the system has some symmetry.

- Gauss’s law is based on the inverse square dependence on distance contained in Coulomb’s law.

## ▶Application of Gauss’s Law

- It is used to calculate electric field due to an
**infinitely long straight uniformly charged wire**.

- It is also used to calculate electric field due to a uniformly charged infinite plane sheet.

- It is also used to calculate electric field due to a
**uniformly charged thin spherical shell**.

### (i). Electric field strength due to an infinitely long straight uniformly charged wire

Let a charged wire of infinite length be +q charge and its linear charge density λ be. To calculate the electric field due to this wire, let us assume a cylindrical Gaussian surface of radius r. Let the area of this Gaussian surface be dS_{1}, dS_{2}, dS_{3}.

Hence the total electric flux passing through the first surface dS_{1},

`\phi_{1}=\oint E.dS_1 cosθ`

`\phi_{1}=\oint E.dS_1 cos90°`

`\phi_1=0` .....(1)

Similarly, the total electric flux passing through the second surface dS_{2},

`\phi_{2}=\oint E.dS_2 cosθ`

`\phi_{2}=\oint E.dS_2 cos0`

`\phi_{2}=\oint E.dS_2`

`\phi_{2}=E\oint dS_2`

`\phi_{2}=E(2\pi rl)` .....(2)

Similarly, the total electric flux passing through the third surface dS_{3},

`\phi_{3}=\oint E.dS_3 cos90°`

`\phi_3=0` .....(3)

Hence, the total electric flux passing through the Gaussian surface,

`\phi=\phi_1+\phi_2+\phi_3`

`\phi=0+E.2\pi rl+0`

`\phi=E.2\pi rl` .....(4)

Putting `\phi= \frac{q}{\epsilon_0}` from Gauss's theorem,

`\frac{q}{\epsilon_0}=E.2\pi rl`

`E=\frac{\frac{q}{l}}{2\pi r\epsilon_0}`

`E=\frac{\lambda}{2\pi r\epsilon_0}`

## ▶Deduction of Coulomb’s law from Gauss' Law

Consider a charge +q in place at origin in a vacuum. We want to calculate the electric field due to this charge at a distance r from the charge. Imagine that the charge is surrounded by an imaginary sphere of radius r as shown in the figure below. This sphere is called the **Gaussian sphere**.

Consider a small area element d**S** on the Gaussian sphere. We can calculate the flux through this area element due to charge as follows:

`\oint \vec{E}.\vec{dS}=E\int dS`

`\oint \vec{E}.\vec{dS}=E(4\pi r^2)`

Using this in Gauss theorem we get

`E(4\pi r^2)=\frac{q}{\epsilon_0}`

`E=\frac{1}{4\pi\epsilon_0}\frac{q}{r^2}`

We know that

`F=Eq_0`

`F=\frac{1}{4\pi\epsilon_0}\frac{qq_0}{r^2}`

This is the required Coulomb’s law obtained from the Gauss theorem.

## ▶Summary

A charge is a property associated with the matter due to which it produces and experiences electrical and magnetic effects.

The force between two point charges at rest varies directly as the product of the magnitude of each charge and inversely as the square of the distance between them.

The force experienced by a unit positive point charge is called electric field intensity.

A field line is an imaginary curve, such that the tangent to which at a point gives the direction of the electric field at that point.

If two equal and opposite point charges q are separated by a distance of 2a, then the electric dipole moment is defined as a vector quantity having magnitude p = q × 2a and direction from negative to positive charge.

The electric flux through an elementary area vector ds is defined as the dot product of electric field intensity E and ds.

The total electric flux linked with a closed surface is (1/ε

_{o}) times the net charge enclosed by the closed surface.