Electric Charges and Fields

Electric Charges and Fields Class 12 Notes for CBSE Physics Exam

By ConceptScroll Team · Published on 19 June 2026 · 5 min read

Electric Charges and Fields class 12 notes provide a clear and concise overview of fundamental concepts in electrostatics. These notes help Class 12 NCERT students grasp definitions, laws, and formulas essential for CBSE Physics exams.

Understanding Electric Charges: Basics and Properties

Electric charge is a fundamental property of matter that causes it to experience a force when placed in an electromagnetic field. There are two types of charges: positive and negative. Like charges repel each other, while unlike charges attract.

Key properties of electric charges include:

  • Quantization: Charge exists in discrete amounts, multiples of the elementary charge $e = 1.6 \times 10^{-19}$ coulombs.
  • Conservation: Total electric charge in an isolated system remains constant.
  • Additivity: Net charge is the algebraic sum of individual charges.

Charges can be transferred by friction, conduction, or induction. Conductors allow free movement of charges, whereas insulators do not.

Example:

If an object gains $3 \times 10^{18}$ electrons, its net charge is:

$$Q = n \times e = 3 \times 10^{18} \times (-1.6 \times 10^{-19}) = -0.48 \text{ C}$$

This negative charge means the object has excess electrons.

Coulomb’s Law: Force Between Two Point Charges

Coulomb’s law quantifies the electrostatic force between two point charges. It states:

> The magnitude of force $F$ between two charges $q_1$ and $q_2$ separated by distance $r$ is directly proportional to the product of the charges and inversely proportional to the square of the distance between them.

Mathematically:

$$F = k \frac{|q_1 q_2|}{r^2}$$

where $k = \frac{1}{4 \pi \epsilon_0} = 9 \times 10^9 \text{ Nm}^2/\text{C}^2$ and $\epsilon_0$ is the permittivity of free space.

Direction: Force acts along the line joining the charges. It is repulsive if charges are alike and attractive if unlike.

Worked Example:

Two charges, $+2 \mu C$ and $-3 \mu C$, are 0.5 m apart. Find the force between them.

$$F = 9 \times 10^9 \times \frac{2 \times 10^{-6} \times 3 \times 10^{-6}}{(0.5)^2} = 0.216 \text{ N}$$

The force is attractive since charges are opposite.

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Electric Field: Definition and Calculation

An electric field is a region around a charged object where another charge experiences an electric force. It is a vector quantity.

Definition: Electric field $\vec{E}$ at a point is the force $\vec{F}$ experienced by a positive test charge $q$ placed at that point divided by the magnitude of the charge.

$$\vec{E} = \frac{\vec{F}}{q}$$

Units: Newton per Coulomb (N/C).

The electric field due to a point charge $Q$ at distance $r$ is:

$$E = k \frac{|Q|}{r^2}$$

Direction: Away from positive charge, towards negative charge.

Superposition Principle: The net electric field due to multiple charges is the vector sum of the fields due to individual charges.

Example:

Calculate the electric field 0.2 m from a $+5 \mu C$ charge.

$$E = 9 \times 10^9 \times \frac{5 \times 10^{-6}}{(0.2)^2} = 1.125 \times 10^6 \text{ N/C}$$

Electric Field Lines and Their Properties

Electric field lines visually represent the direction and strength of an electric field.

Key properties:

  • Lines start from positive charges and end on negative charges.
  • The number of lines is proportional to the magnitude of the charge.
  • Lines never intersect.
  • The density of lines indicates field strength; closer lines mean stronger field.
  • Field lines are perpendicular to the surface of a conductor.

Comparison Table: Electric Field Lines vs Equipotential Surfaces

FeatureElectric Field LinesEquipotential Surfaces
DirectionIndicate direction of $\vec{E}$Perpendicular to $\vec{E}$
ValueVaries along the lineConstant potential value
IntersectionNever intersectCan intersect
Relation to ChargeOriginate/terminate on chargesSurround charges

Understanding these helps in visualizing electric fields and solving related problems.

Gauss’s Law and Its Applications

Gauss’s law states:

> The total electric flux through a closed surface is equal to $\frac{1}{\epsilon_0}$ times the net charge enclosed within the surface.

Mathematically:

$$\Phi_E = \oint \vec{E} \cdot d\vec{A} = \frac{Q_{\text{enclosed}}}{\epsilon_0}$$

where $\Phi_E$ is the electric flux, $\vec{E}$ is the electric field, and $d\vec{A}$ is the area element vector.

Applications:

  • Calculating electric fields of symmetric charge distributions (spheres, cylinders, planes).
  • Deriving the electric field outside and inside a charged conductor.

Example:

For a uniformly charged sphere of radius $R$ and total charge $Q$, the electric field outside ($r > R$) is:

$$E = k \frac{Q}{r^2}$$

Inside ($r < R$), the field is zero for a conductor.

Gauss’s law simplifies complex calculations by exploiting symmetry.

Summary of Important Formulas in Electric Charges and Fields

Here is a quick reference table of key formulas:

ConceptFormulaNotes
Coulomb’s Law$F = k \frac{q_1 q_2}{r^2}$Force between two charges
Electric Field (point)$E = k \frac{Q}{r^2}$Field due to point charge
Electric Field (test)$\vec{E} = \frac{\vec{F}}{q}$Definition of electric field
Electric Flux$\Phi_E = \oint \vec{E} \cdot d\vec{A}$Flux through surface
Gauss’s Law$\Phi_E = \frac{Q_{\text{enclosed}}}{\epsilon_0}$Relates flux to enclosed charge

Use these formulas with proper units and directions for solving NCERT problems effectively.

Frequently asked questions

What is the unit of electric charge?

The unit of electric charge is the coulomb (C).

How does Coulomb’s law explain the force between charges?

Coulomb’s law states force is proportional to product of charges and inversely to square of distance.

What is the significance of electric field lines?

They show the direction and strength of the electric field visually.

How is Gauss’s law useful in electrostatics?

It helps calculate electric fields using symmetry by relating flux to enclosed charge.

Can electric field exist inside a conductor?

No, the electric field inside a conductor in electrostatic equilibrium is zero.

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