Physics > Electrostatics > 2.0 Electric charge
Electrostatics
1.0 Introduction
2.0 Electric charge
3.0 Coulomb's law
3.1 Coulomb's law in vector relations
3.2 Comparision between coulomb's force and gravitational force
4.0 Principle of superposition
5.0 Continuous charge distribution
6.0 Electric field
6.1 Electric field due to a point charge
6.2 Electric field due to a ring of charge
6.3 Electric field due to a line of charge
7.0 Electric field lines
8.0 Insulators and conductors
9.0 Gauss's law
9.1 Electric field due to a point charge
9.2 Electric field due to a linear charge distribution
9.3 Electric field due to a plane sheet of charge
9.4 Electric field near a charged conducting surface
9.5 Electric field due to a charged spherical shell or solid conducting surface
9.6 Electric field due to a solid sphere of charge
10.0 Work done
10.1 Work done by electrical force
10.2 Work done by external force
10.3 Relation between work done by electrical & external force
11.0 Electric potential energy
12.0 Electric Potential
12.1 Properties
12.2 Use of Potential
12.3 Potential Due to Point Charge
12.4 Potential due to a Ring
12.5 Potential Due to Uniformly charged Disc
12.6 Potential Due To Uniformly Charged Spherical Shell
12.7 Potential Due to Uniformly Charged Solid Sphere
13.0 Electric dipole
13.1 Electric field due to a dipole at axial point
13.2 Electric field on equatorial line
13.3 Electric field at any point
13.4 Dipole in an external electric field
13.5 Potential due to an electric dipole
2.1 Basic properties of electric charge
3.2 Comparision between coulomb's force and gravitational force
6.2 Electric field due to a ring of charge
6.3 Electric field due to a line of charge
9.2 Electric field due to a linear charge distribution
9.3 Electric field due to a plane sheet of charge
9.4 Electric field near a charged conducting surface
9.5 Electric field due to a charged spherical shell or solid conducting surface
9.6 Electric field due to a solid sphere of charge
10.2 Work done by external force
10.3 Relation between work done by electrical & external force
12.2 Use of Potential
12.3 Potential Due to Point Charge
12.4 Potential due to a Ring
12.5 Potential Due to Uniformly charged Disc
12.6 Potential Due To Uniformly Charged Spherical Shell
12.7 Potential Due to Uniformly Charged Solid Sphere
13.2 Electric field on equatorial line
13.3 Electric field at any point
13.4 Dipole in an external electric field
13.5 Potential due to an electric dipole
- Charge is invariant: It is independent of frame of reference.
- Charge is transferable: Process of charge transfer is called conduction.
- Charge is a scalar quantity and can be of two types (i.e. $+ve$ or $-ve$). It is added algebraically.
- Charge is conserved. During any chemical, nuclear, decay etc, the net electric charge of an isolated system remains constant.
- Current is known as the drift of charge per unit time. So, the charge is expressed as, $$q=It$$
- The SI unit for measuring the magnitude of an electric charge is the coulomb $(C)$.
- If a charge of $1$ coulomb drift per second through an unit cross-section of conductor then the current flowing is called as $1$ ampere.
- Charge is quantized: Robert Millikan discovered that electric charge always occurs as some integral multiple of fundamental unit of charge $(e)$.
$$q=ne$$ where $n$ is an integer and it corresponds to the number of electrons. - Charge on a body can never be $\left( {\frac{1}{3}} \right)e$, $\left( {\frac{2}{3}} \right)e$ etc as it is due to transfer of electron.
- Charge is always associated with mass. i.e. charge cannot exist without mass. However mass can exist without charge.
- When charge particle is at rest it produces only electric field.
- When charged particle is accelerated it produces electric field $+$ magnetic field $+$ radiate energy.