Electric Charges and Field
We began by defining the electric field at any point in space as the total Coulomb force per unit positive charge at that point.
This shift from discussing forces between existing charges to fields that exist at points in space is a major reorientation
- Electric charge is a basic property of all matter.
- Unlike charges attract, like charges repel.
- Conductor allow flow of electric charges through them while insulators don't
- Electric charges have three basic properties
- Additivity
- Quantisation
- Conservation
Coulomb's law:
- the Electrostatic force of interaction between two point electric charges is directly proportional to the product of the charges,
- inversely proportional to the square of the distance between them
- act along the straight line joining the two charges.
Superposition Principle:
The electric intensity at a point due to several
charges is thevector sum of electric intensities produced by each
charge individually in the absence of other charges.
Electric field
the region of space around a charge or a system of
charges within which other charged particles
experiences an electrostatic force.
charges within which other charged particles
experiences an electrostatic force.
Electric field line
an imaginary straight or curved path along which a unit positive charge is supposed to move when free to do so in any electric field.
Various properties of Electric field lines:
(a) lines are continuous
(b) two field lines cannot cross each other.
(c) Field lines start from positive charge to negative and
cannot form closed loops.
Electric dipole
- a pair of equal and opposite point charges separated by a small distance.
- Electric field generated by an electric dipole.
- The additional charge in the system destroys the spherical symmetry and thereby complicates the general calculation of the field.
- In a uniform electric field, a dipole experiences a torque, and net force becomes zero.
Continuous charge distribution
- an infinite line of charge.
- has cylindrical symmetry about the line of charge; the direction of the field is perpendicular to the line and the magnitude of the field decreases as 1/r.
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