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Faraday’s law
… Law of Electromagnetic Induction states that the induced electromotive force (EMF) in a circuit is directly proportional to the rate of change of magnetic flux through the circuit.
If the magnetic field through a coil changes—either by varying the field strength, the area of the loop, or the angle—the coil experiences an induced voltage (EMF), which can drive an electric current if a closed circuit is present.
Lenz’s law
states that the direction of the induced current in a conductor is always such that it opposes the change in magnetic flux that caused it.
If the magnetic flux through a loop increases, the induced current will flow in a direction that creates a magnetic field opposing this increase.
If the flux decreases, the induced current will generate a field that tries to maintain it.
… Law ensures that energy is conserved by opposing the change that produces the induced current.
Coulomb’s law
states that the electrostatic force between two point charges is directly proportional to the product of their charges and inversely proportional to the square of the distance between them.
If the charges have the same sign (+/++/+ or −/−−/−), the force is repulsive.
If the charges have opposite signs (+/−+/−), the force is attractive.
The force follows an inverse square law, meaning that if the distance doubles, the force becomes one-fourth as strong.
Equipotential lines
Equipotential lines (or equipotential surfaces in 3D) are imaginary lines in an electric field where every point has the same electric potential. This means that no work is required to move a charge along an equipotential line because the electric potential remains constant.
Always Perpendicular to Electric Field Lines
Electric field lines show the direction of force on a positive charge, while equipotential lines are always at right angles to these field lines.
This ensures that no work is done when moving a charge along an equipotential line.
Closer Equipotential Lines Indicate Stronger Fields
When equipotential lines are closer together, the electric field is stronger.
When they are farther apart, the field is weaker.
No Work Done Along Equipotential Lines
Since the potential remains the same, moving a charge along an equipotential surface does not require energy.
Examples in Different Fields:
Uniform Electric Field: Equipotential lines are equally spaced, straight, and parallel.
Point Charge: Equipotential lines are concentric circles (or spheres in 3D) centered around the charge.
Dipole: Equipotential lines form complex curved shapes around the positive and negative charges.
Electrical circuits: Helps in designing capacitors and insulators.
Geophysics: Used to map gravitational and electric potentials.
Medical applications: Helps in electrocardiograms (ECGs) and brain activity mapping.
Internal energy
Total potential energy and random kinetic energy of all the particles in a substance.
Boyle’s law
For a fixed mass of gas at constant temperature the pressure is inversely proportional to the volume. PV = constant
Travelling waves
Transfer energy from one place to another as it moves.
Standing waves
Formation:
Do not transfer energy
Mechanical waves
Require a medium to travel in
Electromagnetic waves
Do not require a medium and can travel in a vacuum.
Longitudinal waves
Direction of energy is parallel to the motion of the particles.
Rarefactions and compressions.
Sound waves
Transverse waves
Motion of particles is perpendicular to the energy transfer.
Crests and troughs
Light waves/EM waves
Gravitational potential energy
Ep
Work done against gravity to assemble the system from an infinite separation of the components.
Gravitational potential
Vg
Work done per unit mass in bringing an object from infinity.