Summary
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The magnetic flux through a surface of area A placed in a uniform magnetic field B is defined as,
where θ is the angle between B and A. - Faraday’s laws of induction imply that the emf induced in a coil of N turns is directly related to the rate of change of flux through it,
Here is the flux linked with one turn of the coil. If the circuit is closed, a current is set up in it, where R is the resistance of the circuit. - Lenz’s law states that the polarity of the induced emf is such that it tends to produce a current which opposes the change in magnetic flux that produces it. The negative sign in the expression for Faraday’s law indicates this fact.
- When a metal rod of length l is placed normal to a uniform magnetic field B and moved with a velocity v perpendicular to the field, the induced emf (called motional emf) across its ends is
- Changing magnetic fields can set up current loops in nearby metal (any conductor) bodies. They dissipate electrical energy as heat. Such currents are eddy currents.
- Inductance is the ratio of the flux-linkage to current. It is equal to
. - A changing current in a coil (coil 2) can induce an emf in a nearby coil
(coil 1). This relation is given by,
The quantity is called mutual inductance of coil 1 with respect to coil 2. One can similarly define . There exists a general equality, - When a current in a coil changes, it induces a back emf in the same coil. The self-induced emf is given by,
L is the self-inductance of the coil. It is a measure of the inertia of the coil against the change of current through it. - The self-inductance of a long solenoid, the core of which consists of a magnetic material of relative permeability
, is given by where A is the area of cross-section of the solenoid, l its length and n the number of turns per unit length. - In an ac generator, mechanical energy is converted to electrical energy by virtue of electromagnetic induction. If coil of N turn and area A is rotated at ν revolutions per second in a uniform magnetic field B, then the motional emf produced is
where we have assumed that at time t = 0 s, the coil is perpendicular to the field.