Faraday's law states that the induced emf is proportional to the rate of change of magnetic flux through the loop.

The induced emf is proportional to both the speed of the conductor and the length of the conductor when moving perpendicular to the magnetic field.

If the magnetic field strength is doubled, the induced emf also doubles, as it is directly proportional to the magnetic field strength.

According to Lenz's law, the induced current will flow in a direction that opposes the change in magnetic flux. If the magnetic field is increasing, the induced current will be counterclockwise.

Flux linkage refers to the total magnetic flux through a coil, which is the product of the magnetic flux and the number of turns in the coil.

If the magnetic field is removed, the induced current stops because there is no longer a change in magnetic flux.

The induced emf depends on the rate of change of magnetic flux, not directly on the area of the loop in a uniform magnetic field. Therefore, it remains the same if the magnetic field is constant.

The induced emf in a coil is given by Faraday's law of electromagnetic induction, which states that emf = -dΦ/dt, where Φ is the magnetic flux.

The principle behind a transformer is electromagnetic induction, where a changing magnetic field induces an emf in a secondary coil.

Induced emf is independent of the resistance of the circuit; however, the current produced will be affected by the resistance according to Ohm's law.

Lenz's law states that the direction of induced current is such that it opposes the change in magnetic flux.

The induced emf is affected by the number of turns in the coil, the rate of change of magnetic flux, and the strength of the magnetic field. The resistance of the wire does not affect the induced emf directly.