A magnetic field is a region of space where a magnetic force acts. Magnetic flux lines run from an N-pole to an S-pole and form a continuous loop (in solenoids). The magnetic flux density,
Magnetic flux,
Where:
Induction is where a changing magnetic flux in a circuit causes a electromotive force to be induced in the circuit. In real circuits, coils with many turns are used, which is why flux linkage is used. Flux linkage,
The induced e.m.f in a coil is given by:
This is known as Faraday's Law of electromagnetic induction. The negative sign is a result of Lenz's Law, which states that the induced e.m.f. in a circuit as a result of a changing magnetic field creates a current with a direction that creates a magnetic field that opposes the original change in the magnetic field.
In a magnetic circuit, the flux lines form a closed loop. Similar to conductance in electrical circuits, magnetic circuits have permeance; higher permeance means more flux. Thus, magnetic circuits are often made from ferromagnetic materials with a high magnetic permeability, for example iron. The magnetic equivalent of p.d. is current-turns
For a electric circuit, the conductance is
Transformers are electromagnetic machines that change the potential difference of electrical power. In a transformer, an alternating p.d. in the primary coil creates a changing flux in the core. This changing flux links with the secondary coil to induce a alternating p.d. in the secondary.
In the primary coil, the changing flux in the core creates a magnetic field that induces a current with a magnetic field that opposes the original alternating p.d., by Lenz's Law. This is called self-inductance.
By Faraday's Law, the e.m.f. from self-inductance is given by
For an ideal transformer,
This equation means that, loosely, all the p.d. from the supply across the primary coil is converted into magnetic flux. In the magnetic circuit, ignoring the negligibly small leakage of flux into the air, the flux in both the primary and secondary coils is equal (because of the high permeance of the circuit). Thus, if the flux is equal at all times, the change in flux in the primary and secondary coils is also equal:
Thus giving the familiar transformer equations below, where the negative sign indicates that the alternating p.d. in the secondary coil is
The ratio
An ideal transformer is perfectly efficient, thus the total power input and output are equal:
The changing flux within the core of a transformer induces currents in the transformer core itself, called eddy currents. By Lenz's law, these currents create magnetic flux that opposes the flux created by the primary coil. This wastes energy and reduces the transformer's efficiency, with the wasted energy dissipated as heat. Eddy currents can be reduced by making the core from a stack of laminations, separated by electrically insulating layers.
A generator uses motion to create a changing magnetic field, to induce an e.m.f For a coil moving at constant speeds perpendicular to a uniform magnetic field, the induced e.m.f. is given by:
For a coil with angle
By differentiating the flux linkage, we get that e.m.f. is given by:
Another way to use Faraday's Law for moving coils is that the induced e.m.f. is equal to the rate at which flux lines are cut. Generators are designed to have as large a changing flux as possible. This can be achieved by creating a stronger magnetic field, by increasing the permeance of the magnetic circuit.
When a current-carrying wire is placed in a magnetic field, the wire creates a magnetic field which adds vectorially to the existing field. This causes an asymmetric field, where the flux lines try to contract and straighten, producing a force (catapult effect). For a straight current-carrying wire perpendicular to a uniform magnetic field, the force is given by:
Where:
A motor uses an electric current to produce a magnetic field that interacts with a permanent magnetic field to cause a force and motion. A motor contains a coil that produces an upwards force on one side, and a downwards force on the other side, causing a net torque and thus rotation.
Motors and generators are the same thing. If you use a generator to deliver current to a load, there will be resistance from the generator acting as a motor. When a motor spins, it generates a back-e.m.f that opposes motion by Lenz's Law, limiting the speed of the motor.