While Oersted's surprising discovery of electromagnetism
paved the way for more practical applications of electricity, it was
Michael Faraday who gave us the key to the practical generation of
electricity: electromagnetic induction. Faraday discovered that a voltage would
be generated across a length of wire if that wire was exposed to a perpendicular
magnetic field flux of changing intensity.
An easy way to create a magnetic field of changing
intensity is to move a permanent magnet next to a wire or coil of wire.
Remember: the magnetic field must increase or decrease in intensity perpendicular
to the wire (so that the lines of flux "cut across" the conductor), or
else no voltage will be induced:
Faraday was able to mathematically relate the rate of
change of the magnetic field flux with induced voltage (note the use of a
lower-case letter "e" for voltage. This refers to instantaneous
voltage, or voltage at a specific point in time, rather than a steady, stable
The "d" terms are standard calculus notation,
representing rate-of-change of flux over time. "N" stands for the
number of turns, or wraps, in the wire coil (assuming that the wire is formed in
the shape of a coil for maximum electromagnetic efficiency).
This phenomenon is put into obvious practical use in the
construction of electrical generators, which use mechanical power to move a
magnetic field past coils of wire to generate voltage. However, this is by no
means the only practical use for this principle.
If we recall that the magnetic field produced by a
current-carrying wire was always perpendicular to that wire, and that the flux
intensity of that magnetic field varied with the amount of current through it,
we can see that a wire is capable of inducing a voltage along its own length
simply due to a change in current through it. This effect is called self-induction:
a changing magnetic field produced by changes in current through a wire inducing
voltage along the length of that same wire. If the magnetic field flux is
enhanced by bending the wire into the shape of a coil, and/or wrapping that coil
around a material of high permeability, this effect of self-induced voltage will
be more intense. A device constructed to take advantage of this effect is called
an inductor, and will be discussed in greater detail in the next chapter.
- A magnetic field of changing intensity perpendicular to
a wire will induce a voltage along the length of that wire. The amount of
voltage induced depends on the rate of change of the magnetic field flux and
the number of turns of wire (if coiled) exposed to the change in flux.
- Faraday's equation for induced voltage: e = N(dΦ/dt)
- A current-carrying wire will experience an induced
voltage along its length if the current changes (thus changing the magnetic
field flux perpendicular to the wire, thus inducing voltage according to
Faraday's formula). A device built specifically to take advantage of this
effect is called an inductor.
Lessons In Electric Circuits copyright (C)
2000-2011 Tony R. Kuphaldt, under the terms and conditions of the Design