There
are few guitarists who are totally happy with their
sound. Some people will spend thousands on gear
trying to find that elusive perfect tone, but all too
frequently the most important element in the sound
chain is neglected. Speakers are a great leveller,
you can massage your guitar sound with the finest
hand built point-to-point valve exotica, but just
like the most basic practice amps, everything ends up
as vibrations on a paper cone, so it stands to reason
that the speaker can make or break a guitar sound.
Your guitar
pickup is a transducer, it converts the kinetic
energy of a moving string into a small electrical
current. At the other end of the signal chain, the
speaker changes that electrical current back into
kinetic energy, moving a paper cone which in turn
moves air molecules to create sound.
At the
heart of your speaker is a coil of wire known as the
voice coil, passing the amplifier's output signal
through this coil generates a small magnetic field,
which is acted on by the much bigger static field of
the loudspeaker's magnet, and the end result is that
the coil moves forwards and backwards in relation to
the audio signal being passed through it.
Attach
a diaphragm or cone to that voice coil and you get
sound. In fact, a speaker is a dynamic microphone in
reverse. The voice coil, magnet and cone are three of
the speaker's four main components, number four is
the basket, a steel or alloy pressing which supports
the cone and magnet and maintains the close
tolerances necessary for the speaker to work.
Ohms
and impedance:
The most commonly misunderstood thing about
loudspeakers is impedance - the loudspeaker's voice
coil resistance. Wiring up one driver is
straightforward, but when you tackle multiple
loudspeakers in, say a 4x12 cab, things get a little
more complex. But there's no real secret - just like
any other resistor, there are only three ways to wire
up multiple drivers, series, parallel and the
series/parallel combination. Let's deal with series
wiring first in a hypothetical 4x12.
The
'hot' wire carrying the amp signal goes to the
positive tag on driver 1 - the negative tag of driver
1 is wired to the positive tag of driver 2 and so on,
with the negative tag of driver 4 going back to the
amp. The sum total resistance is D1 + D2 + D3 + D4.
If all the speakers were 4 ohm, the total impedance
would be 16 ohms. Now for parallel wiring - this time
the hot signal wire from the amp connects to all the
positive terminals, the return wire connects to all
the negative terminals.
The
sum total resistance is calculated using reciprocals
- if all the speakers were 16 ohm then you add 1/16 +
1/16 + 1/16 + 1/16 = 4/16 or 1/4, so the total load
is 4 ohms. Series/parallel wiring is when you take
two pairs of speakers each wired in series, and
connect the two pairs in parallel - or vice versa -
and the calculations are done just the same, so a
4x12 with four 8 ohm drivers wired in series/parallel
will have a total load of 8 ohms. I just used the
words 'impedance' and 'load' - in practice they mean
the same thing.
A
speaker's impedance 'loads' the amplifier's output
stage, governing the amount of power available.
Unlike a simple resistor, this impedance varies with
frequency and heat - the ohm ratings are an
indication, not a true figure. If an amp delivers 100
watts into an 8 ohm speaker, substituting a 4 ohm
unit will make the amp try to deliver more power -
the load has been reduced. If the power supply and
output devices can handle it you could expect about
140 watts into 4 ohms, but if the amp was only
designed for 100 watts into 8 ohms minimum, then
something will give, you will either blow a fuse or
an output device.
Valve
amps are even less forgiving and much more dangerous,
due to the high voltages present. A valve amp must
never run below its minimum impedance, and never,
ever run without a speaker connected. The output
transformer on a valve amp not only matches the
speakers to the valves, it also isolates the
speaker/chassis from high voltage DC - typically 400
to 500 volts - so you can see why cooking it is not a
good thing! Increasing the load is less hazardous -
both valve and solid state amps will simply deliver
less power.
If you
buy a speaker you have to check its spec, looking for
the right impedance and power handling. It's wrong to
suppose that a 100 watt speaker won't get fried by a
100 watt amp - the RMS (Root, Mean, Square) method is
the most realistic way of measuring amp power
outputs, but doesn't take peak distortion levels into
account - a 100 watt Marshall head flat out can hit
peaks of 200 watts and more.
A
speaker is it's own tone control - the size of the
cone determines the upper and lower limits of
frequency it will reproduce. The bigger the cone, the
lower the range and vice-versa. A typical 12"
driver is most efficient between 100Hz and 6KHz,
which coincidentally is perfect for electric guitars
although a 15" is sometimes used for extra low
end thump.
A
10" driver on it's own lacks bottom end, but put
four of them into one cab and you enhance the low end
response - hence the success of the legendary Fender
Bassman combo. But it's the harmonics above this
region that give a driver its tone - distinguishing
the silky-smooth midrange of an Eminence from the
'boxier' tonality of a Celestion Vintage 30 for
example. And here there's no easy tip for success -
your ears have to decide what works for you.
Back to Top