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LOUDSPEAKERS: Does the Totem Mani-2 still rate as one of the ...

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What is <strong>the</strong> impedance <strong>of</strong><br />

Nuts&Bolts Feedback<br />

Speaker Impedance<br />

your loudspeakers? Is<br />

it 8 ohms? Or 4 ohms?<br />

Perhaps you know that<br />

it is not just a single number, but what<br />

difference does it make anyway?<br />

At <strong>the</strong> very le<strong>as</strong>t you are no doubt<br />

aware that a speaker with a very low<br />

impedance can present a problem for an<br />

amplifier, and potentially can damage it.<br />

Think about <strong>the</strong> fact that short-circuiting<br />

an amplifier output can ei<strong>the</strong>r break<br />

it, or blow a fuse, or trigger a protection<br />

circuit. The lower <strong>the</strong> impedance <strong>of</strong><br />

a loudspeaker, <strong>the</strong> closer it comes to<br />

being a short circuit. Some amplifiers<br />

can drive a load <strong>of</strong> 2 Ω or even 1 Ω, but<br />

most will not. (The Greek letter Omega<br />

is <strong>of</strong> course <strong>the</strong> symbol for resistance).<br />

In any c<strong>as</strong>e, low impedance may not be<br />

your only worry.<br />

With this issue, UHF intends to begin<br />

publishing impedance curves for loudspeakers<br />

reviewed, and for that re<strong>as</strong>on<br />

I have been <strong>as</strong>ked to explain speaker<br />

impedance, and also to suggest a simple<br />

manner <strong>of</strong> me<strong>as</strong>uring a speaker's impedance.<br />

“Simple” in this c<strong>as</strong>e means using a<br />

minimum <strong>of</strong> specially-purch<strong>as</strong>ed equipment,<br />

though in day-to-day operation it<br />

is less simple than using a purpose-built<br />

instrument that can spit out a complete<br />

impedance graph in a few seconds. Yes,<br />

impedance me<strong>as</strong>urements result in a<br />

ULTRA HIGH FIDELITY Magazine<br />

graph, not just <strong>the</strong> single figure usually<br />

found in loudspeaker literature, but let<br />

me begin with some b<strong>as</strong>ic concepts.<br />

What is impedance?<br />

If a loudspeaker were to be driven<br />

by DC (direct current) we could speak<br />

simply <strong>of</strong> its resistance. The speaker’s<br />

internal wiring h<strong>as</strong> a certain (low) resistance,<br />

<strong>as</strong> does <strong>the</strong> fine wire that makes up<br />

each driver’s voice coil. However loudspeakers<br />

are intended to be driven by AC<br />

(alternating current), whose frequency <strong>of</strong><br />

alternation is that <strong>of</strong> <strong>the</strong> sound we are<br />

attempting to reproduce. Thus we need<br />

to take into account <strong>the</strong> speaker’s inductance<br />

and capacitance. The voice coil is an<br />

inductor, and <strong>the</strong> internal wiring may be<br />

<strong>as</strong> well. Inductance can be thought <strong>of</strong> <strong>as</strong><br />

a resistance that is frequency-dependent,<br />

with its ohm value rising <strong>as</strong> frequency<br />

drops. Most crossover networks include<br />

capacitors, which introduce capacitance.<br />

A capacitor can also be thought <strong>of</strong> <strong>as</strong> a<br />

frequency-dependent resistor, whose<br />

ohm value rises with frequency. Since a<br />

capacitor’s impedance characteristic is<br />

exactly opposite to that <strong>of</strong> an inductor, it<br />

is e<strong>as</strong>y to see how capacitors and inductors<br />

can be combined to make filters.<br />

I shall add, without great elaboration,<br />

that <strong>the</strong>se are not <strong>the</strong> only factors<br />

by Paul Bergman<br />

determining <strong>the</strong> impedance reflected<br />

back to <strong>the</strong> amplifier. For example, <strong>as</strong><br />

a wo<strong>of</strong>er c<strong>one</strong> moves back and forth,<br />

acting <strong>as</strong> a linear motor, it also acts <strong>as</strong> a<br />

generator, actually generating a voltage<br />

that is opposite to that coming from <strong>the</strong><br />

amplifier. That this complicates things<br />

is an understatement.<br />

It must also be evident that, in a<br />

speaker that combines resistance, inductance<br />

and resistance, <strong>the</strong> total impedance<br />

cannot be a single number, since it will<br />

inevitably vary with frequency. This is<br />

not typically taken into consideration by<br />

designers <strong>of</strong> amplifiers, who test <strong>the</strong>ir<br />

designs by loading <strong>the</strong>m with an 8 ohm<br />

resistor, possessing nei<strong>the</strong>r capacitance<br />

nor inductance, and having a constant<br />

impedance at all frequencies.<br />

The ideal, and <strong>the</strong> practical<br />

The closer a speaker is to a pure<br />

resistance, <strong>the</strong> more confidence an<br />

amplifier designer can have that his<br />

product will behave in <strong>the</strong> customer’s<br />

home exactly <strong>as</strong> it did on <strong>the</strong> test bench.<br />

That said, few loudspeakers are very<br />

much like resistors at all, and so in fact<br />

amplifiers must be designed to ope<strong>rate</strong><br />

with impedances that are v<strong>as</strong>tly different<br />

from that ideal resistor. What is more,<br />

<strong>the</strong> designer cannot know in advance <strong>the</strong><br />

characteristics <strong>of</strong> <strong>the</strong> speakers that will<br />

be used with his product.<br />

To see what he (and we) are up<br />

against, let us look at <strong>the</strong> impedance<br />

curve <strong>of</strong> a small two-way speaker, which<br />

h<strong>as</strong> a famous name I do not propose to<br />

reveal. It is shown on <strong>the</strong> next page.<br />

The curve h<strong>as</strong> been drawn by a<br />

technique I shall describe presently<br />

(see Me<strong>as</strong>uring Impedance on page 20).<br />

Most speakers, I might add by way <strong>of</strong><br />

explanation, have a considerable peak in<br />

impedance at <strong>the</strong> point <strong>of</strong> resonance <strong>of</strong><br />

<strong>the</strong> wo<strong>of</strong>er and cabinet. The <strong>one</strong> I have<br />

arbitrarily selected h<strong>as</strong> only a small rise,<br />

centred around 100 Hz, which would<br />

be <strong>the</strong> practical lower limit <strong>of</strong> its b<strong>as</strong>s<br />

response.<br />

The manufacturer’s nominal impedance<br />

rating is 4 Ω, but you need only<br />

glance at <strong>the</strong> curve to see that it deviates<br />

from that rating quite considerably. It<br />

dips to about 3 Ω at 16 Hz, which should<br />

present little problem for an amplifier<br />

designed <strong>the</strong> le<strong>as</strong>t bit competently.

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