November 1958 Popular Electronics
Table
of Contents
Wax nostalgic about and learn from the history of early electronics. See articles
from
Popular Electronics,
published October 1954  April 1985. All copyrights are hereby acknowledged.

Decibels always have been and always will be a daunting subject
to a lot of people. For electronics types, the issue of when to
multiply the logarithm of the ratio by 10 or by 20 seems to be the
biggest stumbling block. After many years of working with decibels,
it becomes second nature. There are still instances, though, where
I see seasoned engineers and technicians routinely confuse unreferenced
decibel units (dB, the logarithm of a ratio) with logs of ratios
referred to some base value (dBm, dBV, etc.). The bel unit
was originally created to quantitatively assign changes in perceived
levels of sound loudness to the human ear. This article touches
briefly on the history and application of the bel.
After Class: Special Information on Radio, TV,
Radar and Nucleonics
Understanding Decibels
The decibel is probably least understood unit in electronics.
Ask what an ampere is and you'll get the answer, "It's a unit of
current measurement." Ask for the definition of an ohm and, "It's
the unit of electrical resistance," is your answer. Now try and
get the straight information on what a decibel is. You'll go all
around the circuit and back again, and still not have an understandable
explanation.
Here's the big secret  a decibel is nothing more than a unit
of comparison between two sound intensities or loudnesses.
Fig. 1. Logarithmic curve expresses the relationship
between sound intensify and the reaction of the human ear.
Fig. 2. An output meter is connected across a load resistor
for db measurements.
Fig. 3. Microphone level of 70 db is built up by amplifier
with a gain of +120 db to a level of +47 db at speaker.

Sound Intensities. Back in the early 1920's,
the telephone engineers were trying to measure the ability of the
human ear to detect differences in sound intensity. It was a simple
matter to measure a change in light intensity. The light became
brighter and this change in brightness could be read off in footcandles
on a photocell.
Similarly, a change in temperature could be recorded on a thermometer
in degrees. However, when a sound became louder, how would you measure
that, and in what units? There was no unit available, so one was
devised.
The unit for measuring sound levels was called the "bel" and
was named in honor of the inventor of the telephone, Alexander Graham
Bell. A decibel (db) is one tenth of a bel, this being a more practical
unit with which to work.
Once again, the decibel is a unit of comparison of sound intensities.
Comparison is the important word here. A decibel is not an absolute
unit as is the volt, or ohm, or ampere.
The basis for this comparison of sounds is the ability of the
human ear to detect a difference in loudness between two sounds.
To put it another way, when your ear can just distinguish that one
sound is louder than another, there is a difference of 1 db between
the two sounds.
Human Reactance. Let's examine the way in which
the human ear reacts to sound. Imagine you are visiting a dog show
and fifty dogs are all barking at once. Loud, isn't it? Now imagine
that fifty more dog fanciers arrive with their pets and that these
fifty dogs all add to the din. Louder? Yes, but how much louder?
The sound intensity has doubled, but loud as it is, it doesn't
sound twice as loud to your ear as the barking of the original fifty
dogs. Not until five hundred dogs were all barking at once could
your ear detect a sound twice as loud as the initial sound, that
is, if you could stick it out that long.
Your ear responds to sound on what is known as a "logarithmic
curve." Because of this, when the engineers were devising the equation
for the comparison of two sound intensities they had to make it
obey the same mathematical curve as did the logarithm. This curve
is shown in Fig. 1. The decibel measurement, being a logarithmic
function, gives a true picture of sounds as they affect the ear.
We will now relate what we have learned to decibel measurement
in electronics.
Decibel Measurement. If we call the input power
to an amplifier P_{i} and the output power from the amplifier
P_{o}, and then express both quantities in watts, the formula
for obtaining the number of decibels, N_{db}, gained through
use of the amplifier is: N_{db} = 10 log P_{o}/P_{i}.
Note that the logarithms used are to the base 10.
The steps in using this formula are:
1. Compute the ratio of Po/Pi expressed in watts.
2. Look up the value of the logarithm of this ratio in the log
tables.
3. Multiply this logarithm by ten to get your answer in decibels.
Here is a practical example to illustrate the workings of this
very important formula: If the input power to an amplifier is 0.2
watt and the output power of the amplifier is 10 watts, then:
N_{db} = 10 log 10/0.2
N_{db} = 10 log 50
N_{db} = 10 x 1.70
N_{db} = 17 db
An audio VTVM available from Heathkit in kit form at
low cost is shown above.
Note relationship between the db scale and the 05 volt
a.c. scale.

This shows that an increase of 50 times in the input power due
to the amplifier action increases the power level of the output
by 17 decibels. You can readily see that the decibel relationship
compares the two powers, input and output, in the manner of their
effect on the human ear when they are converted into sound.
Figure 2 shows, in block diagram form, one means of actually
measuring decibels.
The amplification of any amplifier will vary according to the
frequency being amplified. For that reason, amplifier ratings will
show a figure such as, "Frequency response; ± 2 db, 20 to 20,000
cps." This indicates that the frequency of the input to the amplifier,
when. varied over a range from 20 to 20,000 cps, will cause a variation
in the output power of ± 2 db. The smaller this variation of output
with change of frequency, the better the frequency response of the
amplifier and the less distortion of the output.
If you are using two or more amplifiers in a circuit and want
to know the overall rating of the system, you add the decibel rating
of each one, assuming that the two units are perfectly matched.
Decibels can be given as a minus (db) figure indicating a loss
as well as a plus (+db) figure indicating a gain. See Fig. 3.
Since the manufacturer of an amplifier does not know how it will
be used in your system, he must establish some sort of zero reference
point in order to figure a decibel rating for the particular unit
under consideration. The zero levels generally used are 0.006 watt
or 0.012 watt. These would represent the power input, or Pi in the
formula we have discussed. There is also a standard impedance termination,
or load, across which the output meter is connected in the measuring
circuit. This value of load resistance must be the same for any
comparative measurements.
Using a Meter. If you have occasion to use a
directreading decibel meter, you will note that the scale spacing
is uneven. This is due to the fact that the scale is laid out in
logarithmic spacing rather than linear spacing which in turn is
due to the logarithm in the decibel formula. A good example of the
difference between a logarithmic scale and a linear scale can be
seen by comparing the scales on a slide rule and on a ruler. The
slide rule is logarithmic and he ruler is linear.
Actually, the output decibel meter is a d.c. voltmeter and rectifier
combination. The meter measures output volts, but the scale reads
in decibels. The zero point on the meter is that point on the scale
where the zero reference level wattage is measured. Any reading
over this zero point is read plus db, any reading below it, minus
db.
It is important that you understand what decibels mean and what
they tell you about the equipment you use. You will meet them often
in your electronics work.
Posted May 29, 2014 