2.0 Information Sources 2.1 Audio Signals: Dr. Ing. Saviour Zammit
2.0 Information Sources 2.1 Audio Signals: Dr. Ing. Saviour Zammit
2.0 Information Sources 2.1 Audio Signals: Dr. Ing. Saviour Zammit
10/8/2010
Sound
Sound is a vibration of air molecules, caused by a vibrating object
which causes the air molecules to compress and rarefy as they are
pushed and pulled (pressure wise) by the vibrating edge.
The sound waves thus produced travel (or propagate) in a direction
parallel to the compression and rarefaction of the air molecules,
and hence sound wave is a longitudinal wave.
The pressure waves, most often propagate through the air to the
ear, where the sound is analyzed first into frequency bands by the
ear, and then carried by nerves to the brain for interpretation and
action.
Human beings both produce and detect sound and have evolved
sound communications to such a degree that it distinguishes us
from all other life forms on earth.
Physical Characteristics
1.5
1
Amplitude A
0.5
Period T
0
1
-0.5
9 11 13 15 17 19 21 23 25 27 29 31 33 35
Time
-1
Frequency f = 1 / T
-1.5
10/8/2010
1.5
1
Amplitude
0.5
Wavelength
0
1
11 13 15 17 19 21 23 25 27 29 31 33 35
Distance m
-0.5
-1
Speed v = f.
-1.5
Sound frequencies
The human ear can hear sound frequencies from 20 Hz to some 22,000 Hz.
Animals such as dogs and bats can hear much higher sounds (ultrasound).
This is the range of Audible frequencies and changes with age.
Young people have a larger range than old people, who start to loose
mostly perception of higher frequencies.
If p(t) measures the pressure of a sound wave, for a pure sound tone, we
can write
2
p (t ) = A sin
t
T
A over middle C on an instrument is the pure tone of 460 Hz and its
pressure function is then of the form
p (t ) = A sin (920t )
10/8/2010
Amplitude
The amplitude of a sound wave is interpreted as loudness
by the human auditory system.
The HAS is not linear, in that it can hear very loud sounds as
well as very small sounds, over a range of some 11 to 12
orders of magnitude.
Amplitude is related to the motion of the molecules in the
medium, which is of the order of one thousandth of a
centimeter for a very loud sound, and millionths of a
centimeter for normal sounds.
In order to compare values with large variations of
magnitude we use decibels. Thus the difference in Level in
decibels between two power values P1 and P2 is given by
Level = log10
P1
dB
P2
Sound Intensity
The threshold of sound is one picowatt (1pW) of sound
power per m2 at a listeners location, and all other sounds
are compared to this.
Thus a 100 Watt stereo is 10.log((100*.01)/10-12) or 120dB
at 1m (assuming 1% conversion efficiency from electrical to
sound power).
P1
P2
10/8/2010
Amplitude
Watts
30000
300
3
0.03
0.0003
0.000003
0.00000003
0.0000000003
0.000000000001
dB
source
165
145
125
105
85
65
45
25
0
jet
threshold of pain
factory noise
highway traffic
appliance
converstation
quite room
whisper
threshold of hearing
10/8/2010
10/8/2010
10/8/2010
HAS Sensitivity
10/8/2010
10/8/2010
Ribbon Microphone
Condenser Microphone
10
10/8/2010
11
10/8/2010
12