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World 
Communicates 
Sound 
waves 
Preliminary 
Physics 
8.2.2 
By 
S. 
Choi
Sound 
wave 
(a) 
• Sound 
waves 
are 
produced 
by 
vibra;ng 
objects 
– 
they 
are 
the 
result 
of 
vibra;ons 
or 
oscilla;ons 
of 
par;cles 
in 
a 
medium. 
• Sound 
energy 
propagates 
in 
3-­‐D 
as 
alterna/ng 
higher 
and 
lower 
pressure 
varia;ons 
(compressions 
and 
rarefac:ons). 
• The 
pressure 
varia;ons 
propagate 
through 
a 
medium 
away 
from 
the 
source 
of 
the 
vibra;ons. 
• Sounds 
waves 
travel 
at 
different 
speeds 
depending 
on 
the 
medium 
and 
temperatures. 
The 
speed 
of 
sound 
in 
dry 
air 
is 
340m/s. 
They 
can 
be 
reflected 
(echo) 
and 
refracted. 
• Sound 
travels 
faster 
in 
liquids 
and 
non-­‐porous 
solids 
than 
it 
does 
in 
air.
Ac;vi;es 
with 
tuning 
forks 
1. Listen 
to 
the 
sound 
when 
a 
vibra;ng 
tuning 
fork 
is 
touched 
on 
a 
solid 
wooden 
surface. 
2. Touch 
a 
vibra;ng 
tuning 
fork 
against 
the 
nose 
or 
the 
ear 
lobe. 
3. Listen 
to 
the 
sound 
produced 
as 
the 
tuning 
fork 
is 
rotated 
close 
to 
the 
ear 
about 
its 
long 
axis. 
4. Dip 
the 
vibra;ng 
tuning 
fork 
into 
water. 
The 
vibra;ng 
prongs 
of 
the 
tuning 
fork 
cause 
the 
molecules 
in 
the 
surrounding 
air 
to 
vibrate 
– 
sound 
propaga;ng 
as 
a 
longitudinal 
wave 
mo;on 
in 
3-­‐D 
away 
from 
the 
source
Longitudinal 
waves 
represented 
as 
transverse 
wave 
(b) 
• When 
a 
sound 
travels 
through 
a 
tube 
fiOed 
with 
pressure 
gauges, 
the 
pressure 
gauges 
will 
record 
varia;ons 
in 
pressure. 
• Compressions 
(C) 
are 
regions 
of 
higher 
pressure 
and 
rarefac;ons 
(R) 
are 
regions 
of 
lower 
pressure. 
• The 
graph 
shows 
the 
pressure 
at 
all 
points 
along 
the 
tube 
at 
one 
instant 
of 
/me. 
R C R C 
Compression
Longitudinal 
waves 
represented 
as 
transverse 
wave 
(b) 
• A 
single 
pressure 
gauge 
recording 
the 
pressure 
at 
a 
fixed 
point 
in 
the 
tube 
over 
a 
period 
of 
;me 
would 
show 
regular 
pressure 
varia/ons. 
• As 
the 
wave 
propagates 
from 
leS 
to 
right 
along 
the 
tube, 
the 
pressure 
alternates 
from 
low 
to 
high 
with 
a 
frequency 
equal 
to 
that 
of 
the 
sound 
wave. 
• The 
graph 
shows 
the 
pressure 
varia;ons 
at 
a 
fixed 
point 
as 
the 
wave 
moves 
along 
the 
tube. 
R C R C
Longitudinal 
waves 
represented 
as 
transverse 
wave 
(b)
Volume 
& 
pitch 
(c) 
• Loudness 
of 
a 
sound 
is 
caused 
by 
the 
amplitude 
of 
the 
sound 
wave 
– 
higher 
the 
amplitude, 
louder 
the 
sound 
• Tone 
or 
the 
pitch 
of 
a 
sound 
is 
caused 
by 
the 
frequency. 
Higher 
the 
frequency, 
higher 
the 
tone/ 
pitch 
• Humans 
have 
the 
hearing 
range 
from 
20 
Hz 
to 
20 
kHz 
(approximately). 
The 
range 
shrinks 
during 
life.
Ultrasound 
& 
infrasound 
Sound 
waves 
with 
a 
frequency 
too 
high 
for 
the 
human 
ear 
are 
called 
ultrasound 
Sound 
waves 
with 
a 
frequency 
too 
low 
for 
the 
human 
ear 
to 
hear 
are 
called 
infrasound. 
Animals 
such 
as 
dogs, 
bats, 
birds 
and 
insects 
can 
hear 
ultrasound. 
Animals 
such 
as 
whales, 
elephants 
and 
hippopotamus 
use 
infrasound 
to 
communicate 
over 
distances.
Echo 
(d) 
• When 
a 
sound 
wave 
meets 
a 
boundary 
between 
two 
media, 
some 
of 
the 
energy 
of 
the 
wave 
will 
be 
reflected 
at 
the 
boundary. 
• Knowing 
the 
speed 
of 
sound 
in 
a 
par;cular 
medium, 
the 
distance 
to 
a 
reflec;ng 
surface 
can 
be 
determined. 
This 
principle 
is 
applied 
in 
SONAR 
used 
by 
ships 
to 
locate 
the 
posi;on 
of 
objec;ons 
under 
water. 
• Bats 
use 
a 
sophis;cated 
sonar 
system 
to 
navigate 
and 
to 
catch 
prey.
The 
speed 
of 
sound 
in 
different 
media 
Material 
Density 
(g/cm) 
Speed 
(m/s) 
Copper 
8.90 
6420 
Steel 
7.86 
5940 
Beryllium 
1.93 
12890 
Aluminium 
2.58 
6420 
Water 
1.00 
1496 
Ethanol 
0.79 
1207 
Air 
0.00139 
331.45 
Helium 
0.000178 
965 
Fat 
0.95 
1450 
Muscle 
1.07 
1580 
Skull 
bone 
1.91 
4080
Superposi;on 
of 
waves 
(e) 
• The 
addi/on 
of 
waves 
is 
called 
superposi:on. 
Sounds 
waves 
from 
separate 
sources 
can 
be 
added. 
• If 
two 
out-­‐of-­‐phase 
waves 
interfere, 
the 
resultant 
sound 
wave 
will 
have 
a 
smaller 
amplitude 
than 
either 
of 
the 
original 
waves 
• If 
two 
in-­‐phase 
waves 
interfere, 
the 
resultant 
sound 
wave 
will 
have 
a 
greater 
amplitude 
than 
either 
of 
the 
original 
waves. 
Construc:ve 
two 
waves 
are 
in-­‐phase 
(half-­‐cycle) 
Destruc:ve 
interference 
occurs 
when 
interference 
occurs 
when 
two 
waves 
are 
out-­‐of-­‐phase 
by 
180° 
(half-­‐ 
cycle). 
If 
the 
amplitudes 
of 
both 
waves 
are 
equal, 
then 
annulment 
of 
waves 
will 
occur.
Graphical 
superposi;on 
of 
waves 
(d) 
No;ce 
any 
paOerns?
Beats 
• When 
two 
sources 
of 
sound 
of 
the 
same 
amplitude 
but 
slightly 
different 
frequency 
are 
heard 
together, 
there 
will 
be 
a 
rhythmic 
change 
to 
the 
volume 
of 
the 
sound. 
• When 
the 
two 
sound 
waves 
are 
in 
phase, 
the 
amplitude 
of 
the 
resul;ng 
sound 
wave 
is 
the 
sum 
of 
the 
amplitudes 
of 
the 
two 
waves, 
and 
results 
in 
a 
loud 
sound. 
• As 
the 
waves 
driS 
out 
of 
phase, 
the 
resultant 
amplitude 
will 
become 
smaller, 
eventually 
reaching 
zero 
before 
increasing 
again 
as 
the 
waves 
driS 
back 
into 
phase. 
• The 
term 
‘beats’ 
is 
used 
to 
describe 
the 
varia;on 
in 
the 
loudness 
of 
the 
sound.

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Preliminary Physics - World communicates 2

  • 1. World Communicates Sound waves Preliminary Physics 8.2.2 By S. Choi
  • 2. Sound wave (a) • Sound waves are produced by vibra;ng objects – they are the result of vibra;ons or oscilla;ons of par;cles in a medium. • Sound energy propagates in 3-­‐D as alterna/ng higher and lower pressure varia;ons (compressions and rarefac:ons). • The pressure varia;ons propagate through a medium away from the source of the vibra;ons. • Sounds waves travel at different speeds depending on the medium and temperatures. The speed of sound in dry air is 340m/s. They can be reflected (echo) and refracted. • Sound travels faster in liquids and non-­‐porous solids than it does in air.
  • 3. Ac;vi;es with tuning forks 1. Listen to the sound when a vibra;ng tuning fork is touched on a solid wooden surface. 2. Touch a vibra;ng tuning fork against the nose or the ear lobe. 3. Listen to the sound produced as the tuning fork is rotated close to the ear about its long axis. 4. Dip the vibra;ng tuning fork into water. The vibra;ng prongs of the tuning fork cause the molecules in the surrounding air to vibrate – sound propaga;ng as a longitudinal wave mo;on in 3-­‐D away from the source
  • 4. Longitudinal waves represented as transverse wave (b) • When a sound travels through a tube fiOed with pressure gauges, the pressure gauges will record varia;ons in pressure. • Compressions (C) are regions of higher pressure and rarefac;ons (R) are regions of lower pressure. • The graph shows the pressure at all points along the tube at one instant of /me. R C R C Compression
  • 5. Longitudinal waves represented as transverse wave (b) • A single pressure gauge recording the pressure at a fixed point in the tube over a period of ;me would show regular pressure varia/ons. • As the wave propagates from leS to right along the tube, the pressure alternates from low to high with a frequency equal to that of the sound wave. • The graph shows the pressure varia;ons at a fixed point as the wave moves along the tube. R C R C
  • 6. Longitudinal waves represented as transverse wave (b)
  • 7. Volume & pitch (c) • Loudness of a sound is caused by the amplitude of the sound wave – higher the amplitude, louder the sound • Tone or the pitch of a sound is caused by the frequency. Higher the frequency, higher the tone/ pitch • Humans have the hearing range from 20 Hz to 20 kHz (approximately). The range shrinks during life.
  • 8. Ultrasound & infrasound Sound waves with a frequency too high for the human ear are called ultrasound Sound waves with a frequency too low for the human ear to hear are called infrasound. Animals such as dogs, bats, birds and insects can hear ultrasound. Animals such as whales, elephants and hippopotamus use infrasound to communicate over distances.
  • 9. Echo (d) • When a sound wave meets a boundary between two media, some of the energy of the wave will be reflected at the boundary. • Knowing the speed of sound in a par;cular medium, the distance to a reflec;ng surface can be determined. This principle is applied in SONAR used by ships to locate the posi;on of objec;ons under water. • Bats use a sophis;cated sonar system to navigate and to catch prey.
  • 10. The speed of sound in different media Material Density (g/cm) Speed (m/s) Copper 8.90 6420 Steel 7.86 5940 Beryllium 1.93 12890 Aluminium 2.58 6420 Water 1.00 1496 Ethanol 0.79 1207 Air 0.00139 331.45 Helium 0.000178 965 Fat 0.95 1450 Muscle 1.07 1580 Skull bone 1.91 4080
  • 11. Superposi;on of waves (e) • The addi/on of waves is called superposi:on. Sounds waves from separate sources can be added. • If two out-­‐of-­‐phase waves interfere, the resultant sound wave will have a smaller amplitude than either of the original waves • If two in-­‐phase waves interfere, the resultant sound wave will have a greater amplitude than either of the original waves. Construc:ve two waves are in-­‐phase (half-­‐cycle) Destruc:ve interference occurs when interference occurs when two waves are out-­‐of-­‐phase by 180° (half-­‐ cycle). If the amplitudes of both waves are equal, then annulment of waves will occur.
  • 12. Graphical superposi;on of waves (d) No;ce any paOerns?
  • 13. Beats • When two sources of sound of the same amplitude but slightly different frequency are heard together, there will be a rhythmic change to the volume of the sound. • When the two sound waves are in phase, the amplitude of the resul;ng sound wave is the sum of the amplitudes of the two waves, and results in a loud sound. • As the waves driS out of phase, the resultant amplitude will become smaller, eventually reaching zero before increasing again as the waves driS back into phase. • The term ‘beats’ is used to describe the varia;on in the loudness of the sound.