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Topic 4.2
Travelling waves
Travelling Waves
There are two types of waves
and pulses that we encounter
in the physical world.
Transverse
 In these waves the source that produces the wave
oscillates at right angles to the direction of travel of
the wave
 It means that the particles of the medium through
which the wave travels also oscillates at right angle
to the direction of travel of the wave.
Direction of travel
of the wave
Direction of oscillation
of the particles
Transverse Wave
Longitudinal
In these waves the source that produces the
wave oscillates in the same direction as the
direction of travel of the wave
It means that the particle of the medium
through which the wave travels also
oscillates in the same direction as the
direction of travel of the wave.
Longitudinal Wave
Direction of travel
of the wave
Direction of oscillations
of the particles
Discrete Pulses and Continuous Waves
A single shake of a slinky will send a discrete
pulse down it
Shake the slinky up and down and a
continuous travelling wave travels down it
This applies to longitudinal waves too
Question:
• List 6 types of wave and classify them
according to the types you have just learnt.
Definitions
 The following definitions are given in terms of the
particles that make up the medium through which
the wave travels.
 For the slinky spring a particle would be a single
turn of the spring
 For the water waves a particle would be a very
small part of the water.
What is a Wave?
A wave is a means by which energy is
transferred between two points in a medium
without any net transfer of the medium itself.
The Medium
 The substance or object in which the wave is
travelling.
 When a wave travels in a medium parts of the
medium do not end up at different places
 The energy of the source of the wave is carried to
different parts of the medium by the wave.
Water waves however, can be a bit
disconcerting.
Waves at sea do not transport water but the
tides do.
Similarly, a wave on a lake does not transport
water but water can actually be blown along
by the wind.
Displacement
(s) is the distance that any particle
is away from its equilibrium position
at an instance
Measured in metres
Crest
This is a term coined from water
waves and refers to the points at
the maximum height of the wave.
It is the positive displacement
from equilibrium
Trough
 A term coined from water waves
referring to the points at the lowest
part of the wave.
The negative displacement from
equilibrium.
Compression
This is a term used in connection with
longitudinal wave and refers to the region
where the particles of the medium are
"bunched up".
High density
High pressure
Rarefaction
A term used in connection with longitudinal
waves referring to the regions where the
particles are "stretched out".
Low density
Low pressure
Wavelength
 () This is the distance along the medium between
two successive particles that have the same
displacement and the same phase of motion.
 Measured in metres
Amplitude
(A, a) This is the maximum displacement of a
particle from its equilibrium position
(It is also equal to the maximum
displacement of the source that produces the
wave).
Normally measured in metres
Period
(T) This is the time that it takes a particle to
make one complete oscillation
(It also equals the time for the source of the
wave to make one complete oscillation).
Measured in seconds
Frequency
 (f) This is the number of oscillations made per
second by a particle
 (It is also equal to the number of oscillations made
per second by the source of the wave)
 The SI unit of frequency is the Hertz - Hz. (1 Hz is
1 oscillation per second)
 Clearly then, f = 1/T
Wave Speed
 (v, c) This is the speed with which energy is carried
in the medium by the wave.
 Measured in m s-1
 A very important fact is that wave speed depends
only on the nature and properties of the medium
Eg
• For example, the speed of sound waves in air is
typically 330 ms-1 to 350 ms-1 depending on the
density of the air and is four times faster in water.
Velocity = displacement of crest/time taken
• If the time taken is equal to the period T of the
wave, the displacement of one crest in this time is
equal to  and the equation can be rewritten as:
• v = /T
• But f = 1/T
• so v = f
Waves speed table
WAVE TYPE MEDIUM SPEED (ms-1)
Sound Carbon Dioxide 260
Air 331
Hydrogen 1290
Pure Water 1410
Sea Water 1450
Glass 5500
Light Vacuum 2.997 x 108
Air 2.998 x 108
Glass (crown) 2.0 x 108
Earthquake Crust 3500 (transverse)
8000 (longitudinal)
Mantle 6500 (transverse)
11000 (longitudinal)
Eg 1
• What will be the time delay in hearing the
sound from a brass band for an observer 660
m away? Assume the light arrives
instantaneously and the sound travels at 330
ms-1.
Solution
• v = 330 ms-1
• s = 660 m
• t = ?
• v = s/t
and rearranging;
• t = s/v
• t = 660/330
• t = 2.0 s
Eg 2
• Waves reaching the beach from an offshore
storm arrives at 4 s intervals. Calculate the
frequency of the waves
Solution
• T = 4 s
T = 1/f
• f = ¼
• f = 0.25 Hz
Eg 3
• Find the period of a 1 kHz sound wave.
Solution
• f = 1 kHz = 1000 Hz
• T = ?
• F = 1/T
• rearranging;
• T = 1/f
• T = 1/1000
• T = 0.001 or 10-3 s.
Eg 4
• Calculate the speed of an earthquake wave
with a wavelength of 2 km and a frequency of
3 Hz.
Solution
•  = 2000m
• f = 3 Hz
• v = ?
• v = f
• v = 3 x 2000
• v = 6000 m s-1
Eg 5
• Given that the speed of sound in air is 330
ms-1, find the wavelength of (a) 20Hz and (b)
20000 Hz sounds.
Solution
• Part (a)
• v = 330 m s-1
• f = 20 Hz
•  = ?
• v = f
•  = 330/20
•  = 16.5 m
Part (b)
v = 330 m s-1
f = 20 000 Hz
 = ?
v = f
 = 330/20 000
 = 0.0165 m
 = 1.65 x 10-2 m
 A very important property associated with all waves
is their so-called periodicity.
 Waves in fact are periodic both in time and space
and this sometimes makes it difficult to appreciate
what actually is going on in wave motion.
Periodicity
If we drew a diagram that froze time
on waves in water
We would have an instantaneous
snapshot of the whole of the water
surface
The next diagram shows the
periodicity of the wave in space
Displacement / Distance
displacement
distancep
The y-axis shows the displacement
of the water from its equilibrium
position
The graph is a displacement-
distance graph.
We now look at one part of the wave that is
labeled p and "unfreeze" time
The next diagram shows how the position of
p varies with time
This illustrates the periodicity of the wave in
time
Displacement / Time
displacement of point p from equilibrium position
time
The y-axis now shows the
displacement of the point p from
equilibrium
The graph is a displacement-time
graph.
The space diagram and the time
diagram are both identical in shape
If we mentally combine them we
have the whole wave moving both
in space and time.
And for Longitudinal Waves?
For the longitudinal wave in the
slinky spring the displacement-
distance graph actually shows the
displacement of the individual turns
of the spring from their equilibrium
position as a function of distance
along the spring.
However
It could equally show how the
density of turns of the spring varies
with length along the spring.
The displacement-time graph
shows the displacement of one turn
of the spring from its equilibrium
positions as a function of time.
Wavelength again!
Wavelength will therefore be equal
to the distance between successive
crests and successive troughs.
rarefactions
wavelength
Sound Waves
A longitudinal wave in a slinky
spring is analogous to a sound
wave in which each turn of the
spring represents an air molecule.
Interpreting Graphs - 1
displacement
distance
crest
trough
amplitude crest
wavelength
amplitude
wavelength
Interpreting Graphs - 2
displacement
time
amplitude
period
period
Deriving v = f 
Imagine a wave with velocity v
Being produced from a source of
frequency f
In 1 second the 1st wavefront would
have travelled a distance of f 
As speed = distance / time
v = f  / 1
 v = f 
2 Important Points
1. The frequency of a wave
depends only on the source
producing the wave
 It will therefore not change if the wave
enters a different medium or the
properties of the medium change
2. The Speed of waves only
depends on the nature and the
properties of the medium
 Water waves do travel faster in deeper
water
 Light travels slower in more optically
dense material
The EM Spectrum Itself
Short Long 
High fLow f
VISIBLERadio
Waves
Micro
Waves
Infra
red
Gamma
rays
Ultra
Violet
X
rays
Wavelengths of Regions (m)
• Gamma Rays <10-12
• X-rays 10-10
• Ultraviolet 10-8
• Violet 7.5 x 10-7 > Visible > Red 4.3 x 10-7
• Infrared 10-5
• Microwaves 10-2
• Radio and TV > 103
The Different Regions
In the context of wave motion, common
properties of all parts of the
electromagnetic spectrum are
 all transverse waves
 all travel at the speed of light in vacuo
(3.0 x 108 ms-1)
 all can travel in a vacuum
Sources of Regions
 Gamma – certain radioactive material’s nuclei
 X-rays – by firing an electron stream at a tungsten
metal target in a highly evacuated tube.
 Ultraviolet – the Sun, ultraviolet lamp
 Visible – hot bodies
 Infrared – the Sun (heat), hot bodies
 Microwaves – Ovens, communication systems
 Radio and TV – transmitter stations, Azteca TV

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4.2

  • 2. Travelling Waves There are two types of waves and pulses that we encounter in the physical world.
  • 3. Transverse  In these waves the source that produces the wave oscillates at right angles to the direction of travel of the wave  It means that the particles of the medium through which the wave travels also oscillates at right angle to the direction of travel of the wave.
  • 4. Direction of travel of the wave Direction of oscillation of the particles Transverse Wave
  • 5. Longitudinal In these waves the source that produces the wave oscillates in the same direction as the direction of travel of the wave It means that the particle of the medium through which the wave travels also oscillates in the same direction as the direction of travel of the wave.
  • 6. Longitudinal Wave Direction of travel of the wave Direction of oscillations of the particles
  • 7. Discrete Pulses and Continuous Waves A single shake of a slinky will send a discrete pulse down it Shake the slinky up and down and a continuous travelling wave travels down it This applies to longitudinal waves too
  • 8.
  • 9.
  • 10. Question: • List 6 types of wave and classify them according to the types you have just learnt.
  • 11. Definitions  The following definitions are given in terms of the particles that make up the medium through which the wave travels.  For the slinky spring a particle would be a single turn of the spring  For the water waves a particle would be a very small part of the water.
  • 12. What is a Wave? A wave is a means by which energy is transferred between two points in a medium without any net transfer of the medium itself.
  • 13. The Medium  The substance or object in which the wave is travelling.  When a wave travels in a medium parts of the medium do not end up at different places  The energy of the source of the wave is carried to different parts of the medium by the wave.
  • 14. Water waves however, can be a bit disconcerting. Waves at sea do not transport water but the tides do. Similarly, a wave on a lake does not transport water but water can actually be blown along by the wind.
  • 15. Displacement (s) is the distance that any particle is away from its equilibrium position at an instance Measured in metres
  • 16. Crest This is a term coined from water waves and refers to the points at the maximum height of the wave. It is the positive displacement from equilibrium
  • 17. Trough  A term coined from water waves referring to the points at the lowest part of the wave. The negative displacement from equilibrium.
  • 18. Compression This is a term used in connection with longitudinal wave and refers to the region where the particles of the medium are "bunched up". High density High pressure
  • 19. Rarefaction A term used in connection with longitudinal waves referring to the regions where the particles are "stretched out". Low density Low pressure
  • 20. Wavelength  () This is the distance along the medium between two successive particles that have the same displacement and the same phase of motion.  Measured in metres
  • 21. Amplitude (A, a) This is the maximum displacement of a particle from its equilibrium position (It is also equal to the maximum displacement of the source that produces the wave). Normally measured in metres
  • 22. Period (T) This is the time that it takes a particle to make one complete oscillation (It also equals the time for the source of the wave to make one complete oscillation). Measured in seconds
  • 23. Frequency  (f) This is the number of oscillations made per second by a particle  (It is also equal to the number of oscillations made per second by the source of the wave)  The SI unit of frequency is the Hertz - Hz. (1 Hz is 1 oscillation per second)  Clearly then, f = 1/T
  • 24. Wave Speed  (v, c) This is the speed with which energy is carried in the medium by the wave.  Measured in m s-1  A very important fact is that wave speed depends only on the nature and properties of the medium
  • 25. Eg • For example, the speed of sound waves in air is typically 330 ms-1 to 350 ms-1 depending on the density of the air and is four times faster in water. Velocity = displacement of crest/time taken • If the time taken is equal to the period T of the wave, the displacement of one crest in this time is equal to  and the equation can be rewritten as: • v = /T • But f = 1/T • so v = f
  • 26. Waves speed table WAVE TYPE MEDIUM SPEED (ms-1) Sound Carbon Dioxide 260 Air 331 Hydrogen 1290 Pure Water 1410 Sea Water 1450 Glass 5500 Light Vacuum 2.997 x 108 Air 2.998 x 108 Glass (crown) 2.0 x 108 Earthquake Crust 3500 (transverse) 8000 (longitudinal) Mantle 6500 (transverse) 11000 (longitudinal)
  • 27. Eg 1 • What will be the time delay in hearing the sound from a brass band for an observer 660 m away? Assume the light arrives instantaneously and the sound travels at 330 ms-1.
  • 28. Solution • v = 330 ms-1 • s = 660 m • t = ? • v = s/t and rearranging; • t = s/v • t = 660/330 • t = 2.0 s
  • 29. Eg 2 • Waves reaching the beach from an offshore storm arrives at 4 s intervals. Calculate the frequency of the waves
  • 30. Solution • T = 4 s T = 1/f • f = ¼ • f = 0.25 Hz
  • 31. Eg 3 • Find the period of a 1 kHz sound wave.
  • 32. Solution • f = 1 kHz = 1000 Hz • T = ? • F = 1/T • rearranging; • T = 1/f • T = 1/1000 • T = 0.001 or 10-3 s.
  • 33. Eg 4 • Calculate the speed of an earthquake wave with a wavelength of 2 km and a frequency of 3 Hz.
  • 34. Solution •  = 2000m • f = 3 Hz • v = ? • v = f • v = 3 x 2000 • v = 6000 m s-1
  • 35. Eg 5 • Given that the speed of sound in air is 330 ms-1, find the wavelength of (a) 20Hz and (b) 20000 Hz sounds.
  • 36. Solution • Part (a) • v = 330 m s-1 • f = 20 Hz •  = ? • v = f •  = 330/20 •  = 16.5 m Part (b) v = 330 m s-1 f = 20 000 Hz  = ? v = f  = 330/20 000  = 0.0165 m  = 1.65 x 10-2 m
  • 37.  A very important property associated with all waves is their so-called periodicity.  Waves in fact are periodic both in time and space and this sometimes makes it difficult to appreciate what actually is going on in wave motion. Periodicity
  • 38. If we drew a diagram that froze time on waves in water We would have an instantaneous snapshot of the whole of the water surface The next diagram shows the periodicity of the wave in space
  • 40. The y-axis shows the displacement of the water from its equilibrium position The graph is a displacement- distance graph.
  • 41. We now look at one part of the wave that is labeled p and "unfreeze" time The next diagram shows how the position of p varies with time This illustrates the periodicity of the wave in time
  • 42. Displacement / Time displacement of point p from equilibrium position time
  • 43. The y-axis now shows the displacement of the point p from equilibrium The graph is a displacement-time graph.
  • 44. The space diagram and the time diagram are both identical in shape If we mentally combine them we have the whole wave moving both in space and time.
  • 45. And for Longitudinal Waves? For the longitudinal wave in the slinky spring the displacement- distance graph actually shows the displacement of the individual turns of the spring from their equilibrium position as a function of distance along the spring.
  • 46. However It could equally show how the density of turns of the spring varies with length along the spring.
  • 47. The displacement-time graph shows the displacement of one turn of the spring from its equilibrium positions as a function of time.
  • 48. Wavelength again! Wavelength will therefore be equal to the distance between successive crests and successive troughs.
  • 50. Sound Waves A longitudinal wave in a slinky spring is analogous to a sound wave in which each turn of the spring represents an air molecule.
  • 51. Interpreting Graphs - 1 displacement distance crest trough amplitude crest wavelength amplitude wavelength
  • 52. Interpreting Graphs - 2 displacement time amplitude period period
  • 53. Deriving v = f  Imagine a wave with velocity v Being produced from a source of frequency f In 1 second the 1st wavefront would have travelled a distance of f  As speed = distance / time v = f  / 1  v = f 
  • 54. 2 Important Points 1. The frequency of a wave depends only on the source producing the wave  It will therefore not change if the wave enters a different medium or the properties of the medium change
  • 55. 2. The Speed of waves only depends on the nature and the properties of the medium  Water waves do travel faster in deeper water  Light travels slower in more optically dense material
  • 56. The EM Spectrum Itself Short Long  High fLow f VISIBLERadio Waves Micro Waves Infra red Gamma rays Ultra Violet X rays
  • 57. Wavelengths of Regions (m) • Gamma Rays <10-12 • X-rays 10-10 • Ultraviolet 10-8 • Violet 7.5 x 10-7 > Visible > Red 4.3 x 10-7 • Infrared 10-5 • Microwaves 10-2 • Radio and TV > 103
  • 58. The Different Regions In the context of wave motion, common properties of all parts of the electromagnetic spectrum are  all transverse waves  all travel at the speed of light in vacuo (3.0 x 108 ms-1)  all can travel in a vacuum
  • 59. Sources of Regions  Gamma – certain radioactive material’s nuclei  X-rays – by firing an electron stream at a tungsten metal target in a highly evacuated tube.  Ultraviolet – the Sun, ultraviolet lamp  Visible – hot bodies  Infrared – the Sun (heat), hot bodies  Microwaves – Ovens, communication systems  Radio and TV – transmitter stations, Azteca TV