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Topic 4 – Oscillations and Waves
4.4 Wave Properties
Reflection and Transmission
● When a wave crosses a boundary between 2
media the wave will be partly reflected and
partly transmitted.
● The amount of reflection and transmission
depends on the nature of the boundary.
● If the wave is able to move at the boundary then the
reflected wave will be in phase. (A Soft Boundary)
● If the wave is fixed at the boundary then the
reflected wave will be out of phase. (A Hard
Boundary)
Reflection and Transmission
● As waves move from one
medium into another the wave
is partially transmitted and
partially reflected.
● If the boundary is from low
density to high density then
this is a hard boundary and
the reflected wave suffers a
phase change.
● If the boundary is from high
density to low density then
this is a soft boundary and the
reflected wave is reflected in
phase.
θi
θR
θr
The Law of Reflection
● The angle of incidence always equals the angle
of reflection.
θi
θR
Changing Media
● As waves move from one medium into another their
wavespeed will change.
● Transverse waves usually have more resistance to
propagation in dense materials
● The wave will therefore usually travel slower in more
dense materials.
● The refractive index (1
n2
) is the ratio of the speeds to
the wave in medium 2 to that in medium 1
● The absolute refractive (n2
) index is that when medium
1 is a vacuum, i.e. c
n2
.
Refractive Indices
● The refractive indices of some common
materials are shown below.
● Calculate the speed of light in these materials
Material n v x108
ms-1
Air 1.0003
Water 1.333
Perspex 1.49
Crown Glass 1.52
Diamond 2.42
Changing Media
● When a wave crosses a boundary between two
media at an angle other than the normal it will
change direction.
● This is called refraction
● The amount of refraction is predicted by Snell’s
law: sin θi
sinθr
=
vi
vr
=
nr
ni
Refraction
● When light crosses from a
less optically dense
medium into an more
optically dense medium
the light refracts towards
the normal.
● When light crosses from a
more optically dense
medium into an less
optically dense medium
the light refracts away the
normal.
θi
θr
Refraction and Critical Angle
● The use of a semi-circular block of medium
allows the effect of moving from a high
optical density to a low optical density to be
studied.
● Any ray that enters the block along a radius
will strike the curved surface normally and
hence will not refract.
● As light exits a material into air or the
vacuum it will refract away from the normal.
● At some angle of incidence, the refracted
ray will be directly along the flat surface of
the block.
● This is known as the critical angle θc
.
● The refractive index of the medium can
hence be determined.
θc
sinθi
sinθr
=
nr
ni
ni=
nr sinθr
sinθi
n=
1sin 90
sinθc
n=
1
sinθc
Diffraction
● When a plane wave
encounters a gap in a
barrier then the waves that
pass through will become
curved at the edges and
spread out.
● This is called diffraction.
● This is the phenomenon
that allows sound to
“travel around corners”
● The amount of diffraction
depends on the ratio of the
width of the gap and the
wavelength.
Diffraction
● If the gap width (d) is
much larger than the
wavelength then the
wave passes through
with only small
diffraction.
Diffraction
● If the gap width (d) is
larger than the
wavelength then the
wave passes through
with only more
diffraction.
● The wave ends start
to noticeable curve
Diffraction
● If the gap width (d) is
slightly wider than the
wavelength then the
wave passes through
with a lot of
diffraction.
● The wave looks more
curved than straight
Diffraction
● If the gap width (d) is
exactly the same
width as the
wavelength then the
wave passes through
and forms perfectly
circular waves.
● There are now no
shadows
Examples of Diffraction
● Water waves are
often seen diffracting
as they enter a
harbour.
● Sound can be heard
around a corner due
to diffraction
Examples of Diffraction
● Light also diffracts but this
is much less noticeable
than sound because of the
short wavelength of light.
● Often the image suffers
chromatic aberration
● Different colours of light
have different
wavelengths so are
diffracted by different
amounts.
● This colour splitting is
known as dispersion
Superposition
● Two waves that exist in the
same space are able to
propagate through each
other.
● When the two waves
interact, the resultant wave
form is that formed by the
superposition of the two
waves.
● Superposition is the vector
addition of the two
amplitudes.
Superposition
● If the two waves are in
phase at the interaction,
then the amplitude
increases.
● This is constructive
superposition.
● If the two waves are out
of phase at the
interaction, then the
amplitude is zero.
● This is destructive
superposition.
Superposition and Harmonics
● Musical Instruments
rarely produce pure
notes.
● Usually additional
harmonics are
audiable.
● If the fundamental
frequency of a string
instrument is f, then
the harmonics are:
● 2f, 3f, 4f etc.

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Wave Properties and Phenomena Explained

  • 1. Topic 4 – Oscillations and Waves 4.4 Wave Properties
  • 2. Reflection and Transmission ● When a wave crosses a boundary between 2 media the wave will be partly reflected and partly transmitted. ● The amount of reflection and transmission depends on the nature of the boundary. ● If the wave is able to move at the boundary then the reflected wave will be in phase. (A Soft Boundary) ● If the wave is fixed at the boundary then the reflected wave will be out of phase. (A Hard Boundary)
  • 3. Reflection and Transmission ● As waves move from one medium into another the wave is partially transmitted and partially reflected. ● If the boundary is from low density to high density then this is a hard boundary and the reflected wave suffers a phase change. ● If the boundary is from high density to low density then this is a soft boundary and the reflected wave is reflected in phase. θi θR θr
  • 4. The Law of Reflection ● The angle of incidence always equals the angle of reflection. θi θR
  • 5. Changing Media ● As waves move from one medium into another their wavespeed will change. ● Transverse waves usually have more resistance to propagation in dense materials ● The wave will therefore usually travel slower in more dense materials. ● The refractive index (1 n2 ) is the ratio of the speeds to the wave in medium 2 to that in medium 1 ● The absolute refractive (n2 ) index is that when medium 1 is a vacuum, i.e. c n2 .
  • 6. Refractive Indices ● The refractive indices of some common materials are shown below. ● Calculate the speed of light in these materials Material n v x108 ms-1 Air 1.0003 Water 1.333 Perspex 1.49 Crown Glass 1.52 Diamond 2.42
  • 7. Changing Media ● When a wave crosses a boundary between two media at an angle other than the normal it will change direction. ● This is called refraction ● The amount of refraction is predicted by Snell’s law: sin θi sinθr = vi vr = nr ni
  • 8. Refraction ● When light crosses from a less optically dense medium into an more optically dense medium the light refracts towards the normal. ● When light crosses from a more optically dense medium into an less optically dense medium the light refracts away the normal. θi θr
  • 9. Refraction and Critical Angle ● The use of a semi-circular block of medium allows the effect of moving from a high optical density to a low optical density to be studied. ● Any ray that enters the block along a radius will strike the curved surface normally and hence will not refract. ● As light exits a material into air or the vacuum it will refract away from the normal. ● At some angle of incidence, the refracted ray will be directly along the flat surface of the block. ● This is known as the critical angle θc . ● The refractive index of the medium can hence be determined. θc sinθi sinθr = nr ni ni= nr sinθr sinθi n= 1sin 90 sinθc n= 1 sinθc
  • 10. Diffraction ● When a plane wave encounters a gap in a barrier then the waves that pass through will become curved at the edges and spread out. ● This is called diffraction. ● This is the phenomenon that allows sound to “travel around corners” ● The amount of diffraction depends on the ratio of the width of the gap and the wavelength.
  • 11. Diffraction ● If the gap width (d) is much larger than the wavelength then the wave passes through with only small diffraction.
  • 12. Diffraction ● If the gap width (d) is larger than the wavelength then the wave passes through with only more diffraction. ● The wave ends start to noticeable curve
  • 13. Diffraction ● If the gap width (d) is slightly wider than the wavelength then the wave passes through with a lot of diffraction. ● The wave looks more curved than straight
  • 14. Diffraction ● If the gap width (d) is exactly the same width as the wavelength then the wave passes through and forms perfectly circular waves. ● There are now no shadows
  • 15. Examples of Diffraction ● Water waves are often seen diffracting as they enter a harbour. ● Sound can be heard around a corner due to diffraction
  • 16. Examples of Diffraction ● Light also diffracts but this is much less noticeable than sound because of the short wavelength of light. ● Often the image suffers chromatic aberration ● Different colours of light have different wavelengths so are diffracted by different amounts. ● This colour splitting is known as dispersion
  • 17. Superposition ● Two waves that exist in the same space are able to propagate through each other. ● When the two waves interact, the resultant wave form is that formed by the superposition of the two waves. ● Superposition is the vector addition of the two amplitudes.
  • 18. Superposition ● If the two waves are in phase at the interaction, then the amplitude increases. ● This is constructive superposition. ● If the two waves are out of phase at the interaction, then the amplitude is zero. ● This is destructive superposition.
  • 19. Superposition and Harmonics ● Musical Instruments rarely produce pure notes. ● Usually additional harmonics are audiable. ● If the fundamental frequency of a string instrument is f, then the harmonics are: ● 2f, 3f, 4f etc.