INTERFERENCE
Robert Eshun
ACCRA POLYTECHNIC
1
 Interference
◦ interaction of two or more waves at a point in a
medium such that the disturbance in the resulting
wave is the vector sum of the disturbances in the
interfering waves.
◦ the phenomenon in which two or more waves
superpose each other to form a resultant wave of
greater or lower amplitude.
2
 Interference - the interaction of waves that
are coherent with each other, either because
they come from the same source or because
they have the same or nearly the same
frequency.
3
 Crest of one wave + crest of another wave at
the same point = constructive interference
 Resultant wave is a crest whose amplitude is
a vector sum of the original wave’s
amplitudes.
 Two interfering troughs behave similarly.
4
 Crest of a wave + trough of another wave =
destructive interference.
 If amplitudes of original waves are the same,
zero displacement of particles results.
5
 Layer of material with thickness in the sub-
nanometer to micron range.
 Light striking surface is either transmitted or
reflected at the upper surface.
 Transmitted light may also be transmitted or
reflected at bottom surface.
6
 Studies of these waves reveal information about
the surface including the thickness of the film or
the effective refractive index of the film medium.
 Thin film interference - the interference of waves
reflected from the top surface with those
reflected from the bottom surface.
 Thin films such as soap bubbles show colourful
patterns because of interference between light
waves.
 The thickness of the film has to be comparable to
the wavelength of light for a nice coloured
pattern to be obtained.
7
 For constructive interference, the two waves
must be shifted by an integer multiple of
wavelengths relative to one another.
8
 Thin film of air trapped between two pieces
of glass
 Monochromatic light incident almost normally
on film.
 Light is reflected from the two interfaces.
 The eye focuses these two parallel light
beams at one spot on the retina.
9
 Destructive interference if path difference =
odd number of ½ wavelength.
 Constructive interference if path difference =
even number of ½ wavelengths.
10
Additional phase difference
 A 1800 phase change on reflection from
interface between air (optically less dense)
and glass (optically dense).
 This is equivalent to an additional path
difference of 𝜆
2.
11
Therefore condition for
 constructive interference is
2t=(m+1⁄2)λ
 destructive interference is
2t=mλ
where m is an integer.
12
 Interferometer made of a metal from which
part of a beam of light is reflected. The other
part proceeds directly to the screen.
 Light from a monochromatic slit source
reflect from a glass surface at a small angle
 Appears to come from a virtual source as a
result.
13
 The reflected light interferes with the direct
light from the source to form interference
fringes.
 This is another method for finding the
wavelength of light by the division of
wavefront.
14
 Glass prism with a large angle producing two
coherent (virtual) sources for light
interference experiments.
 Wavelength λ of the incident monochromatic
radiation given by:
𝜆 =
𝑦𝑑
𝐷
15
 y is the fringe separation, d is the source
separation, and D is the source-screen
distance.
16
 Upper portion of wave refracted downward,
lower portion refracted upward.
 Refracted waves appear to come from two
different sources
 Overlap in shaded region to produce
interference fringes.
17
 mth bright fringe is given by
𝑦 𝑚 = 𝑚𝜆
𝐷
𝑑
y is measured from the centre of the
interference pattern.
 The wavelength of light can be determined
from measurements of fringe separation in
the interference pattern.
18
 Designed to split light beam into two parts
and then recombines them to form an
interference pattern.
 For obtaining accurate length measurements.
 Physical distances can be measured by
counting interference fringes that move when
one or the other of two objects are displaced.
19
 Beams must be mutually coherent for fringes
to be seen.
 Must have a definite phase relationship
between them.
 Mutual coherence obtained by use of a beam
splitter (partially reflecting mirror).
20
 The reflected (R) and transmitted (T) waves
are redirected by ordinary mirrors to the
output where they are superposed to form
fringes.
21
 One of the two mirrors is kept stationary
while the other is mobile.
 The path difference depends on the relative
motion of these mirrors.
 Constructive interference if the two paths
differ by a whole number of wavelengths
(including 0); strong signal at the detector.
 Destructive if they differ by a whole number
and half wavelengths (e.g., 0.5, 1.5, 2.5 ...);
weak signal.
22

Chapter 7 interference

  • 1.
  • 2.
     Interference ◦ interactionof two or more waves at a point in a medium such that the disturbance in the resulting wave is the vector sum of the disturbances in the interfering waves. ◦ the phenomenon in which two or more waves superpose each other to form a resultant wave of greater or lower amplitude. 2
  • 3.
     Interference -the interaction of waves that are coherent with each other, either because they come from the same source or because they have the same or nearly the same frequency. 3
  • 4.
     Crest ofone wave + crest of another wave at the same point = constructive interference  Resultant wave is a crest whose amplitude is a vector sum of the original wave’s amplitudes.  Two interfering troughs behave similarly. 4
  • 5.
     Crest ofa wave + trough of another wave = destructive interference.  If amplitudes of original waves are the same, zero displacement of particles results. 5
  • 6.
     Layer ofmaterial with thickness in the sub- nanometer to micron range.  Light striking surface is either transmitted or reflected at the upper surface.  Transmitted light may also be transmitted or reflected at bottom surface. 6
  • 7.
     Studies ofthese waves reveal information about the surface including the thickness of the film or the effective refractive index of the film medium.  Thin film interference - the interference of waves reflected from the top surface with those reflected from the bottom surface.  Thin films such as soap bubbles show colourful patterns because of interference between light waves.  The thickness of the film has to be comparable to the wavelength of light for a nice coloured pattern to be obtained. 7
  • 8.
     For constructiveinterference, the two waves must be shifted by an integer multiple of wavelengths relative to one another. 8
  • 9.
     Thin filmof air trapped between two pieces of glass  Monochromatic light incident almost normally on film.  Light is reflected from the two interfaces.  The eye focuses these two parallel light beams at one spot on the retina. 9
  • 10.
     Destructive interferenceif path difference = odd number of ½ wavelength.  Constructive interference if path difference = even number of ½ wavelengths. 10
  • 11.
    Additional phase difference A 1800 phase change on reflection from interface between air (optically less dense) and glass (optically dense).  This is equivalent to an additional path difference of 𝜆 2. 11
  • 12.
    Therefore condition for constructive interference is 2t=(m+1⁄2)λ  destructive interference is 2t=mλ where m is an integer. 12
  • 13.
     Interferometer madeof a metal from which part of a beam of light is reflected. The other part proceeds directly to the screen.  Light from a monochromatic slit source reflect from a glass surface at a small angle  Appears to come from a virtual source as a result. 13
  • 14.
     The reflectedlight interferes with the direct light from the source to form interference fringes.  This is another method for finding the wavelength of light by the division of wavefront. 14
  • 15.
     Glass prismwith a large angle producing two coherent (virtual) sources for light interference experiments.  Wavelength λ of the incident monochromatic radiation given by: 𝜆 = 𝑦𝑑 𝐷 15
  • 16.
     y isthe fringe separation, d is the source separation, and D is the source-screen distance. 16
  • 17.
     Upper portionof wave refracted downward, lower portion refracted upward.  Refracted waves appear to come from two different sources  Overlap in shaded region to produce interference fringes. 17
  • 18.
     mth brightfringe is given by 𝑦 𝑚 = 𝑚𝜆 𝐷 𝑑 y is measured from the centre of the interference pattern.  The wavelength of light can be determined from measurements of fringe separation in the interference pattern. 18
  • 19.
     Designed tosplit light beam into two parts and then recombines them to form an interference pattern.  For obtaining accurate length measurements.  Physical distances can be measured by counting interference fringes that move when one or the other of two objects are displaced. 19
  • 20.
     Beams mustbe mutually coherent for fringes to be seen.  Must have a definite phase relationship between them.  Mutual coherence obtained by use of a beam splitter (partially reflecting mirror). 20
  • 21.
     The reflected(R) and transmitted (T) waves are redirected by ordinary mirrors to the output where they are superposed to form fringes. 21
  • 22.
     One ofthe two mirrors is kept stationary while the other is mobile.  The path difference depends on the relative motion of these mirrors.  Constructive interference if the two paths differ by a whole number of wavelengths (including 0); strong signal at the detector.  Destructive if they differ by a whole number and half wavelengths (e.g., 0.5, 1.5, 2.5 ...); weak signal. 22