Physics
Physics
Investigator
Investigator
y
y
Project
Project
Kamal Singh
Kamal Singh
12
12
th
th
A
A
K.V. 2 Colaba
K.V. 2 Colaba
Mumbai
Mumbai
TOTAL
INTERNAL
Certificate
This is hereby to certify that the
original and genuine investigation
work has been carried out to
investigate about the subject matter
and the related data collection and
investigation has been completed
solely, sincerely and satisfactorily by
Kamal Singh
a student
of class
12
th
A
of
Kendriya Vidyalaya 2 Colaba
Mumbai ,
regarding his project
titled
“Total Internal Reflection”
.
ACKNOWLEDGEMENT
It would be my utmost
pleasure to express my
sincere thanks to my Physics
teacher
Mrs.Manju Rawat
mam
in providing a helping
hand in this project. Her
valuable guidance, support and
supervision all through this
project are responsible for
attaining its present form. I
would also like to thank my
parents and friends as they
encouraged me to put forward
my project.
Introduction
Optical description
Critical angle
Phase shift upon total
internal reflection
Total internal reflection in
diamond
Applications of total internal
reflection
Examples in everyday life
Total Internal Reflection
using a Soda
Bottle{EXPERIMENT}
Bibliography
Total internal reflection is an optical phenomenon that happens when a ray of light strikes a medium boundary at an angle larger than a particular critical angle with respect to the normal to the surface. If the refractive index is lower on the other side of the boundary and the incident angle is greater than the critical angle, no light can pass through and all of the light is reflected. The critical angle is the angle of incidence above which the total internal reflectance occurs.
When a light beam crosses a boundary between materials with different kinds of refractive indices, the light beam will be partially refracted at the boundary surface, and partially reflected. However, if the angle of incidence is greater (i.e. the ray is closer to being parallel to the boundary) than the critical angle – the angle of incidence at which light is refracted such that it travels along the boundary – then the light will stop crossing the boundary altogether and instead be totally reflected back internally. This can only occur where light travels from a medium with a higher [n1=higher refractive index] to one with a lower refractive index [n2=lower refractive index]. For example, it will occur when passing from glass to air, but not when passing from air to glass.
Total internal reflection can be demonstrated using a semi-circular block of glass or plastic. A "ray box" shines a narrow beam of light (a "ray") onto the glass. The semi-circular shape ensures that a ray pointing towards the centre of the flat face will hit the curved surface at a right angle; this will prevent refraction at the air/glass boundary of the curved surface. At the glass/air boundary of the flat surface, what happens will depend on the angle? Where is θC
the critical angle measurement which is caused by the sun or a light source (measured normal to the surface):
• If θ < θC, the ray will split. Some of the ray will
reflect off the boundary, and some will refract as it passes through. This is not total internal reflection. • If θ > θC, the entire ray reflects from the
boundary. None passes through. This is called total internal reflection.
This physical property makes optical fibres useful and prismatic binoculars possible. It is also what gives diamonds their distinctive sparkle, as diamond has an unusually high refractive index.
CRITICAL ANGLE
The critical angle is the angle of incidence above which total internal reflection occurs. The angle of incidence is measured with respect to the normal at the refractive boundary (see diagram illustrating Snell's law). Consider a light ray passing from glass into air. The light emanating from the interface is bent towards the glass. When the incident angle is increased sufficiently, the transmitted angle (in air) reaches 90 degrees. It is at this point no light is transmitted into air. The critical angle is given by Snell's law.
n1sinθi=n2sin θt
Rearranging Snell's Law, we get incidence
sin θi=n2
n1
sin θt
To find the critical angle, we find the value for θi
when θt=90 ° and thus sin θt=1 .The resulting
value of is equal to the critical angle θc .
Now, we can solve for θi , and we get the
equation for the critical angle:
θc=θi=sin−1
(
n2n1
)
If the incident ray is precisely at the critical angle, the refracted ray is tangent to the boundary at the point of incidence. If for
acrylic glass (with an index of refraction of 1.50) into air (with an index of refraction of 1.00), the calculation would give the critical angle for light from acrylic into air, which is
θc=sin−1
(
1.00PHASE SHIFT UPON
TOTAL INTERNAL
REFLECTION
A lesser-known aspect of total internal reflection is that the reflected light has an angle dependent phase shift between the reflected and incident light. Mathematically this means that the Fresnel reflection coefficient becomes a complex rather than a real number. This phase shift is polarization dependent and grows as the incidence angle deviates further from the critical angle toward grazing incidence.
The polarization dependent phase shift is long known and was used by Fresnel to design the Fresnel rhomb which allows transforming circular polarization to linear polarization and vice versa for a wide range of wavelengths (colours), in contrast to the quarter wave plate. The polarization dependent phase shift is also the reason why TE and TM guided modes have different dispersion relations.
TOTAL INTERNAL
REFLECTION IN
From glass to air the critical angle is about 42o but it varies from one medium to another. The material that gives the smallest critical angle is diamond. That is why they sparkle so much! Rays of light can easily be made to 'bounce around inside them' by careful cutting of the stone and the refraction at the surfaces splits the light into a spectrum of colours! Relatively speaking, the critical angle 24.4o for the diamond-air boundary is extremely small. This
property of the diamond-air boundary plays an important role in the brilliance of a diamond
gemstone. Having a small critical angle, light has the tendency to become "trapped" inside of a diamond once it enters. Most rays approach the diamond at angles of incidence greater than the critical angle (as it is so small) so a light ray will typically undergo TIR several times before finally refracting out of the
diamond. This gives diamond a tendency to sparkle. The effect can be enhanced by the cutting of a
diamond gemstone with a 'strategically' planned shape.
APPLICATIONS OF
TOTAL INTERNAL
REFLECTION
Total internal reflection is the operating
principle of optical fibres, which are used in endoscopes and telecommunications.
Total internal reflection is the operating
principle of automotive rain sensors, which control automatic windscreen/windshield wipers.
Another application of total internal reflection
is the spatial filtering of light.
Prismatic binoculars use the principle of total
internal reflections to get a very clear image.
Gonioscopy employs total internal reflection
to view the anatomical angle formed between the eye's cornea and iris.
Optical fingerprinting devices use frustrated
total internal reflection in order to record an image of a person's fingerprint without the use of ink.
A Total internal reflection fluorescence
microscope uses the evanescent wave
produced by TIR to excite fluorophores close to a surface. This is useful for the study of surface properties of biological samples.
EXAMPLES IN
EVERYDAY LIFE
Total internal reflection can be observed while swimming, when one opens one's eyes just under the water's surface. If the water is calm, its surface appears mirror-like.
One can demonstrate total internal reflection by filling a sink or bath with water, taking a glass tumbler, and placing it upside-down over the plug hole (with the tumbler completely filled with water). While water remains both in the upturned tumbler and in the sink surrounding it, the plug hole and plug are visible since the angle of refraction between glass and water is not greater than the critical angle. If the drain is opened and the tumbler is kept in position over the hole, the water in the tumbler drains out leaving the glass filled with air, and this then acts as the plug. Viewing this from above, the tumbler now appears mirrored because light reflects off the air/glass interface.
This is different phenomenon from reflection and refraction. Reflection occurs when light goes back in same medium. Refraction occurs when light travels from different mediums. Here both are not happening. This is due to both and a mixture of both.Another common example of total internal reflection is a critically cut diamond. This is what gives it maximum spark
Total Internal Reflection
using a Soda Bottle
Explanation
In this case, nair = 1.00 nwater = 1.33. Therefore:
In this demo light will continually reflect through the stream of water creating total internal reflection
(TIR). The stream of water will 'carry' the light though, to the end of the stream.
Total Internal Reflection is the principle behind fiber optics.
Materials
empty soda pop bottle (2 liter)
tape hand drill drill bits water green laser bucket
old books, etc for stands
Procedure
First set up
the soda bottle by
drilling a hole
near the bottom of the bottle. Begin
with a drill bit that has a
diameter which is slightly larger than the diameter of the laser that will be used. We
used a 1/4 inch drill bit, however sizes as small as 7/32 inch worked as well.
First tape the hole and then fill the bottle with water. The cap will prevent leaking because it creates a vacuum in the bottle.
Stand the soda bottle on top of a stack of books so the hole is facing the bucket. The laser should be placed in a binder clip so it stays on, and then set on a stack of books and papers. The laser should be lined up so that the laser light goes through the soda bottle, and into the center of the hole. See for details.
Carefully remove the tape and then unscrew the top of the soda bottle. The light should reflect within the stream of water so that you could see at least a few points of reflection. The light should be visible through the entire stream.
If the reflections of the light aren’t clear, it may be necessary to expand the hole by drilling through the existing hole with a larger drill bit. This
process may need to be repeated several times.
Notes
This is an messy experiment. Be ready to adjust the bucket which catches the stream of water.
Also be aware that the stream's curvature will change as the water level decreases. It will bend closer to the bottle, and the bucket may need to be adjusted again. When the water level is a little above the hole there will be no total internal
reflection although the stream will continue.
Place the cap back on, or put the bottle inside of the bucket.
Make sure to have lots of paper towels! Towels or rags could be useful too. However, this mess is water, and therefore easy to clean up.
Some resources suggest putting a drop of food coloring in the bottom of the bucket to match the laser light, giving the appearance that the water
has permanently 'trapped' the
colored light.
BIBLIOGRAPHY
Following Books and websites were a source for my project.
Wikipedia
NCERT Physics Textbook for class 12 Feynman Lectures on Physics
