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Activity: The Critical Angle and Fiber Optics (Equipment-Based) |
In today's activity, you will measure the critical angle and index of refraction for a plastic prism and then use a simulation to investigate the effects of total internal reflection for fiber optics. The readings about these topics are found in the module on Reflection, Refraction, and Fiber Optics.
Equipment needed: Each group needs a laser, a plastic semi-circular prism, a device to vertically spread the laser beam mounted at an appropriate height (such as a cylindrical lens attached to a washer and mounted on a magnetic optical carrier), two pieces of blank paper, and a protractor.
Preparatory
Questions:
The following questions should have been answered
before the start of the activity. Your instructor may ask you to
discuss your answers with group members or as a class before continuing.
Measuring
the Critical Angle of a Plastic Prism for a Given Wavelength
| LASERS ARE NOT TOYS. DO NOT
LOOK INTO THE LASER OR POINT YOUR LASER WHERE IT SHINES IN SOMEONE'S EYES.
WHEN YOU ARE NOT USING THE LASER, TURN IT OFF.
Set up the equipment on top of a blank page of paper, as shown to the right. The laser light should shine through a device that spreads the light so you can see the path of the laser on the paper. The light should then strike the curved side of the plastic "prism", travel through the prism, and exit near the middle of the flat side of the prism. Some light will also be reflected off the flat side and exit the curved side. |
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| 1. | Rotate the prism, observing the behavior of the light
beam exiting the flat face (refracted beam) and the behavior of the beam
reflected from the flat face. Start with the flat side perpendicular
to (but facing away from) the laser beam, and rotate it counterclockwise,
as depicted in the diagram above. Continue rotating it until the
flat side is parallel to the laser beam. Describe what happens to
the refracted beam and reflected beam as you rotate the prism. How
do you know when the critical angle has been reached?
When the flat side of the prism is perpendicular to the beam, all the light escapes. As the prism is rotated, the intensity of the refracted beam gradually decreases, and the intensity of the reflected beam increases. The refracted beam rotates toward the flat side of the prism; its intensity goes to zero as the beam becomes parallel with the prism's flat side. Through all this the angle between reflected and incident rays steadily increases. |
| 2. | Continue rotating the prism and determine whether you
can achieve total internal reflection when the light enters the prism,
when light leaves the prism, both, or neither? When you observe light entering
the prism, the flat side should be facing the laser. (Light striking
the curved face does not significantly refract - the angle of incidence
is generally close to 0)
TIR is only possible when light leaves the prism, as it must travel from a denser medium into a rarer medium. Hopefully, students predicted this result in the preparatory questions. |
| 3. | Rotate the prism back until you have achieved the critical
angle for the light traveling from the prism into air at the flat face.
Use a sharp pencil (pen is ok, but sharp pencil is best) to CAREFULLY mark
the following points:
The sheet should look like the image to the left, (without the laser light or the outline of the prism included for reference). The drawing should exhibit expected symmetry between incident and reflected rays. |
| 4. | Measure the angle between the incident ray and the reflected
ray, estimating angles down to the nearest tenth of a degree. Be
sure to line up your protractor as CAREFULLY as you can. A small
error in measurement can lead to bad results in today's experiment!
Exact values will, of course, depend upon the material you use. Most plastic and glass will give results in the vicinity of the 81 degrees we obtained. |
| 5. | Calculate the critical angle from your angle in the previous
question. How are they related?
The critical angle will be half of the angle measured above. The measured angle is the sum of the angle of incidence and the angle of reflection, which just equals twice the angle of incidence, according to the law of reflection. |
| 6. | How does this critical angle compare to the one you predicted
for plastic in the Preparatory Questions?
Hopefully close, if the material used has an index near that given in the preparatory questions. Student values tend to vary between 1.45 and 1.65 when the prism has an index of 1.54. |
| 7. | Use your measured value of the critical angle to determine
the index of refraction of your prism. Discuss your result in light
of any discrepancies found in the previous question.
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Applications to Optical Fibers
Go to this simulation of optical fibers by the Universitat Oldenburg, and answer the following questions. A few notes about the simulation:
| 8. | Will the angle of entry i affect whether or not
the light is totally internally reflected as it enters the fiber?
If so, how? If not, why not?
Yes. the angle at which light enters the fiber determines its angle of incidence on the fiber wall. If the angle of entry is too big, the angle of incidence on the fiber wall will be less than the critical angle, causing light to escape. |
| 9. | Based on what you know about total internal reflection,
what range of values of n2 (relative
to the core index n1) will keep
the light trapped in the fiber? (You may assume the angle of incidence
on the edge of the fiber is larger than the critical angle) Try out
ns
from your range and check.
The cladding index n2 must be less than the core index n1 if TIR is to occur. |
| 10. | Some of the n2
values you expected to trap light in the fiber might have let light escape
in the simulation due to the angle at which light strikes the edge of the
fiber. In these situations would you need to increase or decrease
the
angle at which light strikes the top edge of the fiber (as measured
to the normal) to trap the light?
If light escapes, the angle of incidence at the top edge is less than the critical angle, so you need to increase the angle of incidence on the top edge. |
| 11. | Does this desired increase or decrease in the angle at
the edge of the fiber correspond to an increase or decrease of the entry
angle i at which the light enters the fiber? Use the simulation
to verify your answer.
To increase the angle of incidence at the top edge, one must decrease the angle of entry i. |
| 12. | Set the indices to n1=1.54
and n2 = 1.50, and find the largest
value of i that results in total internal reflection by trying different
values of i. Compare your result to the cut-off angle
given by the simulation.
To three decimal places, the maximum angle of entry is 20.4 degrees, in agreement with the cut-off angle calculated by the simulation. |
| 13. | If you were designing a fiber, do you think you would
prefer for your light to enter at an angle close to (but still less than)
the cut-off angle, or at a much smaller angle close to zero degrees?
What potential benefits do you envision this having?
The primary advantage of light entering at an entry angle of close to zero is if all the light did so. If all of the light entering a fiber enters in a narrow cone, it travels essentially the same path and does not spread out, or disperse. (Such "modal dispersion" is the topic for another module.) A more basic way to look at it is that light entering along the axis of the fiber takes a more direct route and spends less time bouncing around than light that enters near the cut-off angle. Or, that light entering near the cut-off is more likely to exceed the critical angle at an edge should the fiber bend. Students might argue that light entering along the axis travels a shorter distance and so arrives more quickly. You could point out that such an advantage could be negated at the first bend. Additionally, the time it takes a single information "packet" to travel a fiber is much less important than the delay between information packets, or bits. The delay is dictated by dispersion (spreading), not by the transit time. |
Copyright © 1999-2004 Doris Jeanne Wagner and Rensselaer Polytechnic Institute. All Rights Reserved.