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PHYS 1540 4/12/2014
Experiment 11
Reflection, Refraction, Dispersion of Light and Brewster’s Angle
Christopher Douglas
Introduction
Experiment 11 consisted of four individual experiments that each involved various
topics within the branch of physics generally known as optics. The first experiment
dealt with the connection between the angle of incidence and the angle of reflection
as applied to light rays interacting with mirrors of various geometrical shapes. The
second experiment examined some of the same principles however instead of the
use of mirrors, the light ray was passed through a lens and refraction was analyzed.
The third experiment observed the phenomenon of dispersion by passing a light ray
through an acrylic rhomboid. Once the light ray passed through the rhomboid,
various calculations were made relating to the indices for each unique color the ray
produced. Our last experiment introduced Brewster’s Angle by exploring
polarization and the use of polarizing lenses.
Theory A: Reflection
As a ray of light lands and hits a specific point on a perfectly flat mirror, the light
“rebounds” or reflects from that point. This incoming ray is referred to as the
incident ray and the light that “bounces” off the point is called the reflected ray.
When the incident ray makes it’s initial strike on the mirror, a line normal to that
point can be drawn perpendicular to the light ray. On the side of the normal line that
encompasses the incident ray, the angle of incident can be measured between the
normal and the incident ray itself. As one might expect, the angle of reflection
between the normal and the reflection ray can be measured in much the same way.
When these two angles are measured, we see they are equivalent. These two angles
being equal verifies the law of reflection which tells us that the angle of incidence is
equal to the angle of reflection, Θr = Θi.
The Angular Relationship Between the Incident and Reflected Light Rays
Equipment List
• Ray Optics Kit • Basic Optics Light Source • Protractor • Ruler • White Paper • Pencil • D-‐Shaped Acrylic Lens • Polarize
Note: The above equipment list applies to all four experiments included in
lab 11.
Procedure A: Reflection
The procedure began by tracing the three-‐way mirror on a sheet of white paper. The
halfway point on the straight end of the mirror was marked and the normal line was
drawn from the apex on the opposite end through the mark and beyond to about 10
centimeters. This step was then repeated for the remaining two sides.
Drawing Normal Lines
Once all normal lines were drawn, the light source was directed at each side such
that the beam hit the point where the normal line protrudes. The light source being
directed towards the mirror produced an incident ray and a reflected ray, these rays
and their respective angles were each marked and measured carefully with a
protractor and ruler.
Completed Three-‐Way Mirror Angle Analysis
Note: A lab partner held the three-‐way mirror down while the tracing was
performed. This prevented the mirror from slipping out of place which in turn
may yield inaccurate data.
Data A: Reflection
Analysis A: Reflection
As expected, the angles of incidence were equal to the angles of reflection. The law
of reflection, which shows Θi = Θr, was verified. As each side was analyzed, it was
determined that the magnitude of each angle was different based upon the
geometry of the side itself. The concave side of the mirror produced angles that
were slightly smaller than both and straight and convex sides. Naturally the same
trend was observed for the convex and straight sides respectively.
Theory B: Refraction
Refraction is a phenomenon studied in many braches of science. In the branch of
physics termed optics, refraction is a surface phenomenon that simply refers to the
bending of light due to its passing through different material mediums. When light
travels through air then suddenly strikes and passes through glass for instance, the
light ray slows down. The consequence of this change in the material medium
causes the light to bend. The degree to which the light slows down is indicated by
“n” or the index of refraction. The higher the index, the greater the light will
decrease in speed. The angles generated by this change in speed and direction can
be found with Snell’s Law:
n1sin(Θ1)=n2sin(Θ2)
The above equation shows us that n1 (the incident material index) times the
incident angle is equal to n2 (the refraction material index) times the angle of
refraction.
Procedure B: Refraction
The light source was placed on the lab table and adjusted to produce a single beam
of light. The light source was then carefully maneuvered such that the light passed
directly through the middle of the ray table at 0°. The lens shaped like a capital “D”
was placed on the center of the ray table. The ray table was calibrated to the 0°
mark, as relating to the angle of incidence. The angles of refraction were carefully
measure and recorded. Assembly seen below:
Note: While adjusting the light source, the rotation of the ray table proceeded
slowly. It was determined that rushing the rotation of the ray table lead
to inaccurate data.
Data B: Refraction
Analysis B: Refraction
After all the data was recorded, the index of refraction was found by using Snell’s
Law. The given angles and indices selected to plug into the Snell’s Law equation
were n1=1.0 (index in air), Θi=50° and Θr=31°. The result gave an index of refraction
for the lens of n2=1.48. This result was proven successful in that only 0.23% error
was found when comparing the experimental index to the theoretical index.
Theory C: Dispersion
We have all seen a prism or looked up in the sky to witness the beauty of a rainbow.
On he other hand, all of us have enjoyed the sunlight or the convenience of an
ordinary bedside lamp. This ordinary light we see throughout our daily lives is often
times referred to as “white light.” White light is simply light that is a combination of
several different colors that each have a unique wavelength. With careful precision,
one can actually separate out all different colors through refraction and see each
individual color generated by it respective wavelength. This process of separation
by refraction is called dispersion.
Procedure C: Dispersion
An acrylic rhomboid was placed on a white sheet of paper and carefully traced
around its outside perimeter. The rhomboid was lifted off the paper and a normal
line was drawn from the angled side along with another line 45° from the normal.
The light source was then directed through the normal line. The light ray entering,
exiting and the dispersion trends were all traced and labeled. As the light ray existed
through the paper, dispersion of blue and red light was observed. The angles,
indices of refraction and velocities of the dispersion were measured.
Data C: Dispersion
Analysis C: Dispersion
The angles were found using a protractor, the indices were calculated using Snell’s
Law and the velocities were proven by knowing that the index is equal to the speed
of light divided by the velocity, n=c/v, where c=3.00x10^8 m/s. Equations below:
Theory D: Brewster’s Angle
When light bearing a specific polarity travels through a transparent dielectric
surface and results in no reflection, the angle at which it enters (angle of incidence)
is commonly referred to as Brewster’s Angle. This angle can be found with relative
ease with a polarizing disk and by simply locating the angle where the refracted and
reflected rays are separated by 90°.
Procedure D: Brewster’s Angle
The lens with the shape of a capital “D” was placed on the ray table and the light
source was directed at the center of the table and straight side of the lens. The ray
table was rotated while being observed through a polarizing disk. The ray table was
then positioned at an angle of 90° separation between the refracted and reflected
rays. The polarizing disk was rotated until the light intensity diminished. This angle
was the marked and calculated.
Data D: Brewster’s Angle
Analysis D: Brewster’s Angle
By again using Snell’s Law, Brewster’s Angle was observed after a few careful
calculations. Though some substitutions had to be done in order to derive our
needed equation, after the derivation was complete, our needed angle was found.
See below for the derivation:
Discussion of Results
Throughout each experiment, the laws governing reflection, refraction, dispersion
and Brewster’s Angle were rigorously tested and ultimately verified. The Law of
reflection was verified by our angle of incidence being equal to the angle of
reflection. We saw in the refraction experiment that as the index of refraction
increased, the speed decreased and this was verified with Snell’s Law and the
velocity equation. By measuring the angles, speeds and indexes of the dispersed
light through the acrylic rhomboid, the principles of dispersion were upheld.
Brewster’s Angle was found and also verified with the use of the ray table by placing
the refraction and reflected rays 90° apart, then observing with the polarizing lens.
The principles that guide each phenomenon were analyzed and were verified
without exception.
Conclusion
Overall, the experiments were a success. I felt as though my lab partners and myself
actively engaged in each procedure and learned the concepts that were presented.
Some mechanical error can be found due impart by the dispersion of the light source
at the ends of its produced rays. Human error can be found in instances where the
three-‐way mirror was “bumped” accidentally, slightly altering the measured angle.
Although error was present, the overall statistical data was not greatly affected as
can be seen by the minimal percent error and expected results. I enjoyed this lab
very much, I felt as though it increased my understanding of the presented material
and exposed me to the reliable methods behind accurate science.
Work Cited
University of North Texas Physics Department. General Physics 1540 with Calculus
Lab II. Denton: Eagle Image Digital Print Centers, 2013. Print.