The Mathematics of Refraction
Refraction is the bending of the path of a light wave as
it passes across the boundary separating two media. Refraction is caused by
the change in speed experienced by a wave when it changes medium.
In Lesson 1, we learned that if a light wave passes from a
medium in which it travels slow (relatively speaking) into a medium in which it
travels fast, then the light wave would refract away from the normal. In such a
case, the refracted ray will be farther from the normal line than the incident
ray; this is the SFA rule of refraction. On the other
hand, if a light wave passes from a medium in which it travels fast (relatively
speaking) into a medium in which it travels slow, then the light wave will
refract towards the normal. In such a case, the refracted ray will be closer to
the normal line than the incident ray is; this is the FST rule
of refraction. These two rules regarding the refraction of
light only indicate the direction that a light ray bends; they do not indicate
how much bending occurs. Lesson 1 focused on the topics of "What causes
refraction?" and "Which direction does light refract?" Lesson 2
will focus on the question of "By how much does light refract when it crosses
a boundary?"
The question is: "By how much does light refract when it
crosses a boundary?" Perhaps there are numerous answers to such a
question. (For example, "a lot," "a little," "like
wow! Quite a bit dude," etc.) The concern of this lesson is to express the amount of refraction
of a light ray in terms of a measurable quantity that has a mathematical value.
The diagram to the right shows a light ray undergoing refraction as it passes
from air into water. As mentioned in Lesson 1, the incident ray is a ray
(drawn perpendicular to the wavefronts) that
shows the direction that light travels as it approaches the boundary. (The
meaning of an incident ray was first introduced in the discussion of Reflection
of Light in Unit 13 of The Physics Classroom Tutorial.)
Similarly, the refracted ray is a ray (drawn perpendicular to the wavefronts) that shows the direction that light travels
after it has crossed over the boundary. In the diagram, a normal line is drawn
to the surface at the point of incidence. This line is always drawn
perpendicular to the boundary. The angle that the incident ray makes with the
normal line is referred to as the angle of incidence. Similarly, the angle that the refracted ray makes with the normal line
is referred to as the angle of refraction. The angle of incidence and angle of refraction are denoted by the
following symbols:
|
= angle of incidence |
|
= angle of refraction |
The amount of bending that a light ray experiences can be
expressed in terms of the angle of refraction (more accurately, by the
difference between the angle of refraction and the angle of incidence). A ray
of light may approach the boundary at an angle of incidence of 45-degrees and
bend towards the normal. If the medium into which it enters causes a small
amount of refraction, then the angle of refraction might be a value of about
42-degrees. On the other hand if the medium into which the light enters causes
a large amount of refraction, the angle of refraction might be 22-degrees.
(These values are merely arbitrarily chosen values to illustrate a point.) The
diagram below depicts a ray of light approaching three different boundaries at
an angle of incidence of 45-degrees. The refractive medium is different in each
case, causing different amounts of refraction. The angles of refraction are
shown on the diagram.
Of the three boundaries in the diagram, the light ray
refracts the most at the air-diamond boundary. This is evident by the fact that
the difference between the angle of incidence and the angle of refraction is
greatest for the air-diamond boundary. But how can this be explained? The cause
of refraction is a change in light speed; and wherever the light speed changes
most, the refraction is greatest. We have already learned that the speed is
related to the optical density of a material that is related to the index of
refraction of a material. Of the four materials present in the above diagram, air
is the least dense material (lowest index of refraction value) and diamond is
the most dense material (largest index of
refraction value). Thus, it would be reasonable that the most refraction occurs
for the transmission of light across an air-diamond boundary.
In this example, the angle of refraction is the measurable
quantity that indicates the amount of refraction taking place at any boundary.
A comparison of the angle of refraction to the angle of incidence provides a
good measure of the refractive ability of any given boundary. For any given
angle of incidence, the angle of refraction is dependent upon the speeds of
light in each of the two materials. The speed is in turn dependent upon the
optical density and the index of refraction values of the two materials. There
is a mathematical equation relating the angles that the light rays make with
the normal to the indices (plural for index) of refraction of the two materials
on each side of the boundary. This mathematical equation is known as Snell's
Law.