normal. Consider a light ray moving at an angle
other than 90 degrees through the boundary between glass and a
diamond. The glass has an index of refraction of about 1.523.
The diamond has an index of refraction of about 2.419.
Therefore, the ray that continues into the diamond will be bent
towards the normal. When that light ray crosses the boundary
between the diamond and the air at some angle other than 90
degrees, it will be bent away from the normal. The reason for
this is that air has a lower index of refraction, about 1.000
than the index of refraction of the diamond. Interactive
Media Activity Interactivity: Optical Refraction This
activity shows how refraction works in different materials
(starting from a vacuum). Web Links The Transmission of
Wave through Dense media – Reflection and Refraction
http://www.phy.ntnu.edu.tw/java/ propagation/ propagation.html
Content 3.2 Optical Media 3.2.5
Total internal reflection A light ray that is being
turned on and off to send data (1s and 0s) into an optical
fiber must stay inside the fiber until it reaches the far end.
The ray must not refract into the material wrapped around the
outside of the fiber. The refraction would cause the loss of
part of the light energy of the ray. A design must be achieved
for the fiber that will make the outside surface of the fiber
act like a mirror to the light ray moving through the fiber. If
any light ray that tries to move out through the side of the
fiber were reflected back into the fiber at an angle that sends
it towards the far end of the fiber, this would be a good
“pipe” or “wave guide” for the light waves. The laws of
reflection and refraction illustrate how to design a fiber that
guides the light waves through the fiber with a minimum energy
loss. The following two conditions must be met for the light
rays in a fiber to be reflected back into the fiber without any
loss due to refraction: - The core of the optical fiber
has to have a larger index of refraction (n) than the material
that surrounds it. The material that surrounds the core of the
fiber is called the cladding.
- The angle of incidence
of the light ray is greater than the critical angle for the
core and its cladding.
When both of these
conditions are met, the entire incident light in the fiber is
reflected back inside the fiber. This is called total internal
reflection, which is the foundation upon which optical fiber is
constructed. Total internal reflection causes the light rays in
the fiber to bounce off the core-cladding boundary and continue
its journey towards the far end of the fiber. The light will
follow a zigzag path through the core of the fiber. A fiber
that meets the first condition can be easily created. In
addition, the angle of incidence of the light rays that enter
the core can be controlled. Restricting the following two
factors controls the angle of incidence: - The
numerical aperture of the fiber – The numerical aperture of
a core is the range of angles of incident light rays entering
the fiber that will be completely reflected.
- Modes – The paths which a light ray can follow when
traveling down a fiber.
By controlling both
conditions, the fiber run will have total internal reflection.
This gives a light wave guide that can be used for data
communications. Web Links Total Internal Reflection
http://www.glenbrook.k12.il.us/gbssci/
phys/Class/refrn/u14l3b.html
Content 3.2
Optical Media 3.2.6 Multimode fiber The
part of an optical fiber through which light rays travel is
called the core of the fiber. Light rays can only enter the
core if their angle is inside the numerical aperture of the
fiber. Likewise, once the rays have entered the core of the
fiber, there are a limited number of optical paths that a light
ray can follow through the fiber. These optical paths are
called modes. If the diameter of the core of the fiber is large
enough so that there are many paths that light can take through
the fiber, the fiber is called “multimode” fiber. Single-mode
fiber has a much smaller core that only allows light rays to
travel along one mode inside the fiber. Every fiber-optic
cable used for networking consists of two glass fibers encased
in separate sheaths. One fiber carries transmitted data from
device A to device B. The second fiber carries data from device
B to device A. The fibers are similar to two one-way streets
going in opposite directions. This provides a full-duplex
communication link. Just as copper twisted-pair uses separate
wire pairs to transmit and receive, fiber-optic circuits use
one fiber strand to transmit and one to receive. Typically,
these two fiber cables will be in a single outer jacket until
they reach the point at which connectors are attached. Until
the connectors are attached, there is no need for twisting or
shielding, because no light escapes when it is inside a fiber.
This means there are no crosstalk issues with fiber. It is very
common to see multiple fiber pairs encased in the same cable.
This allows a single cable to be run between data closets,
floors, or buildings. One cable can contain 2 to 48 or more
separate fibers. With copper, one UTP cable would have to be
pulled for each circuit. Fiber can carry many more bits per
second and carry them farther than copper can. Usually, five
parts make up each fiber-optic cable. The parts are the core,
the cladding, a buffer, a strength material, and an outer
jacket. The core is the light transmission element at the
center of the optical fiber. All the light signals travel
through the core. A core is typically glass made from a
combination of silicon dioxide (silica) and other elements.
Multimode uses a type of glass, called graded index glass for
its core. This glass has a lower index of refraction towards
the outer edge of the core. Therefore, the outer area of the
core is less optically dense than the center and light can go
faster in the outer part of the core. This design is used
because a light ray following a mode that goes straight down
the center of the core does not have as far to travel as a ray
following a mode that bounces around in the fiber. All rays
should arrive at the end of the fiber together. Then the
receiver at the end of the fiber receives a strong flash of
light rather than a long, dim pulse. Surrounding the core is
the cladding. Cladding is also made of silica but with a lower
index of refraction than the core. Light rays traveling through
the fiber core reflect off this core-to-cladding interface as
they move through the fiber by total internal reflection.
Standard multimode fiber-optic cable is the most common type of
fiber-optic cable used in LANs. A standard multimode
fiber-optic cable uses an optical fiber with either a 62.5 or a
50-micron core and a 125-micron diameter cladding. This is
commonly designated as 62.5/125 or 50/125 micron optical fiber.
A micron is one millionth of a meter (1µ). Surrounding the
cladding is a buffer material that is usually plastic. The
buffer material helps shield the core and cladding from damage.
There are two basic cable designs. They are the loose-tube and
the tight-buffered cable designs. Most of the fiber used in
LANs is tight-buffered multimode cable. Tight-buffered cables
have the buffering material that surrounds the cladding in
direct contact with the cladding. The most practical difference
between the two designs is the applications for which they are
used. Loose-tube cable is primarily used for outside-building
installations, while tight-buffered cable is used inside
buildings. The strength material surrounds the buffer,
preventing the fiber cable from being stretched when installers
pull it. The material used is often Kevlar, the same material
used to produce bulletproof vests. The final element is the
outer jacket. The outer jacket surrounds the cable to protect
the fiber against abrasion, solvents, and other contaminants.
The color of the outer jacket of multimode fiber is usually
orange, but occasionally another color. Infrared Light
Emitting Diodes (LEDs) or Vertical Cavity Surface Emitting