2015

Physics Project















































Ratik Bhat

Amity International School




















Optical Fiber

and its
Applications













Name: Ratik Bhat
School: Amity International School
Roll No.:






























Index






1. Certificate
2. Acknowledgements
3. Aim
4. Important Terms
5. Optical Fibers
6. Applications
7. Principle Of Operation
8. Mechanism of Attenuation
9. Manufacturing
10.Practical Issue
11.Electronically Based Project
12.Bibliography































Acknowledgements








I would like to express my sincere gratitude to my physics mentor
Mr Rahul Gupta, for his vital support, guidance and
encouragement - without which this project would not have
come forth. I would also like to express my gratitude to the other
staffs of the Department of Physics for their support during the
making of this project.

























Aim






To Study the Optical Fibre Cable Principle and its
Applications.











Important Terms


Optical Fiber: An optical fiber (or fibre) is a glass or plastic fiber
that carries light along its length. Fiber optics is the overlap of
applied science and engineering concerned with the design and
application of optical fibers. Optical fibers are widely used in fiber-
optic communications, which permits transmission over longer
distances and at higher bandwidths (data rates) than other forms of
communications.

Refraction: Refraction is the change in direction of a wave due to a
change in its speed. This is most commonly observed when a wave
passes from one medium to another. Refraction of light is the most
commonly observed phenomenon, but any type of wave can refract
when it interacts with a medium, for example when sound waves
pass from one medium into another or when water waves move into
water of a different depth

Reflection: Reflection is the change in direction of a wavefront at
an interface between two different media so that the wavefront
returns into the medium from which it originated. Common
examples include the reflection of light, sound and water waves.

Internal Reflection


Scattering: Scattering is a general physical process where some
forms of radiation, such as light, sound, or moving particles, are
forced to deviate from a straight trajectory by one or more localized
non-uniformities in the medium through which they pass. In
conventional use, this also includes deviation of reflected radiation
from the angle predicted by the law of reflection.

Attenuation: is the gradual loss in intensity of any kind of flux
through a medium. For instance, sunlight is attenuated by dark
glasses, and X-rays are attenuated by lead.



















Optical Fiber Cable (OFC)



An optical fiber (or fibre) is a glass or plastic fiber that carries light along
its length. Fiber optics is the overlap of applied science and engineering
concerned with the design and application of optical fibers. Optical fibers
are widely used in fiber-optic communications, which permits
transmission over longer distances and at higher bandwidths (data rates)
than other forms of communications. Fibers are used instead of metal
wires because signals travel along them with less loss, and they are also
immune to electromagnetic interference. Fibers are also used for
illumination, and are wrapped in bundles so they can be used to carry
images, thus allowing viewing in tight spaces. Specially designed fibers
are used for a variety of other applications, including sensors and fiber
lasers.

Light is kept in the core of the optical fiber by total internal reflection.
This causes the fiber to act as a waveguide. Fibers which support many
propagation paths or transverse modes are called multi-mode fibers
(MMF), while those which can only support a single mode are called
single-mode fibers (SMF). Multi-mode fibers generally have a larger core
diameter, and are used for short-distance communication links and for
applications where high power must be transmitted. Single-mode fibers
are used for most communication links longer than 550 meters (1,800 ft).

Joining lengths of optical fiber is more complex than joining electrical wire
or cable. The ends of the fibers must be carefully cleaved, and then
spliced together either mechanically or by fusing them together with an
electric arc. Special connectors are used to make removable connections.











A bundle of optical fibers






























A TOSLINK fiber optic audio cable being illuminated at one end








Applications

Optical fiber communication



Optical fiber can be used as a medium for telecommunication and
networking because it is flexible and can be bundled as cables. It is
especially advantageous for long-distance communications, because light
propagates through the fiber with little attenuation compared to electrical
cables. This allows long distances to be spanned with few repeaters.
Additionally, the per-channel light signals propagating in the fiber can be
modulated at rates as high as 111 gigabits per second, although 10 or 40
Gb/s is typical in deployed systems. Each fiber can carry many
independent channels, each using a different wavelength of light
(wavelength-division multiplexing (WDM)). The net data rate (data rate
without overhead bytes) per fiber is the per-channel data rate reduced by
the FEC overhead, multiplied by the number of channels (usually up to
eighty in commercial dense WDM systems as of 2008). The current
laboratory fiber optic data rate record, held by Bell Labs in Villarceaux,
France, is multiplexing 155 channels, each carrying 100 Gbps over a 7000
km fiber.


For short distance applications, such as creating a network within an
office building, fiber-optic cabling can be used to save space in cable
ducts. This is because a single fiber can often carry much more data than
many electrical cables, such as Cat-5 Ethernet cabling. Fiber is also
immune to electrical interference; there is no cross-talk between signals
in different cables and no pickup of environmental noise. Non-armored
fiber cables do not conduct electricity, which makes fiber a good solution
for protecting communications equipment located in high voltage
environments such as power generation facilities, or metal communication
structures prone to lightning strikes. They can also be used in
environments where explosive fumes are present, without danger of
ignition. Wiretapping is more difficult compared to electrical connections,
and there are concentric dual core fibers that are said to be tap-proof.



Although fibers can be made out of transparent plastic, glass, or a
combination of the two, the fibers used in long-distance
telecommunications applications are always glass, because of the lower
optical attenuation. Both multi-mode and single-mode fibers are used in
communications, with multi-mode fiber used mostly for short distances,








up to 550 m (600 yards), and single-mode fiber used for longer distance
links. Because of the tighter tolerances required to couple light into and
between single-mode fibers (core diameter about 10 micrometers),
single-mode transmitters, receivers, amplifiers and other components are
generally more expensive than multi-mode components.

Fiber optic sensors

Fibers have many uses in remote sensing. In some applications, the
sensor is itself an optical fiber. In other cases, fiber is used to connect a
non-fiberoptic sensor to a measurement system. Depending on the
application, fiber may be used because of its small size, or the fact that
no electrical power is needed at the remote location, or because many
sensors can be multiplexed along the length of a fiber by using different
wavelengths of light for each sensor, or by sensing the time delay as light
passes along the fiber through each sensor. Time delay can be
determined using a device such as an optical time-domain reflectometer.



Optical fibers can be used as sensors to measure strain, temperature,
pressure and other quantities by modifying a fiber so that the quantity to
be measured modulates the intensity, phase, polarization, wavelength or
transit time of light in the fiber. Sensors that vary the intensity of light
are the simplest, since only a simple source and detector are required. A
particularly useful feature of such fiber optic sensors is that they can, if
required, provide distributed sensing over distances of up to one meter.



Extrinsic fiber optic sensors use an optical fiber cable, normally a multi-
mode one, to transmit modulated light from either a non-fiber optical
sensor, or an electronic sensor connected to an optical transmitter. A
major benefit of extrinsic sensors is their ability to reach places which are
otherwise inaccessible. An example is the measurement of temperature
inside aircraft jet engines by using a fiber to transmit radiation into a
radiation pyrometer located outside the engine. Extrinsic sensors can also
be used in the same way to measure the internal temperature of electrical
transformers, where the extreme electromagnetic fields present make
other measurement techniques impossible. Extrinsic sensors are used to
measure vibration, rotation, displacement, velocity, acceleration, torque,
and twisting.








Other uses of optical fibers

Fibers are widely used in illumination applications. They are used as light
guides in medical and other applications where bright light needs to be
shone on a target without a clear line-of-sight path. In some buildings,
optical fibers are used to route sunlight from the roof to other parts of the
building (see non-imaging optics). Optical fiber illumination is also used
=for decorative applications, including signs, art, and artificial Christmas
trees. Swarovski boutiques use optical fibers to illuminate their crystal
showcases from many different angles while only employing one light
source. Optical fiber is an intrinsic part of the light-transmitting concrete
building product, LiTraCon.




Optical fiber is also used in imaging optics. A coherent bundle of fibers is
used, sometimes along with lenses, for a long, thin imaging device called
an endoscope, which is used to view objects through a small hole. Medical
endoscopes are used for minimally invasive exploratory or surgical
procedures (endoscopy). Industrial endoscopes (see fiberscope or
borescope) are used for inspecting anything hard to reach, such as jet
engine interiors.




In spectroscopy, optical fiber bundles are used to transmit light from a
spectrometer to a substance which cannot be placed inside the
spectrometer itself, in order to analyze its composition. A spectrometer
analyzes substances by bouncing light off of and through them. By using
fibers, a spectrometer can be used to study objects that are too large to
fit inside, or gasses, or reactions which occur in pressure vessels.




An optical fiber doped with certain rare earth elements such as erbium
can be used as the gain medium of a laser or optical amplifier. Rare-earth
doped optical fibers can be used to provide signal amplification by splicing
a short section of doped fiber into a regular (undoped) optical fiber line.
The doped fiber is optically pumped with a second laser wavelength that
is coupled into the line in addition to the signal wave. Both wavelengths of
light are transmitted through the doped fiber, which transfers energy
from the second pump wavelength to the signal wave. The process that
causes the amplification is stimulated emission.













A frisbee illuminated by fiber optics



Light reflected from optical fiber illuminates exhibited model
































Optical fibers doped with a wavelength shifter are used to collect
scintillation light in physics experiments.

Optical fiber can be used to supply a low level of power (around one watt)
to electronics situated in a difficult electrical environment. Examples of
this are electronics in high-powered antenna elements and measurement
devices used in high voltage transmission equipment.








Principle of Operation
An optical fiber is a cylindrical dielectric waveguide (non conducting
waveguide) that transmits light along its axis, by the process of total
internal reflection. The fiber core is surrounded by a cladding layer

Index of Refraction

The index of refraction is a way of measuring the speed of light in a
material. Light travels fastest in a vacuum, such as outer space. The
actual speed of light in a vacuum is about 300 million meters (186
thousand miles) per second. Index of refraction is calculated by dividing
the speed of light in a vacuum by the speed of light in some other
medium. The index of refraction of a vacuum is therefore 1, by definition.
The typical value for the cladding of an optical fiber is 1.46. The core
value is typically 1.48. The larger the index of refraction, the slower light
travels in that medium. From this information, a good rule of thumb is
that signal using optical fiber for communication will travel at around 200
million meters per second. Or to put it another way, to travel 1000
kilometres in fiber, the signal will take 5 milliseconds to propagate. Thus a
phone call carried by fiber between Sydney and New York, a 12000
kilometre distance, means that there is an absolute minimum delay of 60
milliseconds (or around 1/16th of a second) between when one caller
speaks to when the other hears. (Of course the fiber in this case will
probably travel a longer route, and there will be additional delays due to
communication equipment switching and the process of encoding and
decoding the voice onto the fiber).


















Total Internal Reflection

When light travelling in a dense medium hits a boundary at a steep angle
(larger than the "critical angle" for the boundary), the light will be
completely reflected. This effect is used in optical fibers to confine light in
the core. Light travels along the fiber bouncing back and forth off of the
boundary. Because the light must strike the boundary with an angle
greater than the critical angle, only light that enters the fiber within a
certain range of angles can travel down the fiber without leaking out. This
range of angles is called the acceptance cone of the fiber. The size of this
acceptance cone is a function of the refractive index difference between
the fiber's core and cladding.

In simpler terms, there is a maximum angle from the fiber axis at which
light may enter the fiber so that it will propagate, or travel, in the core of
the fiber. The sine of this maximum angle is the numerical aperture (NA)
of the fiber. Fiber with a larger NA requires less precision to splice and
work with than fiber with a smaller NA. Single-mode fiber has a small NA.











A laser bouncing down an acrylic rod, illustrating the total internal reflection of light in a
multi-mode optical fiber.











Single Mode Fiber

Fiber with a core diameter less than about ten times the wavelength of
the propagating light cannot be modeled using geometric optics. Instead,
it must be analyzed as an electromagnetic structure, by solution of
Maxwell's equations as reduced to the electromagnetic wave equation.
The electromagnetic analysis may also be required to understand
behaviours such as speckle that occur when coherent light propagates in
multi-mode fiber. As an optical waveguide, the fiber supports one or more
confined transverse modes by which light can propagate along the fiber.
Fiber supporting only one mode is called single-mode or mono-mode
fiber. The behaviour of larger-core multi-mode fiber can also be modeled
using the wave equation, which shows that such fiber supports more than
one mode of propagation (hence the name). The results of such modeling
of multi-mode fiber approximately agree with the predictions of geometric
optics, if the fiber core is large enough to support more than a few
modes.





The structure of a typical single-mode fiber.
1. Core: 8 m diameter
2. Cladding: 125 m dia.
3. Buffer: 250 m dia.
4. Jacket: 400 m dia.













Multi Mode Fiber

The propagation of light through a multi-mode optical fiber.
A laser bouncing down an acrylic rod, illustrating the total internal
reflection of light in a multi-mode optical fiber.

Fiber with large core diameter (greater than 10 micrometers) may be
analyzed by geometrical optics. Such fiber is called multi-mode fiber, from
the electromagnetic analysis (see below). In a step-index multi-mode
fiber, rays of light are guided along the fiber core by total internal
reflection. Rays that meet the core-cladding boundary at a high angle
(measured relative to a line normal to the boundary), greater than the
critical angle for this boundary, are completely reflected. The critical angle
(minimum angle for total internal reflection) is determined by the
difference in index of refraction between the core and cladding materials.
Rays that meet the boundary at a low angle are refracted from the core
into the cladding, and do not convey light and hence information along
the fiber. The critical angle determines the acceptance angle of the fiber,
often reported as a numerical aperture. A high numerical aperture allows
light to propagate down the fiber in rays both close to the axis and at
various angles, allowing efficient coupling of light into the fiber. However,
this high numerical aperture increases the amount of dispersion as rays at
different angles have different path lengths and therefore take different
times to traverse the fiber.





















The propagation of light through a multi-mode optical fiber.











Single-Mode Optical Fiber Cable





























Multi-Mode Optical fiber cables

(Multiple Fiber Channel)










Mechanisms of Attenuation
Attenuation in fiber optics, also known as transmission loss, is the
reduction in intensity of the light beam (or signal) with respect to distance
travelled through a transmission medium. Attenuation coefficients in fiber
optics usually use units of dB/km through the medium due to the
relatively high quality of transparency of modern optical transmission
media. The medium is typically usually a fiber of silica glass that confines
the incident light beam to the inside. Attenuation is an important factor
limiting the transmission of a digital signal across large distances. Thus,
much research has gone into both limiting the attenuation and
maximizing the amplification of the optical signal. Empirical research has
shown that attenuation in optical fiber is caused primarily by both
scattering and absorption.

Light scattering

The propagation of light through the core of an optical fiber is based on
total internal reflection of the lightwave. Rough and irregular surfaces,
even at the molecular level, can cause light rays to be reflected in random
directions. This is called diffuse reflection or scattering, and it is typically
characterized by wide variety of reflection angles.

Light scattering depends on the wavelength of the light being scattered.
Thus, limits to spatial scales of visibility arise, depending on the frequency
of the incident light-wave and the physical dimension (or spatial scale) of
the scattering center, which is typically in the form of some specific
micro-structural feature.
























Specular reflection
















Diffuse reflection




Thus, attenuation results from the incoherent scattering of light at internal
surfaces and interfaces. In (poly)crystalline materials such as metals and
ceramics, in addition to pores, most of the internal surfaces or interfaces
are in the form of grain boundaries that separate tiny regions of
crystalline order. It has recently been shown that when the size of the
scattering centre (or grain boundary) is reduced below the size of the
wavelength of the light being scattered, the scattering no longer occurs to
any significant extent. This phenomenon has given rise to the production
of transparent ceramic materials.

Similarly, the scattering of light in optical quality glass fiber is caused by
molecular level irregularities (compositional fluctuations) in the glass
structure. Indeed, one emerging school of thought is that a glass is
simply the limiting case of a polycrystalline solid. Within this framework,
"domains" exhibiting various degrees of short-range order become the
building blocks of both metals and alloys, as well as glasses and ceramics.
Distributed both between and within these domains are micro-structural
defects which will provide the most ideal locations for the occurrence of
light scattering. This same phenomenon is seen as one of the limiting
factors in the transparency of IR missile domes.











Materials
Manufacturing

Glass optical fibers are almost always made from silica, but some other
materials, such as fluorozirconate, fluoroaluminate, and chalcogenide
glasses, are used for longer-wavelength infrared applications. Like other
glasses, these glasses have a refractive index of about 1.5. Typically the
difference between core and cladding is less than one percent.

Plastic optical fibers (POF) are commonly step-index multi-mode fibers
with a core diameter of 0.5 millimeters or larger. POF typically have
higher attenuation coefficients than glass fibers, 1 dB/m or higher, and
this high attenuation limits the range of POF-based systems.

Silica

Silica exhibits fairly good optical transmission over a wide range of
wavelengths. In the near-infrared (near IR) portion of the spectrum,
particularly around 1.5 m, silica can have extremely low absorption and
scattering losses of the order of 0.2dB/km. A high transparency in the
1.4-m region is achieved by maintaining a low concentration of hydroxyl
groups (OH). Alternatively, a high OH concentration is better for
transmission in the ultraviolet (UV) region.

Silica can be drawn into fibers at reasonably high temperatures, and has a
fairly broad glass transformation range. One other advantage is that
fusion splicing and cleaving of silica fibers is relatively effective. Silica
fiber also has high mechanical strength against both pulling and even
bending, provided that the fiber is not too thick and that the surfaces
have been well prepared during processing. Even simple cleaving
(breaking) of the ends of the fiber can provide nicely flat surfaces with
acceptable optical quality. Silica is also relatively chemically inert. In
particular, it is not hygroscopic (does not absorb water).

Silica glass can be doped with various materials. One purpose of doping is
to raise the refractive index (e.g. with Germanium dioxide (GeO2) or
Aluminium oxide (Al2O3)) or to lower it (e.g. with fluorine or Boron
trioxide (B2O3)). Doping is also possible with laser-active ions (for
example, rare earth-doped fibers) in order to obtain active fibers to be
used, for example, in fiber amplifiers or laser applications. Both the fiber
core and cladding are typically doped, so that the entire assembly (core
and cladding) is effectively the same compound (e.g. an aluminosilicate,
germanosilicate, phosphosilicate or borosilicate glass).











Particularly for active fibers, pure silica is usually not a very suitable host
glass, because it exhibits a low solubility for rare earth ions. This can lead
to quenching effects due to clustering of dopant ions. Aluminosilicates are
much more effective in this respect.

Silica fiber also exhibits a high threshold for optical damage. This property
ensures a low tendency for laser-induced breakdown. This is important for
fiber amplifiers when utilized for the amplification of short pulses.

Because of these properties silica fibers are the material of choice in
many optical applications, such as communications (except for very short
distances with plastic optical fiber), fiber lasers, fiber amplifiers, and
fiber-optic sensors. The large efforts which have been put forth in the
development of various types of silica fibers have further increased the
performance of such fibers over other materials.

















Tetrahedral structural unit of silica (SiO2).

The amorphous structure of glassy silica (SiO2).









Process

Standard optical fibers are made by first constructing a large-diameter
preform, with a carefully controlled refractive index profile, and then
pulling the preform to form the long, thin optical fiber. The preform is
commonly made by three chemical vapor deposition methods: inside
vapor deposition, outside vapor deposition, and vapor axial deposition.

With inside vapor deposition, the preform starts as a hollow glass tube
approximately 40 centimeters (16 in) long, which is placed horizontally
and rotated slowly on a lathe. Gases such as silicon tetrachloride (SiCl4)
or germanium tetrachloride (GeCl4) are injected with oxygen in the end of
the tube. The gases are then heated by means of an external hydrogen
burner, bringing the temperature of the gas up to 1900 K (1600 C, 3000
F), where the tetrachlorides react with oxygen to produce silica or
germania (germanium dioxide) particles. When the reaction conditions are
chosen to allow this reaction to occur in the gas phase throughout the
tube volume, in contrast to earlier techniques where the reaction occurred
only on the glass surface, this technique is called modified chemical vapor
deposition.

Coatings

Fiber optic coatings are UV-cured urethane acrylate composite materials
applied to the outside of the fiber during the drawing process. The
coatings protect the very delicate strands of glass fiberabout the size of
a human hairand allow it to survive the rigors of manufacturing, proof
testing, cabling and installation.

Todays glass optical fiber draw processes employ a dual-layer coating
approach. An inner primary coating is designed to act as a shock absorber
to minimize attenuation caused by microbending. An outer secondary
coating protects the primary coating against mechanical damage and acts
as a barrier to lateral forces.

These fiber optic coating layers are applied during the fiber draw, at
speeds approaching 100 kilometers per hour (60 mph). Fiber optic
coatings are applied using one of two methods: wet-on-dry, in which the
fiber passes through a primary coating application, which is then UV
cured, then through the secondary coating application which is
subsequently cured; and wet-on-wet, in which the fiber passes through
both the primary and secondary coating applications and then goes to UV
curing.











Fiber optic coatings are applied in concentric layers to prevent damage to
the fiber during the drawing application and to maximize fiber strength
and microbend resistance. Unevenly coated fiber will experience non-
uniform forces when the coating expands or contracts, and is susceptible
to greater signal attenuation. Under proper drawing and coating
processes, the coatings are concentric around the fiber, continuous over
the length of the application and have constant thickness.

Fiber optic coatings protect the glass fibers from scratches that could lead
to strength degradation. The combination of moisture and scratches
accelerates the aging and deterioration of fiber strength. When fiber is
subjected to low stresses over a long period, fiber fatigue can occur. Over
time or in extreme conditions, these factors combine to cause microscopic
flaws in the glass fiber to propagate, which can ultimately result in fiber
failure.








































Illustration of the modified chemical vapour deposition (inside) process








Practical issues

Optical fiber cables

In practical fibers, the cladding is usually coated with a tough resin buffer
layer, which may be further surrounded by a jacket layer, usually plastic.
These layers add strength to the fiber but do not contribute to its optical
wave guide properties. Rigid fiber assemblies sometimes put light-
absorbing ("dark") glass between the fibers, to prevent light that leaks
out of one fiber from entering another. This reduces cross-talk between
the fibers, or reduces flare in fiber bundle imaging applications.

Modern cables come in a wide variety of sheathings and armor, designed
for applications such as direct burial in trenches, high voltage isolation,
dual use as power lines,[40][not in citation given] installation in conduit,
lashing to aerial telephone poles, submarine installation, and insertion in
paved streets. The cost of small fiber-count pole-mounted cables has
greatly decreased due to the high Japanese and South Korean demand for
fiber to the home (FTTH) installations.

Fiber cable can be very flexible, but traditional fiber's loss increases
greatly if the fiber is bent with a radius smaller than around 30 mm. This
creates a problem when the cable is bent around corners or wound
around a spool, making FTTX installations more complicated. "Bendable
fibers", targeted towards easier installation in home environments, have
been standardized as ITU-T G.657. This type of fiber can be bent with a
radius as low as 7.5 mm without adverse impact. Even more bendable
fibers have been developed. Bendable fiber may also be resistant to fiber
hacking, in which the signal in a fiber is surreptitiously monitored by
bending the fiber and detecting the leakage.

Another important feature of cable is cable withstanding against the
horizontally applied force. It is technically called max tensile strength
defining how much force can applied to the cable during the installation of
a period.

Telecom Anatolia fiber optic cable versions are reinforced with aramid
yarns or glass yarns as intermediary strength member. In commercial
terms, usages of the glass yarns are more cost effective while no loss in
mechanical durability of the cable. Glass yarns are also protect the cable
core against rodents and termites.








Termination and splicing

Optical fibers are connected to terminal equipment by optical fiber
connectors. These connectors are usually of a standard type such as FC,
SC, ST, LC, or MTRJ.

Optical fibers may be connected to each other by connectors or by
splicing, that is, joining two fibers together to form a continuous optical
waveguide. The generally accepted splicing method is arc fusion splicing,
which melts the fiber ends together with an electric arc. For quicker
fastening jobs, a "mechanical splice" is used.

Fusion splicing is done with a specialized instrument that typically
operates as follows: The two cable ends are fastened inside a splice
enclosure that will protect the splices, and the fiber ends are stripped of
their protective polymer coating (as well as the more sturdy outer jacket,
if present). The ends are cleaved (cut) with a precision cleaver to make
them perpendicular, and are placed into special holders in the splicer. The
splice is usually inspected via a magnified viewing screen to check the
cleaves before and after the splice. The splicer uses small motors to align
the end faces together, and emits a small spark between electrodes at the
gap to burn off dust and moisture. Then the splicer generates a larger
spark that raises the temperature above the melting point of the glass,
fusing the ends together permanently. The location and energy of the
spark is carefully controlled so that the molten core and cladding don't
mix, and this minimizes optical loss. A splice loss estimate is measured by
the splicer, by directing light through the cladding on one side and
measuring the light leaking from the cladding on the other side. A splice
loss under 0.1 dB is typical. The complexity of this process makes fiber
splicing much more difficult than splicing copper wire.

Mechanical fiber splices are designed to be quicker and easier to install,
but there is still the need for stripping, careful cleaning and precision
cleaving. The fiber ends are aligned and held together by a precision-
made sleeve, often using a clear index-matching gel that enhances the
transmission of light across the joint. Such joints typically have higher
optical loss and are less robust than fusion splices, especially if the gel is
used. All splicing techniques involve the use of an enclosure into which
the splice is placed for protection afterward.








Optical Fiber splicing




Fiber fuse

At high optical intensities, above 2 megawatts per square centimetre,
when a fiber is subjected to a shock or is otherwise suddenly damaged, a
fiber fuse can occur. The reflection from the damage vaporizes the fiber
immediately before the break, and this new defect remains reflective so
that the damage propagates back toward the transmitter at 13 meters
per second (411 km/h, 28 mph). The open fiber control system, which
ensures laser eye safety in the event of a broken fiber, can also
effectively halt propagation of the fiber fuse. In situations, such as
undersea cables, where high power levels might be used without the need
for open fiber control, a "fiber fuse" protection device at the transmitter
can break the circuit to prevent any damage.







Electronically Based Project



To Test Passage of Light through Commercial/Industrial

Optical Fiber Cable (OFC)






Devices Used:

1. Industrial Optical Fiber Cable(Multi-Mode)
2. LED(3V)
3. PCB Circuit Board
4. 3VDC Rectifier.


















Books:
Bibliography

Physics (Part 1&2) Textbook for Class XII; National
Council of Educational Research and Training
Encyclopaedias

Websites:


Image Courtesy:

www.google.com/images
www.wikipedia.org

Source and other Information:

www.google.com
www.icbse.com
www.wikipedia.org