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Fiber Fiber Optics Optics

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Fiber Optics. Introduction Optical fiber is a long thin transparent dielectric material which carries EM waves of visible and IR frequencies from one end to the other end of the fiber by means of TIR . NOTE: Glass or Plastic is used as Dielectric material. - PowerPoint PPT Presentation

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Page 1: Fiber Optics

Fiber Fiber OpticsOptics

Page 2: Fiber Optics

Introduction

Optical fiber is a long thin transparent dielectric material which carries EM waves of visible and IR frequencies from one end to the other end of the fiber by means of TIR.

NOTE: Glass or Plastic is used as Dielectric material.

Optical fibers works as Wave guides in optical television signals, digital data to transmit voice television signals, digital data to any desired distance from one end to the other end of the fiber.

Page 3: Fiber Optics

Optical fiber consists of three sections

1. Core 2. Cladding 3. Protective Jacket

Core: It is an inner cylindrical material made up of glass or plastic.

Cladding: It is a cylindrical shell of glass or plastic material in which Core is inserted.

Protective Jacket: The Cladding is enclosed in polyurethane jacket and it protects the fiber from surroundings.

NOTE: The RI of core is slightly greater than the RI of Cladding. The normal standard values are 1.48 and 1.46 respectively.

Page 4: Fiber Optics

Structure of an Optical fiber

Poly urethane protective jacket

Cladding

Core

• Principle: Optical fiber works on the principle of TIR. Once light ray enters into core ,it propagates by means of multiple TIR’ s at core-cladding interface.

Page 5: Fiber Optics

c c

DENSAR MEDIUM

RERAR MEDIUM

NORMAL

NORMAL

r r = 90

Page 6: Fiber Optics

c

NORMAL

RERAR MEDIUM

DENSAR MEDIUM

Page 7: Fiber Optics

1

2

0

1

2

0

21

sin

90sinsin

90

sinsin

n

n

n

n

r

rnn

refractionoflawtoaccording

c

c

c

Page 8: Fiber Optics

Acceptance Angle

• The maximum angle of incidence at the end face of an Optical fiber for which the light ray can be propagated along Core-Cladding interface is known as maximum Acceptance angle. It is also called Acceptance cone half angle.

Page 9: Fiber Optics

Core-Cladding interface

Fiber axis

Core n1

Cladding n2

A

B

C

θr

θi

θr θ

Incident light ray

Page 10: Fiber Optics

Applying Snell’ s law for Air-Core media

)2.........(cossin

cossin

)90sin(sin

90

90

)1....(..........sinsin

0

1

10

010

0

0

10

n

n

nn

nn

ABCtriangleanglerightthefrom

nn

i

i

i

r

r

ri

Page 11: Fiber Optics

)4..(..........cos

)(1sin1cos

sin

90sinsin

90

sinsin

)3......(..........cossin

)(

1

22

21

2

1

22

1

2

0

1

2

0

21

0

1

n

nn

n

n

n

n

n

n

ri

rnin

refractionoflawtoaccording

n

n

anglecriticalwhen

c

cc

c

c

c

cm

mic

Page 12: Fiber Optics

22

21

1max

22

21

0

1

22

21

0

1

sin

sin

1,

sin

)3()4(

nn

nn

nthenairisfiberthegsurroundinmediumtheif

n

nn

n

n

inequationsubstitute

m

m

Which is required expression for Maximum Acceptance Angle in optical fibers.

Page 13: Fiber Optics

Acceptance Cone Rotating the Acceptance angle about the fiber axis describes the Acceptance Cone of the fiber.Light launched at the fiber end within this Acceptance Cone alone will be accepted and propagated to the other end of the fiber by total internal reflection.

θm

θm

Acceptance Cone

Page 14: Fiber Optics

Numerical Aperture

• The light gathering capacity of an optical fiber is known as Numerical Aperture and it is proportional to Acceptance Angle.

• It is numerically equal to sine of minimum Acceptance Angle.

2

2

)(

))((

sin

sin

1

21

21

211

1

21

2121

22

21

0

22

21

max

max

nNA

nNA

nn

nnnNA

n

nn

nnnnNA

nnNA

n

nn

NA

The ratio between the difference in RI’s of Core and Cladding to that of RI of core is called the fractional change.

Page 15: Fiber Optics

TYPES OF OPTICAL FIBRES

On the basis of variation of RI of core, the optical fibers are mainly classified into following types. i.e., 1.Step Index fiber 2.Gradex Index fiber

NOTE: Based on Mode of propagation, the fibers are further divided into Single Mode and Multi Mode.

Page 16: Fiber Optics

Single Mode Step Index fiber

The RI is constant for the core in this fiber. As we go radically from center of the core, the RI undergoes a step change at core-cladding interface .

The core diameter of this fiber is about 8 to 10µm and the outer diameter of cladding is 60 to 70µm.

There is only one path for light ray propagation. Hence it is called single mode step index fiber.

It is a reflective fiber since light is transmitted from one end to the other end of a fiber by TIR.

These are extensively used because distortion and transmission losses are very less.

Page 17: Fiber Optics

Refractive index profile of single mode step index fiber

Radial distance

60 to 70 µm

8 to 10 µm

RI

Page 18: Fiber Optics

SINGLE MODE STEP INDEX FIBER

CORE

CLADDING

RAY PROPAGATION

Page 19: Fiber Optics

Multimode Step Index Fiber

The construction of this fiber is similar to Single mode step index fiber but dimensions of Core and Cladding are much larger to have more number of paths for light propagation.

The Core diameter varies from 50 to 200µm and the Cladding diameter varies from 100 to 250µm.

It is also a reflective fiber since light is propagated in the form of multiple TIRS.

Page 20: Fiber Optics

Radial distance

100 to 250 µm

50 to 200 µm

RI

REFRACTIVE INDEX PROFILE OF MULTI MODE STEP INDEX FIBRE

Page 21: Fiber Optics

GRADED INDEX FIBRE

In this fiber , Radially the RI of Core continuously decreases from center to the surface.

The RI is maximum at the center of Core and Minimum at the Surface.

This fiber can be a single mode or Multimode ,the diameters of core and cladding varies from 50-200µm and 100-250µm respectively.

Page 22: Fiber Optics

Radial distnce

100 to 2500 µm

50 to 200 µm

RI

REFRACTIVE INDEX PROFILE OF SINGLE MODE GRADED INDEX FIBER

Page 23: Fiber Optics

Radial distance

100 to 250 µm

50 to 200 µm

RI

REFRACTIVE INDEX PROFILE OF MULTIMODE GRADED INDEX FIBRE

Page 24: Fiber Optics

• As RI changes continuously radially in Core, the light rays suffers continuous refraction with in the Core from its center to surface.

• Thus the propagation of light rays are not due to TIR but by refraction. Therefore it is called Refractive fiber.

• In this fiber, the light rays travel at different speeds in different parts.

• Near the surface RI is least so, the light rays travel faster compared to the light rays near the axis. Because of this all the rays almost arrive at the same time at the other end of the fiber.

Page 25: Fiber Optics

CLADDING

CORE

LIGHT PROPAGATION IN MUTI-MODE GRADED INDEX FIBRE

Page 26: Fiber Optics

Optical fiber Communication System

• An efficient optical fiber communication system requires high information carrying capacity such as voice signals, video signals over long distances with a minimum number of repeaters. It essentially consists of following parts.

1.Encoder 2. Transmitter 3.Wave guide

4.Receiver 5.Decoder

Page 27: Fiber Optics

• 1.Encoder: It converts electric signal corresponding to analog information such as voice, figures, objects etc into a binary data. This binary data comes out in the form of stream of electrical pulses.

• 2.TRANSMITTER: It mainly consists of drive circuit and a light source. Drive circuit supplies the electric pulses to the light source from the encoder.

• NOTE: LED or diode laser is used as light source and it

converts electrical signals are infected into optical signals. These optical signals are injected into wave guide.

Page 28: Fiber Optics

Electrical signal

ENCODER

DRIVE SOURCE LIGHT SOURCE

TRANSMITTER

OPTICAL SIGNAL

AMPLIFIER

PHOTO DETECTOR

SIGNAL RESTORER

DECODER

Wave guide

receiver

Page 29: Fiber Optics

Attenuation or Power loss in Optical fibers

• The power of the light at the out put end is found to be always less than the power launched at the input end.

• Attenuation is found t be a function of fiber material, wavelength of light and length of the fiber and it is measured in terms of the decibel.

Attenuation mainly three types…. 1.Scattering losses 2.Absorption losses 3.Bending losses