Download presentation
1
Optical Fiber Basics-Part 2
Prof. Manoj Kumar Dept. of Electronics and Communication Engineering DAVIET Jalandhar Lecture 3
2
Single-Mode Step Index Fiber
The Core diameter is 8 to 9mm All the multiple-mode or multimode effects are eliminated However, pulse spreading remains Bandwidth range 100GHz-Km Lecture 3
3
Typical Core and Cladding Diameters (mm)
Lecture 3
4
Multiple OFC Lecture 3
5
Standard Optical Core Size
The standard telecommunications core sizes in use today are: 8.3 µm (single-mode), µm (multimode) Lecture 3
6
How a light ray enters an optical fiber
Lecture 3
7
Numerical Aperture (NA)
The numerical aperture (NA) is a measurement of the ability of an optical fiber to capture light. The NA is also used to define the acceptance cone of an optical fiber. OR Numerical aperture (NA) determines the light accepting ability of a fiber Lecture 3
8
Light Guidance in Optical Fiber
Lecture 3
9
Low-order and high-order modes
Lecture 3
10
PROPERTIES OF OPTICAL FIBER TRANSMISSION
Lecture 3
11
Fiber Loss & Dispersion
dB/Km at 1.3mm - 0.2 dB/Km at 1.5mm - Minimum Reduction Expected in future is 0.01dB/Km Fiber Dispersion -Material dispersion - Waveguide Dispersion - Multimode group Delay Dispersion Lecture 3
12
What is Group Velocity ? Group Velocity (Vg) is Considered as the velocity of energy propagating in the direction of the axis of the guide fiber. In order to convey intelligence; Modulation is done. When is done, there are group velocities those must be propagating along the fiber. The waves of different frequencies in the group will be transmitted with slightly different velocities. Vg = dw/db. Lecture 3
13
Cause of Fiber Dispersion
Types of Dispersion Multimode Dispersion Material Dispersion Waveguide Dispersion - Multimode group delay/dispersion is the variation in group velocity among the propagation modes at a single frequency - Material Dispersion is due to variation in the refractive index of the core material as a function of wavelength. - Waveguide dispersion depends upon the fiber design. The propagation constant which is the function of the ratio of fiber dimension (i.e. core radius) to the wavelength. Lecture 3
14
Dispersion Curves Lecture 3
15
Lecture 3
16
Lecture 3
17
Dispersion in Optical Fibers
There are two main types of dispersion that cause pulse spreading in a fiber: - Chromatic dispersion - Inter-modal dispersion Dispersion is typically measured as a time spread per distance traveled (s/km) Single-mode fiber has only one mode, so inter-modal dispersion is not an issue In multimode fiber, inter-modal dispersion is the dominant cause of dispersion, but chromatic dispersion can be important at 850 nm Lecture 3
18
Chromatic Dispersion The speed of light is dependent on the refractive index c = c0/ n where c0 is the speed of light in a vacuum The index of refraction, n, varies with the light transmission wavelength All light sources (LEDs and LDs) have some coloration, or variation, in wavelength output The low wavelength portion of the pulse travels slower than the high wavelength one – creating pulse spreading Lecture 3
19
Chromatic Dispersion (continued)
Chromatic dispersion is measured in units of time divided by distance and Tx source spectral width (ps/nm-km) It is zero near 1310 nm in silica optical fibers It is zero near 1550 nm in Dispersion Shifted optical fibers Even at the dispersion zero, there is some pulse spreading due to the spectral width of the light source Lecture 3
20
Pulse Spreading due to Dispersion
Lecture 3
21
Pulse Spreading T Pulse from zero-order mode T T
Pulses from other modes T Pulse from highest-order mode T Resulting pulse time Lecture 3
22
Calculation of Pulse Spread
y/2 y/2 C C x Lecture 3
23
Dispersion Management: Problem Chromatic Dispersion (CD)
Bit 1 Bit 2 Bit 1 Bit 2 Bit 1 Bit 2 Bit 1 Bit 2 Bit 1 Bit 2 The optical pulse tend to spread as it propagates down the fiber generating Inter-Symbol-Interference (ISI) and therefore limiting either the bit rate or the maximum achievable distance at a specific bit rate Physics behind the effect The refractive index has a wavelength dependent factor, so the different frequency-components of the optical pulses are traveling at different speeds Lecture 3 basica di prova - autore Andreoli 1
24
Pulse Spreading due to Dispersion
z=0 z=L Dispersion Lecture 3
25
Dispersion Curves Lecture 3
26
Dispersion Management: Problem Fiber Dispersion Characteristic
Normal Single Mode Fiber (SMF) >95% of Deployed Plant 17 Dispersion Shifted Fiber (DSF) Dispersion Coefficient ps/nm-km l 1310 nm 1550nm Lecture 3
27
Dispersion Management: Problem Increasing the Bit Rate
Higher Bit Rates experience higher signal degradation due to Chromatic Dispersion: Time Slot OA 2.5Gb/s Dispersion 1) OA 10Gb/s Dispersion 16 Times Greater Dispersion Scales as (Bit Rate)2 Lecture 3
28
Dispersion Management: Solution Direct vs. External Modulation
Direct Modulation External Modulation Electrical Signal in Iin DC Iin Electrical Signal in Unmodulated Optical Signal Mod. Optical Signal Optical Signal out External Modulator Laser diode’s bias current is modulated with signal input to produce modulated optical output Approach is straightforward and low cost, but is susceptible to chirp (spectral broadening) thus exposing the signal to higher dispersion The laser diode’s bias current is stable Approach yields low chirp and better dispersion performance, but it is a more expensive approach Lecture 3
29
Dispersion Management: Limitation Chromatic Dispersion
CD places a limit on the maximum distance a signal can be transmitted without electrical regeneration: For directly modulated (high chirp laser) LD = 1/ B D (1) D dispersion coefficient (ps/km-nm): source line width or optical bandwidth (nm): 0.5nm B bit rate (1/T where T is the bit period): 2.5Gb/s LD ~ 47 km (*) For externally modulated (very low chirp laser f ~ 1.2B ) LD ~ Gb/s (*) LD ~ 61 10Gb/s (*) @1.55μm and 17ps/nm*km Lecture 3
30
Dispersive properties
Anomalous dispersion: b2 < 0 or D > 0 — short wavelength components (blue) travel faster than long wavelength components (red) Normal dispersion: b2 > 0 or D < 0 — long wavelength components (red) travel faster than short wavelength components (blue) Lecture 3
31
Dispersion Management: Solution Dispersion Compensation
Note: f = c/ Lecture 3
32
Chromatic Dispersion in Optical Fiber
A high-speed pulse contains a spectrum of l components Lecture 3
33
Explaining Material Dispersion
Lecture 3
34
Chromatic Dispersion Definitions
Lecture 3
35
Dispersion Management: Solution Dispersion Compensation (Cont.)
Dispersion Compensating Fiber: By joining fibers with CD of opposite signs and suitable lengths an average dispersion close to zero can be obtained; the compensating fiber can be several kilometers and the reel can be inserted at any point in the link, at the receiver or at the transmitter Note: Although the Total Dispersion Is Close to Zero, This Technique Can Also Be Employed to Manage FWM and CPM Since at Every Point We Have Dispersion Which Translates in Decoupling the Different Channels Limiting the Mutual Interaction Lecture 3
36
Why Require Dispersion Compensation ?
Lecture 3
37
Dispersion Compensating Fiber (DCF) Application
Lecture 3
38
Thanks Lecture 3
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.