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Lectures07 By Engr. Muhammad Ashraf Bhutta
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In Manufacturing fiber there are Two challenges
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Purifying Silica For good fiber the maximum tolerable level of impurity due the presence of transition metals like Fe,Cu,Mn etc is about 1 part 10 9 that is 1000 times better than traditional chemical purification About 1 part in 10 8 but this is also very hard to achieve
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Form this process is difficult because of high temperatures involved
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Drawing The Fiber
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From a reservoir
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Drawing Tower This tower is About 20feet high to allow The fiber to cool down before being spooled
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Vapour deposition Techniques
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Problems of this process
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Vapour Phase Axial Deposition
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MCVD
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With G IMM fiber It can be significant problem
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Mid-1960s: Attenuation in bulk glass was ∼ Attempted guiding structures included surface-wave devices ◦Metallic tubes and hollow dielectric tubes Kao and Hockham pointed out what had to be done to reduce attenuation Reduce concentration of transition-metal ions (Fe, Cu, Cr, Ni, Mn, Co) to less than 1 part per billion Increase purity of SiO2 to make attenuation mostly scattering loss In 1971 Kapron et al. at Corning made a fiber with α ≈ BRIEF HISTORY OF OPTICAL FIBER TECHNOLOGY
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◦ Dispersion produces pulse broadening and limits bit rate Unclad fiber was widely used for imaging and short- distance transmission ◦Very rapid pulse broadening not suitable for communications
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OVERVIEW OF OPTICAL FIBER MANUFACTURING An optical fiber is drawn from a preform Dimensions are 1 meter in length by 2 cm in diameter Refractive-index profile is the same (relative to the outside diameter) as in the finished fiber The core is doped with GeO2 or P2O5 to increase the refractive index B2O3 and F can be used in the cladding to decrease the refractive index
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In the vapor-deposition methods, SiO2 is obtained by reacting SiCl4 with O2 to produce a porous “soot” of silica: SiCl4 + 2O2 →SiO2 + 2Cl2
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DRAWING AN OPTICAL FIBER
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OVERVIEW OF OPTICAL FIBER MANUFACTURING (2) Methods for fabricating a preform Modified chemical vapor deposition (MCVD) ◦The cladding and core are deposited on the inside of a fused silica tube The refractive-index profile is controlled by adding various dopants as deposition progresses At the end, the tube is heated and collapses into a solid rod Outside vapor deposition (OVD) The layers of the preform are deposited on the outside of a rotating mandrel using flame hydrolysis(Al 2 O 3 or graphite rod is rotated ) The mandrel’s thermal expansion coefficient is larger than that of the preform, so the mandrel drops out after cooling ◦
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Vapor axial deposition (VAD) Deposition occurs on the end of a rotating rod
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MCVD PROCESS FOR FABRICATING A PREFORM
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OVERVIEW OF OPTICAL FIBER MANUFACTURING (3) Coating Deposited immediately after the fiber is pulled Purposes: ◦Protection from abrasion Surface flaws cause cracks to form Protection from H2O Exposure to H2O would promote growth of crystallites fracture Identification
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Cable Jacket contains one to many fiber bundles, each inside a buffer tube Purposes: Mechanical strength ◦Protection from H2O and other environmental chemicals
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DISPERSION IN OPTICAL COMMUNICATION SYSTEMS Dispersion is the property that the velocity of light depends on the optical frequency or the mode of propagation in a wave guide Dispersion causes the duration and shape of an optical pulse to change in the course of propagation, causing bit errors in reception Causes of dispersion: Frequency dependence of the refractive index (material dispersion) Frequency dependence of the propagation constant in a fiber mode (wave guide dispersion) Dispersion in optical fibers: Different fiber modes have different propagation constants at the same frequency, making pulses launched simultaneously in different modes arrive at the receiver at different times (intermodal dispersion)
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A single pulse in a single fiber mode contains a range of frequencies, each of which propagates at a different velocity (group-velocity dispersion)
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INTERMODAL DISPERSION (1) Different modes of propagation in a waveguide correspond to different E and H field patterns For a fiber with a sufficiently small core radius, there is only one propagating mode Different modes propagate at different speeds because some modes take a longer path through a fiber than others Also called multipath dispersion The differential mode delay for step-index fiber is the difference in arrival times of two pulses launched into different modes
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is the propagation velocity of a monochromatic wave in the core of the fiber Differential mode delay is important for LAN technologies
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INTERMODAL DISPERSION (2)
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INTERMODAL DISPERSION (3)
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INTERMODAL DISPERSION (4)
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INTERMODAL DISPERSION (5)
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GROUP-VELOCITY DISPERSION
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