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Information and Communications University School of Engineering NAME: MWAPE MWANGO STUDENT IDENTIFICATION NUMBER (SIN): 1406147126 PROGRAMME: B.Ed. IN INFORMATION AND COMMUNICATIONS TECHNOLOGY COURSE NAME: OPTIC FIBER TECHNOLOGY ASSIGNMENT No. : 1 LECTURER: Mr N. PHIRI Question 1. Process and analyze information from secondary sources to compare and contrast copper cables with fiber optic cables in relation to; Carrying capacity Multimode optical fiber, whether or not it is also carrying laser power, can readily transmit high bandwidth data over moderate distances; a typical bandwidth-distance product for multimode fiber is 500 MHz/km, so a 500 m tether can transmit 1 GHz (several Gbits/second, with appropriate modulation). Signal losses over 500 m are negligible; the bandwidth is limited by dispersion (time-smearing) of signals. Lightweight copper cable, by contrast, has very high losses at high frequencies. Twisted pair optimized for high data rates (Cat 6) can transmit 500 MHz over only 100 meters (bandwidth-distance product of 50 MHz/km); lightweight unshielded cable optimized for power transmission will have even lower bandwidth-distance product. Cost The raw materials for glass are plentiful, unlike copper. This means that glass can be made more cheaply than copper. Transmission over copper or aluminum wire is, and will likely remain, cheaper than transmission over fiber. The dominant cost of the fiber is the fiber itself, which is not present in the electrical system. However, the cost of the laser power system is already comparable to or less than the cost of the rest of a surveillance or communications platform, and will decline significantly with quantity purchases. Rate of information transfer Fiber optic cables have a much greater bandwidth than metal cables. The amount of information that can be transmitted per unit time over other transmission media is its most significant advantage. An optic fiber offers low power loss. This allows for longer transmission distances. In comparison to copper cables, in a network, the longest recommended copper distance is 100m while with fiber it is 2000m. Security The fiber is nonconducting, and is therefore safe in all electromagnetic environments. On land, this means it can safely be used around electrical transmission lines, as well as in high RF and magnetic fields. Also, it will not attract or transmit lightning. Copper cables tend to require very high voltages (hundreds to thousands of volts) to transmit power efficiently over very thin conductors, which is both a safety hazard and a reliability and maintenance issue. Optical fiber cables are difficult to tap. As they do not radiate electromagnetic energy, emissions cannot be intercepted. As physically tapping the fiber takes great skill to do undetected, fiber is the most secure medium available for carrying sensitive data. A broken or damaged, optical fiber can be detected extremely quickly by monitoring either the actual transmission or (preferably) the transmission of a pilot signal at a shorter wavelength. With a suitable crowbar circuit, the laser transmission can be shut off within 1-2 microseconds. Question 2. Fusion splicing is the act of joining two optical fibers end-to-end using heat. The goal is to fuse the two fibers together in such a way that light passing through the fibers is not scattered or reflected back by the splice, and so that the splice and the region surrounding it are almost as strong as the virgin fiber itself. The source of heat is usually an electric arc, but can also be a laser, or a gas flame, or tungsten filament through which current is passed. The process of fusion splicing normally involves using localized heat to melt or fuse the ends of two optical fibers together. The splicing process begins by preparing both fiber ends for a fusion, which requires that all protective coating is removed from the ends of each fiber. Question 3. Attenuation/ Km (dB/Km) Attenuation/optical connector (dB) Attenuation/joint (dB) Mini Average Maximum 0.17 0.22 0.4 0.2 0.35 0.7 0.01 0.05 0.1 Best Conditions Normal Worst situation Estimating the Attenuation on the Optical Link We can arrive at the total attenuation (TA) of an elementary cable section by: TA = n x C + c x J + L x a + M Where: n_number of connectors C_attenuation for one optical connector (dB) c_number of splices in elementary cable section J_attenuation for one splice (dB) M_system margin (patch cords, cable bend, unpredictable optical attenuation events, and so on, should be considered around 3dB) a_attenuation for optical cable (dB/Km) L_total length of the optical cable 1. Best Conditions TA = n x C + c x J + L x a + M=2 x 0.2dB+4x0.01dB+20.5Kmx0.17/Km+3dB=6.49dB 2. Normal TA = n x C + c x J + L x a + M = 2 x 0.35dB+ 4x 0.05dB+ 20.5Km x 0.22dB/Km+ 3dB = 8.41dB 3. Worst situation TA = n x C + c x J + L x a + M=2 x 0.7dB+4 x 0.1dB+20.5Km x 0.4dB/Km+3dB = 11.42dB