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2.1.1 The basic satellite link Figure 2.1 shows, in its simplest form, a satellite link carrying a duplex (two-way) communication circuit: the earth station A transmits to the satellite an uplink (U/L) carrier wave (modulated by the baseband signal, i.e. by the signal from the message source transmitted by the user terminal) at radio frequency (RF) Fu1 (e.g. 5 980 MHz). The satellite antenna and transponder system receives this carrier and, after frequency conversion from Fu1 to Fd1 (e.g. 5 980 MHz 2 225 MHz = 3 755 MHz), amplifies and re-radiates it as a downlink (D/L) wave which is received by the earth station B. To establish the return link, B transmits a U/L carrier at another RF Fu2 (e.g. 6 020 MHz) which is received by A at the converted D/L RF Fd2 (e.g. 6 020 MHz 2 225 MHz = 3 795 MHz).

Fiber optics can be either multimode when more than one propagation mode is possible or single-mode when only one mode propagates in the fiber The former type of fiber is characterized by modal dispersion and low installation cost The latter does not present modal dispersion and is more expensive to install than the former, due to the accurate signal coupling required between fibers, transmitters and receivers Typically, three spectral regions, referred to as windows, are defined that have low signal attenuation in the fiber The first window is in the 800 900-nm interval range optical frequencies are conventionally characterized in terms of wavelengths and it is generally used to transmit multimode signals The second and third windows are, respectively, in the 1240 1340-nm and 1500 1650-nm regions, and are typically used to transmit single-mode signals.

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The bandwidth potentially available in each window is about 20 THz, but the actual bandwidth available for data transmission is considerably less and limited by a number of factors Among these factors, one can enumerate the limited bandwidth of other optical components, such as transmitters, receivers, and optical amplifiers, and the limited electronic processing speed at the network nodes, the so-called electronic bottleneck of the first-generation optical networks An optical signal is generated by either a light-emitting diode (LED) or a laser diode (laser) The main difference between LEDs and lasers is the spectral density of the emitted light beam The LED signal has a large spectrum and is used in conjunction with multimode fiber LEDs are relatively inexpensive and used in networks with low data rates (eg, FDDI), short distances, and limited power budget (eg.

And the total of the three elements checks at $978,224.54. Subject to exceptions involving just one or two changes in the series of payments, the solution will be to set up a cash flow schedule. This will be covered after the next chapter because we first have to outline the basic tools of NPV and IRR.

, LANs, fiber to the home, fiber to the curb, coarse WDM (CWDM), access networks) Instead, the laser emits a light beam with power concentrated in a narrow bandwidth Its cost grows with its selectivity in bandwidth Lasers are currently expensive and used in conjunction with single-mode fiber to deploy DWDM systems, in which the wavelength or channel density is high Lasers can be designed either to operate at one fixed wavelength or to be tunable In the latter case there is a trade-off between the laser tuning speed and its tuning range, ie, fast tunable lasers have a small tuning range and vice versa At the receiver node, photodetectors are used to convert the optical signal back into the electronic domain.

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When the received optical signal is weak, avalanche photodiodes (APDs) can be used, in which the reception of a photon generates an avalanche of photons that are easier to detect Optical amplifiers became commercially available in the early 1990s to regenerate the optical signal without requiring the two phase O-E-O conversion plus electrical signal amplification that was previously utilized Without any doubt optical amplifiers constitute one of the most important milestones in the history of optical communications By avoiding O-E-O conversion, an optical signal can be regenerated directly in the optical domain, thus circumventing the limited bandwidth of electronic circuitry For example, a single.

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