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When DVD contains widescreen video and is played in a DVD player, the different output modes of the player can be combined with different widescreen TV display modes to create a confusing array of options. Figure 2.20 shows how the different DVD output modes look on a regular TV and on a widescreen TV. Note that there is one good way to view widescreen video on a standard TV (Figure 2.20e) but that a very large TV or a widescreen TV is required to do it justice. Also note that there is only one good way to view widescreen video on a widescreen TV, and this is with widescreen (anamorphic) output to wide mode (Figure 2.20o). Neither the Wide or the Expand modes should be used with Blu-ray players, as the player outputs a true widescreen picture. In cases where the disc contains standard definition 4:3 video (either 720 480 or 720 576) the player will center the image on the 16:9 display, or

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step-by-step back into the line signal for transmission. This makes plesiochronous multiplexing technology an expensive solution for telecommunications networking. When originally conceived, network management and maintenance practices in PDH high-capacity networks were based on manual signal crossconnection and outof-service testing techniques. There was no need to add extra capacity to the frame structures of the multiplexed signals for management and maintenance. As the complexity of the networks increased, however, and automatic computer management techniques became available, the lack of spare signal capacity in these signal frame structures severely limited the improvements that could be made. A further limitation of PDH high-capacity line systems was that there was no common standard. Individual manufacturers of network equipment had their own proprietary designs. Both ends of the line system therefore had to be purchased from the same manufacturer. There was no possibility of interworking among components supplied by different manufacturers. 13.3 The Synchronous Network The arrival of optical fiber as a transmission medium led to a rapid rise in achievable data rates and consequent available bandwidth within the telecommunications network. Coupled with the proliferation of automatic (microprocessor) control within the network, these developments opened the prospect of building extremely flexible and complex networks operating at high data rates. The limitations of PDH systems meant that it would have been very expensive, if not impossible, to take full advantage of these changes using the existing techniques. To answer this need, committees within ANSI and ITU-T in the mid-1980s started to define a new network standard. The objective was to produce a worldwide standard for synchronous transmission systems that would provide network operators with a flexible and economical network. In 1985 the ANSI-accredited T1X1 committee started work on the Synchronous Optical Network (SONET) standard for North America; in June of 1986, ITU-T s Study Group XVIII started work on the Synchronous Digital Hierarchy (SDH) standards. SDH is the recognized international standard. The two standards were first published in 1988 and are broadly similar, the major difference being the base data rate used for multiplexing (see section 13.6). Unless otherwise stated, the information in this chapter applies to both standards. A list of documents relevant to each standard can be found in section 13.13.1 near the end of the chapter. The synchronous standards that were defined have the following advantages over the previous PDH standards:

Use full vector values of S (Z 0 ) in calculations (for example, S11 0.35 45 ). We will have many instances when we have to convert from rectangular (Z R jX) to polar (Z R ) notation, and back, when designing amplifiers. The manual technique below good only for positive real numbers is one method. However, a simple scientific calculator performs the job much faster and more accurately. 1. To convert rectangular into polar form (R jX to Z a. Z R2 X 2 b. tan 1 X/R (Note: tan 1 arc tangent) 2. To convert polar into rectangular form (Z a. R Z (COS ) b. X Z (SIN ) ):

FIGURE 2.15. Comparison of basic curves DRD cam. (Follower has 11/2-in. rise in 150 degrees of cam rotation at 30 rpm.)

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6.6.2 Tunable filter design A half-octave range 50-ohm tunable bandpass filter (Fig. 6.56)

In summary, we determine the equation of a line in the plane by finding two expressions for the slope and equating them. If a line has slope m and passes through the point (x0 , y0 ) then it has equation y y0 = m(x x0 ). This is the point-slope form of a line.

The two issues to be addressed here are the following:

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