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To understand the SDH frame structure, it is first helpful to understand the relationship between SDH and SONET. Functionally, they are identical. In both cases, the intent of the technology is to provide a globally standardized transmission system for high-speed data. SONET is indeed optimized for the T-1-heavy North American market, whereas SDH is more applicable to Europe. Beyond that, however, the overhead and design considerations of the two are virtually identical. However, some key differences can be seen. Perhaps the greatest difference between the two lies in the physical nature of the frame. A SONET STS-1 frame comprises 810 total bytes for an overall aggregate bit rate of 51.84 Mbps, perfectly adequate for the North American 44.736-Mbps DS-3. An SDH STM-1 frame, however, designed to transport a 139.264-Mbps European E-4 or a CEPT-4 signal, must be larger if it is to accommodate that much bandwidth. It clearly won t fit in the limited space available in an STS-1. An STM-1, then, operates at a fundamental rate of 155.52 Mbps, enough for the bandwidth requirements of the E-4. This should be where the d j vu starts to kick in. Perceptive readers will remember that 155.52 Mbps number from our discussions of the SONET STS-3, which offers exactly the same bandwidth. An STM-1 frame is shown in Figure 3-67. It is a byte-interleaved, 9-row by 270-column frame, with the first 9 columns devoted to overhead and the remaining 261 devoted to payload transport. A comparison of the bandwidth between SONET and SDH systems is also interesting. The fundamental SDH signal is exactly three times the bandwidth of the fundamental SONET signal, and this relationship continues all the way up the hierarchy.

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If an ac circuit contains reactance, things get interesting. The rate of energy expenditure is the same as the VA power in a pure resistance. But when inductance and/or capacitance exists in an ac circuit, these two definitions of power part ways. The VA power becomes greater than the power actually manifested as heat, light, radio waves, or whatever. The extra power is called imaginary power, because it exists in the reactance, and reactance can be, as you have learned, rendered in mathematically imaginary numerical form. It is also known as reactive power. Inductors and capacitors store energy and then release it a fraction of a cycle later. This phenomenon, like true power, is expressible as the rate at which energy is changed from one form to another. But rather than any immediately usable form of power, such as radio or sound waves, imaginary power is stashed as a magnetic or electric field and then dumped back into the circuit, over and over again. You might think of the relationship between imaginary and true power in the same way as you think of potential versus kinetic energy. A brick held out of a seventh-story window has potential energy, just as a charged-up capacitor or inductor has imaginary power. Although the label imaginary power carries a connotation that it s not real or important, it s significant indeed. Imaginary power is responsible for many aspects of ac circuit behavior.

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1. 6. 11. 16. b b b d 2. 7. 12. 17. a c b c 3. 8. 13. 18. d c a a 4. 9. 14. 19. d a b b 5. 10. 15. 20. d c b a

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An important semantical point should be brought up concerning true power, not only in ac circuits, but in any kind of circuit or device. A common and usually harmless misconception about true power is that it travels. For example, if you connect a radio transmitter to a cable that runs outdoors to an

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