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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Physical Layer PART II

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Position of the physical layer

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Services

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Chapters Chapter 3 Signals Chapter 4 Digital Transmission Chapter 5 Analog Transmission Chapter 6 Multiplexing Chapter 7 Transmission Media Chapter 8 Circuit Switching and Telephone Network Chapter 9 High Speed Digital Access

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Chapter 3 Signals

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 To be transmitted, data must be transformed to electromagnetic signals. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 3.1 Analog and Digital Analog and Digital Data Analog and Digital Signals Periodic and Aperiodic Signals

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Signals can be analog or digital. Analog signals can have an infinite number of values in a range; digital signals can have only a limited number of values. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.1 Comparison of analog and digital signals

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 In data communication, we commonly use periodic analog signals and aperiodic digital signals. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 3.2 Analog Signals Sine Wave Phase Examples of Sine Waves Time and Frequency Domains Composite Signals Bandwidth

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.2 A sine wave

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.3 Amplitude

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Frequency and period are inverses of each other. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.4 Period and frequency

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Table 3.1 Units of periods and frequencies UnitEquivalentUnitEquivalent Seconds (s)1 shertz (Hz)1 Hz Milliseconds (ms)10 –3 skilohertz (KHz)10 3 Hz Microseconds (ms)10 –6 smegahertz (MHz)10 6 Hz Nanoseconds (ns)10 –9 sgigahertz (GHz)10 9 Hz Picoseconds (ps)10 –12 sterahertz (THz)10 12 Hz

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Frequency is the rate of change with respect to time. Change in a short span of time means high frequency. Change over a long span of time means low frequency. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 If a signal does not change at all, its frequency is zero. If a signal changes instantaneously, its frequency is infinite. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Phase describes the position of the waveform relative to time zero. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.5 Relationships between different phases

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.6 Sine wave examples

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.6 Sine wave examples (continued)

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.6 Sine wave examples (continued)

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 An analog signal is best represented in the frequency domain. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.7 Time and frequency domains

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.7 Time and frequency domains (continued)

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.7 Time and frequency domains (continued)

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 A single-frequency sine wave is not useful in data communications; we need to change one or more of its characteristics to make it useful. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 When we change one or more characteristics of a single-frequency signal, it becomes a composite signal made of many frequencies. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 According to Fourier analysis, any composite signal can be represented as a combination of simple sine waves with different frequencies, phases, and amplitudes. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.8 Square wave

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.9 Three harmonics

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.10 Adding first three harmonics

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.11 Frequency spectrum comparison

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.12 Signal corruption

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 The bandwidth is a property of a medium: It is the difference between the highest and the lowest frequencies that the medium can satisfactorily pass. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 In this book, we use the term bandwidth to refer to the property of a medium or the width of a single spectrum. Note:

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.13 Bandwidth

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 3 If a periodic signal is decomposed into five sine waves with frequencies of 100, 300, 500, 700, and 900 Hz, what is the bandwidth? Draw the spectrum, assuming all components have a maximum amplitude of 10 V. Solution B = f h f l = 900 100 = 800 Hz The spectrum has only five spikes, at 100, 300, 500, 700, and 900 (see Figure 13.4 )

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.14 Example 3

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 4 A signal has a bandwidth of 20 Hz. The highest frequency is 60 Hz. What is the lowest frequency? Draw the spectrum if the signal contains all integral frequencies of the same amplitude. Solution B = f h f l 20 = 60 f l f l = 60 20 = 40 Hz

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.15 Example 4

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 5 A signal has a spectrum with frequencies between 1000 and 2000 Hz (bandwidth of 1000 Hz). A medium can pass frequencies from 3000 to 4000 Hz (a bandwidth of 1000 Hz). Can this signal faithfully pass through this medium? Solution The answer is definitely no. Although the signal can have the same bandwidth (1000 Hz), the range does not overlap. The medium can only pass the frequencies between 3000 and 4000 Hz; the signal is totally lost.

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 3.5 Data Rate Limit Noiseless Channel: Nyquist Bit Rate Noisy Channel: Shannon Capacity Using Both Limits

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 7 Consider a noiseless channel with a bandwidth of 3000 Hz transmitting a signal with two signal levels. The maximum bit rate can be calculated as Bit Rate = 2 3000 log 2 2 = 6000 bps

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 8 Consider the same noiseless channel, transmitting a signal with four signal levels (for each level, we send two bits). The maximum bit rate can be calculated as: Bit Rate = 2 x 3000 x log 2 4 = 12,000 bps Bit Rate = 2 x 3000 x log 2 4 = 12,000 bps

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 9 Consider an extremely noisy channel in which the value of the signal-to-noise ratio is almost zero. In other words, the noise is so strong that the signal is faint. For this channel the capacity is calculated as C = B log 2 (1 + SNR) = B log 2 (1 + 0) = B log 2 (1) = B 0 = 0

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 10 We can calculate the theoretical highest bit rate of a regular telephone line. A telephone line normally has a bandwidth of 3000 Hz (300 Hz to 3300 Hz). The signal- to-noise ratio is usually 3162. For this channel the capacity is calculated as C = B log 2 (1 + SNR) = 3000 log 2 (1 + 3162) = 3000 log 2 (3163) C = 3000 11.62 = 34,860 bps

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Example 11 We have a channel with a 1 MHz bandwidth. The SNR for this channel is 63; what is the appropriate bit rate and signal level? Solution C = B log 2 (1 + SNR) = 10 6 log 2 (1 + 63) = 10 6 log 2 (64) = 6 Mbps Then we use the Nyquist formula to find the number of signal levels. 4 Mbps = 2 1 MHz log 2 L L = 4 First, we use the Shannon formula to find our upper limit.

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 3.6 Transmission Impairment Attenuation Distortion Noise

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.20 Impairment types

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.21 Attenuation

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.23 Distortion

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.24 Noise

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 3.7 More About Signals Throughput Propagation Speed Propagation Time Wavelength

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.25 Throughput

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McGraw-Hill©The McGraw-Hill Companies, Inc., 2004 Figure 3.26 Propagation time

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Chapter 3 Introduction To Physical Layer 1.# 1

Chapter 3 Introduction To Physical Layer 1.# 1

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