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1 Wire Propagation Effects Propagation Effects –Signal changes as it travels –If change is too great, receiver may not be able to recognize it Distance.

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Presentation on theme: "1 Wire Propagation Effects Propagation Effects –Signal changes as it travels –If change is too great, receiver may not be able to recognize it Distance."— Presentation transcript:

1 1 Wire Propagation Effects Propagation Effects –Signal changes as it travels –If change is too great, receiver may not be able to recognize it Distance Original Signal Final Signal

2 2 Wire Propagation Effects: Attenuation Attenuation: Signal Gets Weaker as it Propagates –May become too weak for receiver to recognize Signal Strength Distance

3 3 Wire Propagation Effects: Distortion Distortion: Signal changes shape as it propagates –Adjacent bits may overlap –May make recognition impossible for receiver Distance

4 4 Wire Propagation Effects: Noise Noise: Thermal Energy in Wire Adds to Signal –Noise floor is average noise energy –Random energy, so noise spikes sometimes occur Signal Strength Time Signal Noise Spike Noise Floor Error

5 5 Wire Propagation Effects Noise and Attenuation –As signal attenuates, gets closer to noise floor –So noise errors increase with distance, even if the average noise level is constant Signal Strength Distance Signal Noise Floor

6 6 Wire Propagation Effects: SNR Want a high Signal-to-Noise Ratio (SNR) –Signal strength divided by average noise strength –As SNR falls, errors increase Signal Strength Distance Signal Noise Floor SNR

7 7 Wire Propagation Effects: Noise & Speed Noise and Speed –As speed increases, each bit is briefer –Noise fluctuations do not average out as much –So noise errors increase as speed increases One Bit Noise Spike Average Noise During Bit Low Speed (Long Duration) One Bit Noise Spike Average Noise During Bit High Speed (Short Duration) OK Error

8 8 Wire Propagation Effects: Interference Interference –Energy from outside the wire (nearby motors, other wires, etc.) –Adds to signal, like noise –Often intermittent (comes and goes), so hard to diagnose Signal Strength Time Signal Interference

9 9 Wire Propagation Effects: Cross- Talk Interference Cross-Talk Interference –Often, multiple wires in a bundle –Each radiates some of its signal –Causes “cross-talk” interference in nearby wires

10 10 Wire Propagation Effects:Cross Talk Wire Usually is Twisted –Usually, several twists per inch –Interference adds to signal over half twist, subtracts over other half –Roughly cancels out –Simple but effective Single Twist Interference -+ Signal

11 11 Wire Propagation Effects:Cross Talk Terminal Cross-Talk Interference –Wire must be untwisted at ends to fit into connectors –So cross-talk interference is high at termination –Problems severe if untwist more than about 1.25 cm (1/2 inch) –Usually the biggest propagation effect Terminal Cross Talk

12 12 Practical Issues in Propagation Effects Distance limits in standards prevent serious propagation effects –For instance, usually 100 meters (328 feet) maximum for ordinary copper wire Problems usually occur at connectors –Crossed wires –Poor connections –Cross-talk interference

13 13 Wire Media: UTP to the Desktop UTP –Dominant for line from desktop to first switch –Inexpensive to buy and install –Rugged: can take punishment of office work –Easily 100 Mbps, 1 Gbps with careful insulation UTP First Hub or Switch

14 14 Categories of UTP Cat 1 - traditional telephone cabling designed for voice and not data (2 wire pairs RJ-11) Cat 2 - certified for transmissions of 4Mpbs (not used in networks where typical transmissions are >=10Mbps Cat 3 - certified for transmission up to 10Mbps –in 8 wire pair with RJ-45 –not recommended for new installations because transmission speeds are > 10 Mbps ~ 100 Mbps

15 15 Categories of UTP Cat 4 - certified for transmissions up to 16-20Mbps Cat 5 - certified for transmission up to 100 Mbps –typical cable in use today Enhanced Cat 5 - more twists transmission up to 200 Mbps Cat 6 - extra foil insulation –supports up to 600Mbps

16 16 Wire Media: Optical Fiber Limited by Distortion –Light entering at different angles travels different distances (different number of reflections) –Different ways of traveling are called modes –Light modes from successive bits will begin to overlap given enough distance, making the bits unreadable Light Source

17 17 Wire Media: Optical Fiber Multimode Fiber –Wide core makes easy to splice (50 or 62 microns) –Many angles for rays (modes) –Short propagation distance (usually 200 m to 500 m) Light Source Md B

18 18 Wire Media: Optical Fiber Single Mode Fiber –Narrow core difficult to splice (5 or 8 microns) –Only one angle for rays (one mode), so (almost) no distortion –Longer propagation distance (usually up to 2 km for LAN fiber, longer for long-distance fiber) –Narrow core makes fiber fragile and difficult to splice Mod B

19 19 Single Mode Fiber Single Mode Fiber is very thin –Only one mode will propagate even over fairly long distances –Expensive to produce –Expensive to install (fragile, precise alignments needed) –Used by carriers to link distant switches

20 20 Multimode Fiber Core is thick –Modes will appear even over fairly short distances –Must limit distances to a few hundred meters –Inexpensive to purchase and install –Dominates LANs

21 21 Graded Index Multimode Fiber Index of fraction is not constant in core –Varies from center to edge –Reduces time delays between different modes –Can go farther than if core has only a single index of fraction (step index multimode fiber) –Dominates multimode fiber today

22 22 Multimode Optical Fiber and Frequency Signal Frequency Determines the Propagation Distance before Mode Problems Become Serious Short Wavelength (high frequency) –Signals do not travel as far before mode problems occur –Uses the least expensive light sources –Good for LAN use within buildings Long Wavelength (low frequency) –Signals travel farther but light sources cost more –Within large buildings and between buildings

23 23 Wave Division Multiplexing Use multiple light sources of different frequencies –Place a separate signal on each –Increases the capacity of the optical fiber

24 24 Wire Media: Optical Fiber Optical Fiber –High speeds over long distances 200 m to 2 km –Costs more than UTP, but worth it on long runs –Good for all links between hubs and switches within and between buildings in a site network Optical Fiber

25 25 Wire Media: UTP and Optical Fiber The emerging pattern: UTP from first hub or switch to desk, Fiber everywhere else on site

26 26 Wire Media: Coax Coaxial Cable –Used in cable TV, VCRs –Central wire, external concentric cylinder –Outer conductor wrapped in PVC Screw-On Connector Inner Wire Outer Conductor Wrapped in PVC

27 27 Wire Media: Coaxial Cable Coaxial Cable –Installed widely today in old 10 Mbps Ethernet LANs ThinNet and ThickNet –Not being used in new installations Optical fiber more cost-effective for long links UTP more cost-effective for desktop links

28 28 Duplex Full-duplex transmission: both sides can transmit simultaneously –Even if only one sends, still full-duplex line –Even if neither is sending, still full-duplex line AB Time 1 Both can send Both do AB Time 1 Both can send Only A does AB Time 1 Both can send Neither does

29 29 Duplex Half-duplex transmission: only one can transmit at a time; must take turns –Still half duplex if neither transmits ABAB Time 1 Only one side Can send A does Time 2 Only one side Can send Neither does

30 30 Duplex Duplex is a Characteristic of the Transmission System, Not of Use at a Given Moment –In full duplex, both sides can transmit at once; in half duplex, only one side can transmit at a time –Still full duplex system if only one side or neither side actually is transmitting at a moment –Still half duplex if neither side actually is transmitting at a moment

31 31 Wireless Transmission Infrared -uses light beams to send signals between pairs of devices –Direct - transmitter and receiver are within line-of-sight of each other ex. Laptop and printer in same room –Indirect - signal bounces off walls, ceilings etc.

32 32 Radio Propagation Broadcast signal –Not confined to a wire

33 33 Radio Waves When Electron Oscillates, Gives Off Radio Waves –Single electron gives a very weak signal –Many electrons in an antenna are forced to oscillate in unison to give a practical signal

34 34 Radio Propagation Problems Radio Propagation is Difficult –Signals are reflected –May arrive at a destination via multiple paths –Signals arriving by different paths can interfere with one another –This is called multipath interference Nw

35 35 Radio Propagation Problems Wires Propagation is Predictable –Signals go through a fixed path: the wire –Propagation problems can be easily anticipated –Problems can be addressed easily Radio Propagation is Difficult –Signals begin propagating as a simple sphere –Inverse square law attenuation –If double distance, only ¼ signal strength –If triple distance only 1/9 signal strength

36 36 Radio Propagation: Waves Waves Amplitude (strength) Wavelength (meters) Frequency in hertz (Hz) Cycles per Second One Second 7 Cycles 1 Hz = 1 cycle per second

37 37 Radio Propagation: Frequency Spectrum Frequency Spectrum –Frequencies vary (like strings in a harp) –Frequencies measured in hertz (Hz) –Frequency spectrum: all possible frequencies from 0 Hz to infinity 0 Hz

38 38 Frequencies Metric system –kHz (1,000 Hz) kilohertz; note lower-case k –MHz (1,000 kHz) megahertz –GHz (1,000 MHz) gigahertz –THz (1,000 GHz) terahertz

39 39 Radio Propagation: Service Bands Service Bands –Divide spectrum into bands for services –A band is a contiguous range of frequencies –FM radio, cellular telephone service bands etc. 0 Hz Cellular Telephone FM Radio AM Radio Service Bands

40 40 Radio Propagation: Channels and Bandwidth Service Bands are Further Divided into Channels –Like television channels –Bandwidth of a channel is highest frequency minus lowest frequency 0 Hz Channel 3 Channel 2 Channel 1 Service Band

41 41 Radio Propagation: Service Bands Service Bands –Divide spectrum into bands for services –A band is a contiguous range of frequencies –FM radio, cellular telephone service bands etc. 0 Hz Cellular Telephone FM Radio AM Radio Service Bands

42 42 Radio Propagation: Channels and Bandwidth Example –Highest frequency of a radio channel is 43 kHz –Lowest frequency of the radio channel is 38 kHz –Bandwidth of radio channel is 5 kHz (43-38 kHz ) 0 Hz Channel 3 Channel 2 Channel 1 Service Band Channel Bandwidth

43 43 Radio Propagation: Channels and Bandwidth Shannon’s Equation –W is maximum possible (not actual) transmission speed in a channel –B is bandwidth of the channel: highest frequency minus lowest frequency –S/N is the signal-to-noise ratio W = B Log 2 (1 + S/N) D = 2 B Log2 K (Nyquist’s Theorem)

44 44 Radio Transmission: Broadband Speed and Bandwidth –The wider the channel bandwidth (B), the faster the maximum possible transmission speed (W) –W = B Log 2 (1+S/N) Maximum Possible Speed Bandwidth

45 45 Telephony is Narrowband Bandwidth in Telephone Channels is Narrow –Sounds below about 300 Hz cut off to reduce equipment hum within telephone system –Sounds above about 3,400 Hz cut off to reduce the bandwidth needed to send a telephone signal 20 kHz300 Hz 3.4 kHz 3.1 kHz

46 46 Telephony is Narrowband Bandwidth in Telephone Channels is Narrow –A radio channel would have to be from 0 to 3.4 kHz (3.4 kHz) –This would mean a maximum possible transmission speed of about 35 kbps 20 kHz300 Hz 3.4 kHz 3.1 kHz Required Radio Channel

47 47 Broadband Two Uses of the Term “Broadband” Technically, the signal is transmitted in a single channel AND the bandwidth of the channel is large –Therefore, maximum possible transmission speed is high Popularly, if the signal is fast, the system is called “broadband” whether it uses channels at all


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