Download
15 441 computer networking n.
Skip this Video
Loading SlideShow in 5 Seconds..
15-441 Computer Networking PowerPoint Presentation
Download Presentation
15-441 Computer Networking

15-441 Computer Networking

410 Vues Download Presentation
Télécharger la présentation

15-441 Computer Networking

- - - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - - -
Presentation Transcript

  1. 15-441 Computer Networking Lecture 2 – Physical Layer

  2. Network Protocols • Protocol • A set of rules and formats that govern the communication between communicating peers • Protocol layering • Decompose a complex problem into smaller manageable pieces (e.g., Web server) • Abstraction of implementation details • Reuse functionality • Ease maintenance • Cons? Lecture 2: Physical Layer

  3. Application: supporting network applications FTP, SMTP, HTTP Transport: host-host data transfer TCP, UDP Network: routing of datagrams from source to destination IP, routing protocols Link: data transfer between neighboring network elements WiFi, Ethernet Physical: bits “on the wire” Radios, coaxial cable, optical fibers application transport network link physical Network Protocol Stack Lecture 2: Physical Layer

  4. Analog Signal “Digital” Signal 0 0 1 0 1 1 1 0 0 0 1 Bit Stream Packet Transmission 0100010101011100101010101011101110000001111010101110101010101101011010111001 Packets Sender Receiver Header/Body Header/Body Header/Body From Signals to Packets Lecture 2: Physical Layer

  5. Outline • RF introduction • Modulation • Antennas and signal propagation • Equalization, diversity, channel coding • Multiple access techniques • Wireless systems and standards Lecture 2: Physical Layer

  6. Outline • RF introduction • What is “RF” • Digital versus analog contents • Modulation • Antennas and signal propagation • Equalization, diversity, channel coding • Multiple access techniques • Wireless systems and standards Lecture 2: Physical Layer

  7. RF Introduction • RF = Radio Frequency. • Electromagnetic signal that propagates through “ether” • Ranges 3 KHz .. 300 GHz • Or 10 km .. 0.1 cm (wavelength) • Has been used for communication for a long time, but improvements in technology have made it possible to use higher frequencies. Lecture 2: Physical Layer

  8. Wireless Communication • 300 GHz is huge amount of spectrum! • Spectrum can also be reused in space • Not quite that easy: • Most of it is hard or expensive to use! • Noise and interference limits efficiency • Most of the spectrum is allocated by FCC • FCC controls who can use the spectrum and how it can be used. • Need a license for most of the spectrum • Limits on power, placement of transmitters, coding, .. • Need rules to optimize benefit: guarantee emergency services, simplify communication, return on capital investment, … Lecture 2: Physical Layer

  9. Spectrum Allocation See: http://www.ntia.doc.gov/osmhome/allochrt.html Most bands are allocated. • Industrial, Scientific, and Medical (ISM) bands are “unlicensed”. • But still subject to various constraints on the operator, e.g. 1 W output • 433-868 MHz (Europe) • 902-928 MHz (US) • 2.4000-2.4835 GHz • Unlicensed National Information Infrastructure (UNII) band is 5.725-5.875 GHz Lecture 2: Physical Layer

  10. What Is an Electromagnetic Signal • We will be vague about this and we will use two “cartoon” views: • Think of it as energy that radiates from an antenna and is picked up by another antenna. • Can easily explain properties such as attenuation • Can also view it as a “wave” that propagates between two points. • Can easily explain properties Space and Time Lecture 2: Physical Layer

  11. Decibels • A ratio between signal powers is expressed in decibels decibels (db) = 10log10(P1 / P2) • Is used in many contexts: • The loss of a wireless channel • The gain of an amplifier • Note that dB is a relative value. • Can be made absolute by picking a reference point. • Decibel-Watt – power relative to 1W • Decibel-milliwatt – power relative to 1 milliwatt • 4.5 mW = (10*log10 4.5) dBm Lecture 2: Physical Layer

  12. Analog and Digital Information • Initial RF use was for analog information. • Radio and TV stations • The information that is sent is of a continuous nature • In digital transmission, the signal consists of discrete units (e.g. bits). • Data networks, cell phones • Focus of this course • We can also send analog information as digital data. • Sample the signal, i.e. analog  digital  analog • E.g., Cell phones, … • Also digital  analog  digital (e.g. modem) Lecture 2: Physical Layer

  13. Outline • RF introduction • Modulation • Baseband versus carrier modulation • Forms of modulation • Channel capacity • Antennas and signal propagation • Equalization, diversity, channel coding • Multiple access techniques • Wireless systems and standards Lecture 2: Physical Layer

  14. The Frequency Domain • A (periodic) signal can be viewed as a sum of sine waves of different strengths. • Corresponds to energy at a certain frequency • Every signal has an equivalent representation in the frequency domain. • What frequencies are present and what is their strength (energy) • Again: Similar to radio and TV signals. Amplitude Time Frequency Lecture 2: Physical Layer

  15. Signal = Sum of Sine Waves = + 1.3 X + 0.56 X + 1.15 X Lecture 2: Physical Layer

  16. Modulation • Sender changes the nature of the signal in a way that the receiver can recognize. • Assume a continuous information signal for now • Amplitude modulation (AM): change the strength of the carrier according to the information. • High values  stronger signal • Frequency (FM) and phase modulation (PM): change the frequency or phase of the signal. • Frequency or Phase shift keying • Digital versions are sometimes called “shift keying”. • Amplitude (ASK), Frequency (FSK) and Phase (PSK) Shift Keying Lecture 2: Physical Layer

  17. Amplitude and FrequencyModulation 0 0 1 1 0 0 1 1 0 0 0 1 1 1 0 0 0 1 1 0 0 0 1 1 1 0 0 1 1 0 1 1 0 0 0 1 Lecture 2: Physical Layer

  18. Baseband versus Carrier Modulation • Baseband modulation: send the “bare” signal. • Use the lower part of the spectrum • Everybody competes – not attractive for wireless • Carrier modulation: use the (information) signal to modulate a higher frequency (carrier) signal. • Can be viewed as the product of the two signals • Corresponds to a shift in the frequency domain Lecture 2: Physical Layer

  19. Amplitude Carrier Modulation Signal Carrier Frequency Modulated Carrier Lecture 2: Physical Layer

  20. Frequency Division Multiplexing:Multiple Channels Determines Bandwidth of Link Amplitude Determines Bandwidth of Channel Different Carrier Frequencies Lecture 2: Physical Layer

  21. The more frequencies are present in a signal, the more detail can be represented in the signal. The signal can look “cleaner” Energy is distributed over a larger part of the spectrum, i.e. it consumes more (spectrum) bandwidth Signals with more detail can represent more bits, so in general, higher (spectrum) bandwidth translates into a higher (information) bandwidth. Signal Bandwidth Considerations Lecture 2: Physical Layer

  22. Every medium supports transmission in a certain frequency range. Outside this range, effects such as attenuation, .. degrade the signal too much Transmission and receive hardware will try to maximize the useful bandwidth in this frequency band. Tradeoffs between cost, distance, bit rate As technology improves, these parameters change, even for the same wire. Thanks to our EE friends Transmission Channel Considerations Good Bad Frequency Signal Lecture 2: Physical Layer

  23. The Nyquist Limit • A noiseless channel of width H can at most transmit a binary signal at a rate 2 x H. • E.g. a 3000 Hz channel can transmit data at a rate of at most 6000 bits/second • Assumes binary amplitude encoding Lecture 2: Physical Layer

  24. More aggressive encoding can increase the channel bandwidth. Example: modems Same frequency - number of symbols per second Symbols have more possible values Past the Nyquist Limit psk Psk+ AM Lecture 2: Physical Layer

  25. Capacity of a Noisy Channel • Can’t add infinite symbols - you have to be able to tell them apart. This is where noise comes in. • Shannon’s theorem: • C = B x log(1 + S/N) • C: maximum capacity (bps) • B: channel bandwidth (Hz) • S/N: signal to noise ratio of the channel • Often expressed in decibels (db). 10 log(S/N). • Example: • Local loop bandwidth: 3200 Hz • Typical S/N: 1000 (30db) • What is the upper limit on capacity? • Modems: Teleco internally converts to 56kbit/s digital signal, which sets a limit on B and the S/N. Lecture 2: Physical Layer

  26. Example: Modem Rates Lecture 2: Physical Layer

  27. Some Examples • Differential quadrature phase shift keying • Four different phases representing a pair of bits • Used in 802.11b networks • Quadrature Amplitude Modulation • Combines amplitude and phase modulation • Uses two amplitudes and 4 phases to represent the value of a 3 bit sequence Lecture 2: Physical Layer

  28. Modulation vs. BER • More symbols = • Higher data rate: More information per baud • Higher bit error rate: Harder to distinguish symbols • Why useful? • 802.11b uses DBPSK (differential binary phase shift keying) for 1Mbps, and DQPSK (quadriture) for 2, 5.5, and 11. • 802.11a uses four schemes - BPSK, PSK, 16-QAM, and 64-AM, as its rates go higher. • Effect: If your BER / packet loss rate is too high, drop down the speed: more noise resistance. • We’ll see in some papers later in the semester that this means noise resistance isn’t always linear with speed. Lecture 2: Physical Layer

  29. Outline • RF introduction • Modulation • Antennas and signal propagation • How do antennas work • Propagation properties of RF signals • Equalization, diversity, channel coding • Multiple access techniques • Wireless systems and standards Lecture 2: Physical Layer

  30. What is an Antenna? • Conductor that carries an electrical signal and radiates an RF signal. • The RF signal “is a copy of” the electrical signal in the conductor • Also the inverse process: RF signals are “captured” by the antenna and create an electrical signal in the conductor. • This signal can be interpreted (i.e. decoded) • Efficiency of the antenna depends on its size, relative to the wavelength of the signal. • E.g. half a wavelength Lecture 2: Physical Layer

  31. Types of Antennas • Abstract view: antenna is a point source that radiates with the same power level in all directions – omni-directional or isotropic. • Not common – shape of the conductor tends to create a specific radiation pattern • Note that isotropic antennas are not very efficient!! • Unless you have a very large number of receivers • Shaped antennas can be used to direct the energy in a certain direction. • Well-known case: a parabolic antenna • Pringles boxes are cheaper Lecture 2: Physical Layer

  32. Antennas and Attenuation • Isotropic Radiator: A theoretical antenna • Perfectly spherical radiation. • Used for reference and FCC regulations. • Dipole antenna (vertical wire) • Radiation pattern like a doughnut • Parabolic antenna • Radiation pattern like a long balloon • Yagi antenna (common in 802.11) • Looks like |--|--|--|--|--|--| • Directional, pretty much like a parabolic reflector Lecture 2: Physical Layer

  33. Multi-element antennas have multiple, independently controlled conductors. Signal is the sum of the individual signals transmitted (or received) by each element Can electronically direct the RF signal by sending different versions of the signal to each element. For example, change the phase in two-element array. Covers a lot of different types of antennas. Number of elements, relative position of the elements, control over the signals, … Multi-element Antennas Lecture 2: Physical Layer

  34. Directional Antenna Properties • dBi: antenna gain in dB relative to an isotropic antenna with the same power. • Example: an 8 dBi Yagi antenna has a gain of a factor of 6.3 (8 db = 10 log 6.3) Lecture 2: Physical Layer

  35. Antennas • Spatial reuse: • Directional antennas allow more communication in same 3D space • Gain: • Focus RF energy in a certain direction • Works for both transmission and reception • Frequency specific • Frequency range dependant on length / design of antenna, relative to wavelength. • FCC bit: Effective Isotropic Radiated Power. (EIRP). • Favors directionality. E.g., you can use an 8dB gain antenna b/c of spatial characteristics, but not always an 8dB amplifier. Lecture 2: Physical Layer

  36. Propagation Modes • Line-of-sight (LOS) propagation. • Most common form of propagation • Happens above ~ 30 MHz • Subject to many forms of degradation (next set of slides) • Ground-wave propagation. • More or less follows the contour of the earth • For frequencies up to about 2 MHz, e.g. AM radio • Sky wave propagation. • Signal “bounces” off the ionosphere back to earth – can go multiple hops • Used for amateur radio and international broadcasts Lecture 2: Physical Layer

  37. Limits to Speed and Distance • Noise: “random” energy is added to the signal • Attenuation: some of the energy in the signal leaks away • Dispersion: attenuation and propagation speed are frequency dependent. • Changes the shape of the signal Lecture 2: Physical Layer

  38. Propagation Degrades RF Signals • Attenuation in free space: signal gets weaker as it travels over longer distances. • Radio signal spreads out – free space loss • Absorption • Obstacles can weaken signal through absorption or reflection. • Part of the signal is redirected • Multi-path effects: multiple copies of the signal interfere with each other. • Similar to an unplanned directional antenna • Mobility: moving receiver causes another form of self interference. • Receiver moves ½ wavelength -> big change in wavelength Lecture 2: Physical Layer

  39. Refraction • Speed of EM signals depends on the density of the material. • Vacuum: 3 x 108 m/sec • Denser: slower • Density is captured by refractive index. • Explains “bending” of signals in some environments. • E.g. sky wave propagation • But also local, small scale differences in the air denser Lecture 2: Physical Layer

  40. Free Space Loss Loss = Pt / Pr = (4p d)2 / (Gr Gtl2) • Loss increases quickly with distance (d2). • Need to consider the gain of the antennas at transmitter and receiver. • Loss depends on frequency: higher loss with higher frequency. • But careful: antenna gain depends on frequency too • For fixed antenna area, loss decreases with frequency • Can cause distortion of signal for wide-band signals Lecture 2: Physical Layer

  41. Fairly • Predictable • Can be planned for or avoided Other LOS Factors • There are many noise sources. • Thermal noise: caused by agitation of the electrons • Intermodulation noise: result of mixing signals; appears at f1 + f2 and f1 – f2 • Cross talk: picking up other signals (i.e. from other source-destination pairs) • Impulse noise: irregular pulses of high amplitude and short duration – harder to deal with • Absorption of energy in the atmosphere. • Very serious at specific frequencies, e.g. water vapor (22 GHz) and oxygen (60 GHz) • Obviously objects also absorb Lecture 2: Physical Layer

  42. Propagation Mechanisms • Besides line of sight, signal can reach receiver in three other “indirect” ways. • Reflection: signal is reflected from a large object. • Diffraction: signal is scattered by the edge of a large object – “bends”. • Scattering: signal is scattered by an object that is small relative to the wavelength. Lecture 2: Physical Layer

  43. Multipath Effects • Receiver receives multiple copies of the signal, each following a different path • Copies can either strengthen or weaken each other. • Depends on whether they are in our out of phase • Small changes in location can result in big changes in signal strength. • Short wavelengths, e.g. 2.4 GHz  12 cm • Difference in path length can cause inter-symbol interference (ISI). Lecture 2: Physical Layer

  44. Example Lecture 2: Physical Layer

  45. Fading in the Mobile Environment • Fading: time variation of the received signal strength caused by changes in the transmission medium or paths. • Rain, moving objects, moving sender/receiver, … • Fast versus slow fading. • Fast: changes in distance of about half a wavelength – result in big fluctuations in the instantaneous power • Slow: changes in larger distances affects the paths – result in a change in the average power levels around which the fast fading takes place • Selective versus non-selective (flat) fading. • Does the fading affect all frequency components equally • Region of interest is the spectrum used by the channel Lecture 2: Physical Layer

  46. Fading - Example • Frequency of 910 MHz or wavelength of about 33 cm Lecture 2: Physical Layer

  47. Fading Channel Models • Statistical distribution that captures the properties of classes of fading channels. • Raleigh distribution: multiple indirect paths but no dominating, direct LOS path. • E.g. urban environment with large cells, in buildings • Ricean distribution: LOS path plus indirect paths. • Open space or small cells Lecture 2: Physical Layer

  48. Wireless Technologies • Great technology: no wires to install, convenient mobility, .. • High attenuation limits distances. • Wave propagates out as a sphere • Signal strength reduces quickly (1/distance)3 • High noise due to interference from other transmitters. • Use MAC and other rules to limit interference • Aggressive encoding techniques to make signal less sensitive to noise • Other effects: multipath fading, security, .. • Ether has limited bandwidth. • Try to maximize its use • Government oversight to control use Lecture 2: Physical Layer

  49. Next Lecture • RF introduction • Modulation • Antennas and signal propagation • Equalization, diversity, channel coding • Multiple access techniques • Wireless systems and standards Lecture 2: Physical Layer