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ECE 4710: Lecture #36 1 Chapter 8 Chapter 8 : Wired and Wireless Communication Systems Telephone Fiber Optic DSL Satellite Digital & Analog TV Cellular Telephone Personal Communication Systems (PCS) Link Budget Analysis and System Design
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ECE 4710: Lecture #36 2 Link Budget Analysis BER baseband performance determined by received signal to noise ratio ( S/N ) How do we predict the received signal and noise power? Link Budget Analysis Predict received signal power at input to Rx »Depends on Tx output power, channel attenuation (path loss), antenna gains (wireless), etc. Predict received noise power at input to Rx »Depends on frequency, antenna field of view, temperature, etc. Predict signal + noise power at detector or MF input in Rx »Depends on Rx gain, noise characteristics, etc. »S/N (or E b /N o ) at detector or MF input determines BER of digital system
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ECE 4710: Lecture #36 3 Signal Power @ Rx Signal power at Rx input is a critical parameter in the design of any communication system For a given Tx power how do we predict the received signal power? Basic communication system (Tx + Channel + Rx) Receiver
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ECE 4710: Lecture #36 4 Signal Power @ Rx Free Space Transmission Channel Wireless Communication System Atmosphere (usually) or Outer Space Power gain of channel Gain? Book includes Tx and Rx antennas as part of channel »Not standard perspective but is OK All channels attenuate the Tx signal and are therefore lossy do NOT have gain (signal amplification) Wired Channel cable attenuation Wireless Channel free space path loss
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ECE 4710: Lecture #36 5 Signal Power @ Rx Power gain of channel P Rx is almost always much smaller than P Tx Example: Cell phone tower P Tx W while P Rx nW
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ECE 4710: Lecture #36 6 Antennas Antenna Power Gain ( G A ) NOT actual amplification of signal Power gain relative to “isotropic” antenna Isotropic antenna »“Iso” = same »Theoretical non-realizable antenna that radiates equal (same) power in all directions (spherical expansion) »Useful reference to compare performance of practical antennas Power gain
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ECE 4710: Lecture #36 7 Antennas Practical antennas Purpose is to radiate power in specific direction(s) towards Rx Focus P Tx in given direction greater focus larger “gain” Larger antenna size (relative to ) greater ability to focus energy in specific direction larger gain Antenna is effectively a transducer which takes a time- varying voltage from a circuit and launches a time-varying EM wave in free space »Only time-varying EM waves can effectively propagate large distances
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ECE 4710: Lecture #36 8 Power Density Radiated EM wave characterized by power density Power density = power per unit area ( W / m 2 ) Power density of isotropic antenna at distance d EIRP = Effective Isotropic Radiated Power Equal power at any given distance isotropic Power decays 1 / d 2 as surface area of sphere expands »Point source of EM energy Best case free space path gain (loss) is
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ECE 4710: Lecture #36 9 Power Density For real antenna the radiated power density is larger than P EIRP for direction of max radiation antenna gain FCC specifies EM radiation safety regulations in terms of electric field intensity E ( V / m ) instead of power density ( W / m 2 ) Conversion : Free-space wave impedance = 377
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ECE 4710: Lecture #36 10 Signal Power @ Rx Radiated power density of real antenna : Rx antenna at distance d will intercept / capture some of the Tx power density The amount of power captured at Rx is directly related to Rx antenna size or effective area ( A e ) Larger area = more power captured from Tx density
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ECE 4710: Lecture #36 11 Signal Power @ Rx Rx antenna gain is related to effective area by Thus the signal power at output of Rx antenna is Link Formula Friis Transmission Formula
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ECE 4710: Lecture #36 12 Antenna is a reciprocal element Gain is the same whether it is transmitting or receiving G A is linear quantity that is unitless relative measure between to powers In decibels G A (dB) = 10 log ( G A ) Antenna G A & A e
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ECE 4710: Lecture #36 13 Signal Power @ Rx Example 1: A PCS cell phone tower transmits at a frequency of 1.9 GHz, has a Tx power of 20 W, and an antenna gain 18 dB. Determine the Rx signal power (in dBm) of a mobile phone at a distance of 3 km assuming the Rx antenna has a gain of 3 dB and has a LOS link to Tx.
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ECE 4710: Lecture #36 14 Signal Power @ Rx Example 2: A DirecTV satellite is in geosynchronous orbit above the earth at an altitude of 22,300 miles. The satellite transmits at a frequency of 4 GHz, has a Tx power of 200 W, and uses a dish antenna with a 3 m radius. Determine the Rx signal power at a home Rx that also uses a dish antenna with 0.3 m ( 1 ft ) radius.
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ECE 4710: Lecture #36 15 Free Space Loss Recall that book defines where G FS is free space power gain Using Then where L FS is the free space loss :
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ECE 4710: Lecture #36 16 Free Space Loss Free space loss : in dB : Best case loss Free space free of all matter and particles (vacuum) Earth’s atmosphere can cause additional loss due to attenuation of EM wave by atmospheric molecules (O 2, H 2 0, etc.) »Only significant for f > 2 GHz and distances > 100 km Many links are not Line of Sight (LOS) obstructed (OBS)
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ECE 4710: Lecture #36 17 Free Space Loss For obstructed conditions (mobile radio) then useful model is n is path loss exponent n = 2 free space or LOS with no atmospheric attenuation n > 2 for OBS conditions Mobile radio path loss models use n = 2 – 5 and n in the range of 2.8 - 3.5 is typical
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ECE 4710: Lecture #36 18 Link Formula Link formula in simplest form predicts the best case received signal power Many factors can cause Rx signal power to be lower than simple form of link formula, e.g. Obstructed link »Building, trees, hills, earth curvature, etc. Atmospheric attenuation »f > 2 GHz and/or large separation distances Antenna misalignment (gain is less than max value)
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