By Ya Bao1 Antennas and Propagation. 2 By Ya Bao Introduction An antenna is an electrical conductor or system of conductors Transmission - radiates electromagnetic.

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Presentation transcript:

by Ya Bao1 Antennas and Propagation

2 By Ya Bao Introduction An antenna is an electrical conductor or system of conductors Transmission - radiates electromagnetic energy into space Reception - collects electromagnetic energy from space In two-way communication, the same antenna can be used for transmission and reception

3 By Ya Bao Radiation Patterns Radiation pattern Graphical representation of radiation properties of an antenna Depicted as two-dimensional cross section Beam width (or half-power beam width) Measure of directivity of antenna Reception pattern Receiving antenna’s equivalent to radiation pattern

4 By Ya Bao Radiation patterns

5 By Ya Bao Types of Antennas Isotropic antenna (idealized) Radiates power equally in all directions Dipole antennas Half-wave dipole antenna (or Hertz antenna) Quarter-wave vertical antenna (or Marconi antenna) Parabolic Reflective Antenna

6 By Ya Bao

7 Antenna Gain Antenna gain Power output, in a particular direction, compared to that produced in any direction by a perfect omnidirectional antenna (isotropic antenna) Effective area Related to physical size and shape of antenna

8 By Ya Bao Antenna Gain Relationship between antenna gain and effective area G = antenna gain A e = effective area f = carrier frequency c = speed of light (» 3 ´ 10 8 m/s) = carrier wavelength

9 By Ya Bao

10 By Ya Bao Propagation Modes Ground-wave propagation Sky-wave propagation Line-of-sight propagation

11 By Ya Bao Ground Wave Propagation

12 By Ya Bao Sky Wave Propagation

13 By Ya Bao Line-of-Sight Propagation

14 By Ya Bao Line-of-Sight Equations Effective, or radio, line of sight d = distance between antenna and horizon (km) h = antenna height (m) K = adjustment factor to account for refraction, rule of thumb K = 4/3 Maximum distance between two antennas for LOS propagation:

15 By Ya Bao LOS Wireless Transmission Impairments Attenuation and attenuation distortion Free space loss Noise Atmospheric absorption Multipath Refraction Thermal noise

16 By Ya Bao Attenuation Strength of signal falls off with distance over transmission medium Attenuation factors for unguided media: Received signal must have sufficient strength so that circuitry in the receiver can interpret the signal Signal must maintain a level sufficiently higher than noise to be received without error Attenuation is greater at higher frequencies, causing distortion

17 By Ya Bao Free Space Loss Free space loss, ideal isotropic antenna P t = signal power at transmitting antenna P r = signal power at receiving antenna = carrier wavelength d = propagation distance between antennas c = speed of light (» 3 ´ 10 8 m/s) where d and are in the same units (e.g., meters)

18 By Ya Bao Free Space Loss Free space loss equation can be recast:

19 By Ya Bao Free Space Loss Free space loss accounting for gain of other antennas can be recast as

20 By Ya Bao Categories of Noise Thermal Noise Intermodulation noise Crosstalk Impulse Noise

21 By Ya Bao Thermal Noise Amount of thermal noise to be found in a bandwidth of 1Hz in any device or conductor is: N 0 = noise power density in watts per 1 Hz of bandwidth k = Boltzmann's constant =  J/K T = temperature, in kelvins (absolute temperature)

22 By Ya Bao Thermal Noise Noise is assumed to be independent of frequency Thermal noise present in a bandwidth of B Hertz (in watts): or, in decibel-watts

23 By Ya Bao Noise Terminology Intermodulation noise – occurs if signals with different frequencies share the same medium Interference caused by a signal produced at a frequency that is the sum or difference of original frequencies Crosstalk – unwanted coupling between signal paths Impulse noise – irregular pulses or noise spikes Short duration and of relatively high amplitude Caused by external electromagnetic disturbances, or faults and flaws in the communications system

24 By Ya Bao Expression E b /N 0 Ratio of signal energy per bit to noise power density per Hertz The bit error rate for digital data is a function of E b /N 0 Given a value for E b /N 0 to achieve a desired error rate, parameters of this formula can be selected As bit rate R increases, transmitted signal power must increase to maintain required E b /N 0

Multipath Propagation