lecture2 antennas and propagation

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Antennas and Propagation Antennas and Propagation NETW4004 Lecture 2 NETW4004 Lecture 2 Source: Stallings Ch.5 Source: Stallings Ch.5

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Page 1: Lecture2 antennas and propagation

Antennas and PropagationAntennas and Propagation

NETW4004 Lecture 2NETW4004 Lecture 2

Source: Stallings Ch.5Source: Stallings Ch.5

Page 2: Lecture2 antennas and propagation

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

Antenna characteristics essentially the same when sending or receiving electromagnetic energy

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Page 3: Lecture2 antennas and propagation

Example: Quarter-Wave Antenna

Source: A VISUAL TOUR OF CLASSICAL ELECTROMAGNETISM, MIT Physics 8.02: Electromagnetism I

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Page 4: Lecture2 antennas and propagation

Types of Antennas Isotropic antenna (idealized)

A point of space that 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

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Page 5: Lecture2 antennas and propagation

Antenna: Gain and Effective Area 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

Relationship between antenna gain and effective area

• G = antenna gain

• Ae = effective area

• f = carrier frequency• c = speed of light ∀λ = carrier wavelength

2

2

2

44

c

AfAG ee π

λπ ==

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Page 6: Lecture2 antennas and propagation

More on Duality Electromagnetic signals have time domain

as well as frequency domain representations.

Waveforms in time domain and frequency domain has duality.

Convolution and multiplication in t.d. and f.d. have duality.

Light/electromagnetic wave has duality. Wave Particle

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Page 7: Lecture2 antennas and propagation

Propagation Modes Ground-wave propagation Sky-wave propagation Line-of-sight (LOS) propagation

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Page 8: Lecture2 antennas and propagation

Ground Wave Propagation Follows contour of the earth Can propagate considerable distances Frequencies up to 2 MHz Example

AM radio

Earth

Signal propagation

transmit antenna receive

antenna

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Page 9: Lecture2 antennas and propagation

Source: http://www.tpub.com/neets/book10/40e.htm

Ionosphere Refraction Reflection effect caused by refraction

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Page 10: Lecture2 antennas and propagation

Sky Wave Propagation Signal reflected from ionized layer of atmosphere back

down to earth Signal can travel a number of hops, back and forth

between ionosphere and earth’s surface Picks up thousands of kilometers Examples

Amateur radio CB radio Long-distance broadcast

Earth

Ionosphere

transmit antenna receive

antenna10

Page 11: Lecture2 antennas and propagation

Line-of-Sight Propagation Transmitting and receiving antennas

must be within line of sight Satellite communication – signal above 30

MHz not reflected by ionosphere Ground communication – antennas within effective line of site due to refraction

Earth

transmit antenna

receive antenna

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Page 12: Lecture2 antennas and propagation

Line-of-Sight Equations Optical line of sight

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:

• h1, h2: heights of the two antennas

hd 57.3=

hd Κ= 57.3

( )2157.3 hhd Κ+Κ=

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Page 13: Lecture2 antennas and propagation

LOS Transmission Impairments Attenuation and attenuation distortion Free space loss Noise Atmospheric absorption Multipath Refraction Thermal noise

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Page 14: Lecture2 antennas and propagation

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

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Page 15: Lecture2 antennas and propagation

Free Space Loss Free space loss, ideal isotropic antenna

• Pt = signal power at transmitting antenna• Pr = signal power at receiving antenna∀λ = carrier wavelength• d = propagation distance between antennas• c = speed of light • where d and λ are in the same units (e.g., meters)

Recast

( ) ( )2

2

2

2 44

c

fdd

P

P

r

t πλπ ==

( ) ( ) dB 98.21log20log20 ++−= dLdB λ

( ) ( ) dB 56.147log20log20 −+= df15

Page 16: Lecture2 antennas and propagation

Free Space Loss with Antenna Gains Free space loss accounting for gain of other

antennas

• Gt = gain of transmitting antenna

• Gr = gain of receiving antenna

• At = effective area of transmitting antenna

• Ar = effective area of receiving antenna

Recast as

( ) ( ) ( ) ( )trtrtrr

t

AAf

cd

AA

d

GG

d

P

P2

22

2

224 === λλ

π

( ) ( ) ( )rtdB AAdL log10log20log20 −+= λ( ) ( ) ( ) dB54.169log10log20log20 +−+−= rtAAdf

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Page 17: Lecture2 antennas and propagation
Page 18: Lecture2 antennas and propagation

So Many Noises Thermal Noise Intermodulation noise Crosstalk Impulse Noise How much is the noise?

Ratio of signal energy per bit to noise power density per Hertz

Related to SNR Suppose the bit rate R increases, the

transmission signal power S should increase to maintain the same Eb/N0.

00

/

N

RS

N

Eb =

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Page 19: Lecture2 antennas and propagation

Thermal Noise Thermal noise due to agitation of electrons Present in all electronic devices and transmission

media; cannot be eliminated Function of temperature Particularly significant for satellite communication Thermal noise present in a bandwidth of B Hz (in

watts):

• k = Boltzmann's constant• T = temperature, in kelvins (absolute temperature)

TBN k=

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Page 20: Lecture2 antennas and propagation

Other Noises Intermodulation noise – occurs if signals with

different frequencies share the same medium A signal produced at a frequency that is the sum or

difference of original frequencies Nonlinearity in transmitter, receiver systems.

Crosstalk Unwanted coupling between signal paths Dominates in unlicensed ISM bands

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 Primary source of error in digital data transmission

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Page 21: Lecture2 antennas and propagation

Other Impairments Atmospheric absorption – water vapor

and oxygen contribute to attenuation Rain and fog are significant damaging factors

Multipath – obstacles reflect signals so that multiple copies with varying delays are received

Refraction – bending of radio waves as they propagate through the atmosphere

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Page 22: Lecture2 antennas and propagation

Multipath Propagation

Figure 5.10 Sketch of three important propagation mechanisms: Reflection (R), Scattering (S), Diffraction (D)

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Page 23: Lecture2 antennas and propagation

Multipath Propagation Reflection - occurs when signal

encounters a surface that is large relative to the wavelength of the signal

Diffraction - occurs at the edge of an impenetrable body that is large compared to wavelength of radio wave

Scattering – occurs when incoming signal hits an object whose size in the order of the wavelength of the signal or less

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Page 24: Lecture2 antennas and propagation

The Effects of Multipath Propagation Multiple copies of a signal may arrive at different

phases If phases add destructively, the signal level relative to

noise declines, making detection more difficult

Intersymbol interference (ISI) One or more delayed copies of a pulse may arrive at

the same time as the primary pulse for a subsequent bit

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Page 25: Lecture2 antennas and propagation

Fading Time variation of received signal power caused

by changes in the medium or path, e.g., rainfall, mobility etc.

Fast fading: over a distance of a half of wavelength

Slow fading: change in average received power over larger distances

Fading pattern on frequencies: flat fading or selective fading

Rayleigh fading: e.g. urban settings Rician fading: LOS, e.g. indoor

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Page 26: Lecture2 antennas and propagation

Error Compensation Mechanisms Forward error correction Adaptive equalization Diversity techniques

Space diversity: use of collocated directional antennas

Frequency diversity: eg. using spread spectrum

Time diversity: using TDMA

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Page 27: Lecture2 antennas and propagation

Recap Antennas Propagation modes LOS loss model Noise: types and causes Other impairments esp. multipath Fading

Try Problems 5.2, 13 ~ 17 in William Stallings Text Book.

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