Wireless data networks Physical Layer Martin Heusse X L A TEX E - - PowerPoint PPT Presentation

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Wireless data networks Physical Layer Martin Heusse X L A TEX E - - PowerPoint PPT Presentation

Wireless data networks Physical Layer Martin Heusse X L A TEX E Attenuation / Propagation Ethernet (twisted pair), attenuation < 10dB for 100m Fiber: typically 1dB/km Radio waves in the air: 10 2 dB/km Butthe signal is


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SLIDE 1

X E L

ATEX

Wireless data networks Physical Layer

Martin Heusse

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SLIDE 2
  • PHY. 2

Attenuation / Propagation

  • Ethernet (twisted pair), attenuation < 10dB for 100m
  • Fiber: typically 1dB/km
  • Radio waves in the air: 10−2dB/km

But—the signal is not guided: the energy is projected on a surface that grows with the distance Pr = PtGtGr ( λ 4πd )2 (Friis transmission equation) Pr,t received / transmitted power; Gr,t rec./trans. antenna gain; d: distance, λ: wavelength (Grλ is the effective area of the receiver)

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  • PHY. 3

Consequences

  • ✓ d = 1km → −80dB

✓ d = 10m → −40dB ✓ d = 1m → −30dB

  • I’m deaf when I’m talking
  • Relatively high gain input amplification
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SLIDE 4
  • PHY. 4

Real world propagation

  • Reflections
  • Diffraction
  • Absorption

Loss at 5GHz

✓ Wood house siding: 8̃dB ✓ Concrete wall: 22dB

  • Scattering
  • Doppler (People movement)
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  • PHY. 5

Fresnel zone

  • Elliptically shaped surface of revolution where the

reflected/diffracted path length is different by a multiple of 180° from the direct path

n = 3 d1 d2 r1 a b n = 1 n = 2 Transmitter Receiver Propagation path (can be curved)

Figure 2.19 Fresnel zones around a propagation path shown in 2 dimensions.

  • Surface such that: d1 + d2 + nλ/2 = a + b
  • rn ≈

nλd1d2 d1+d2

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SLIDE 6
  • PHY. 6

Two ray ground

ht hr d d1 d2

  • Pr = PtGtGr

( λ

4πd

)2

  • 1 −

(

d d1+d2

) e−jδφ

  • 2
  • If d1 + d2 ≈ d then |1 −

(

d d1+d2

) e−jδφ|2 ≈ δφ2 and (…) δφ = 2π

λ (d1 + d2 − d) ≈ 2π λ 2 hthr d

  • Then:

Pr = PtGtGr (hthr)2 d4

(No more proportional to λ…)

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  • PHY. 7

Antennas

  • Current → charge displacement → Electrical field…

Current in a two-wire transmission line

_ +

  • Corpuscular version: electrons emit photons when shaken!
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SLIDE 8
  • PHY. 8

Antennas (cont.)

  • Eletrical field lines
  • Dipole antenna

λ/2

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  • PHY. 9

Antennas (cont.)

Figure 4.11 Three-dimensional pattern of a λ/2 dipole. (SOURCE: C. A. Balanis, “Antenna Theory: A Review” Proc. IEEE, Vol. 80, No 1. Jan. 1992.  1992 IEEE).

Do not point it toward the intended receiver!

  • Marconi antenna

Same thing, using the reflection on a ground plane.

λ/4

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SLIDE 10
  • PHY. 10

Antennas (cont.)

θ θ 30° 0° 60° 90° 90° 60° 30° 120° 150° 180° 150° 120° Relative power (dB down) 10 20 30 20 10 30 − − − + + −

Two-dimensional amplitude patterns for a thin dipole of l = 1.25λ (Copied from Balanis)

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SLIDE 11
  • PHY. 11

Other antennas

  • Horn

July 11, 1962, first transmission from the US to france of a TV signal, bounced back by the Telstar satellite. The satellites were low orbiting so that required a tracking antenna. No positioning system on the satellite: they were spheres and no parabolic antenna!! Antenna weight: 280 tons! 6.69 GHz uplink, 4.12 GHz downlink. The radome is

  • inflated. Still the biggest radomes ever built, and still there in Plemeur-Bodou!
  • Yagi

Directors Driven element Reflector

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SLIDE 12
  • PHY. 12

Other antennas (cont.)

  • Parabola

+

All points equidistant from a fixed line and a fixed point

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SLIDE 13
  • PHY. 13

Modulation techniques

  • ASK
  • FSK
  • PSK (BPSK, QPSK)
  • QAM
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  • PHY. 14

Signal shaping

  • PSK exemple: abrupt transitions on symbol boundaries

1 2 3 4 5 −1.0 −0.5 0.0 0.5 1.0 t f (x)

→ Infinite spectrum! () ★ Signal shaping

✓ Ex.: raised cosine spectrum. ✓ The impulse response of a raised cosine is 0 at every nT (no interference at sampling instant)

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  • PHY. 15

Example: QAM modulation

R bps

sin(2πfct)

Shaping Shaping

cos(2πfct)

+

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  • PHY. 16

What is fading?

  • Additive white Gaussian noise (AWGN)

✓ Thermal noise, electronics, propagation

  • Rayleigh fading: multiple indirect paths; no dominant (LOS) path

✓ The signal enveloppe follows a Rayleigh distribution

★ Rician: there is a dominant path; parameter K = power(LOSpat)

powerotherpaths

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  • PHY. 17

What is fading? (cont.)

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SLIDE 18
  • PHY. 18

Spread spectrum

  • Use as much of the channel as possible

Make Ebb/N0 as large as possible

  • Helps in presence of narrow band interferences
  • Spread the transmitted power over a wider freq. range (ISM

bands…)

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SLIDE 19
  • PHY. 19

FHSS

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  • PHY. 20

DSSS

  • XOR each bit of data with a predefined sequence (or code)
  • Same operation at the receiver (x ⊗ c ⊗ c = x)
  • Used by 802.11b
  • Related to CDMA
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  • PHY. 21

OFDM Orthogonal Frequency Division Multiplexing

  • Many narrow band symbols sent in parallel

(→ gain and phase is constant in each sub-channel)

  • Good spectrum utilization
  • Limited complexity at both the emitter and receiver
  • Works great with severe channel conditions
  • But:

✓ Sensitive to Doppler shift ✓ Requires linear amplifiers, high peak to average power ratio (the power peaks when the sine waves add to each other)

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  • PHY. 22

OFDM Orthogonal Frequency Division Multiplexing (cont.)

  • 0.4
  • 0.2

0.2 0.4 0.6 0.8 1

  • 10
  • 5

5 10 sin(x+pi)/(x+pi) sin(x)/x sin(x-pi)/(x-pi)

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SLIDE 23
  • PHY. 23

OFDM Orthogonal Frequency Division Multiplexing (cont.)

Serial to parallel R bps IFFT

fc

Parallel to serial

T T T

DAC

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SLIDE 24
  • PHY. 24

OFDM Orthogonal Frequency Division Multiplexing (cont.)

  • Applications

✓ (A)DSL (250 sub-carriers split between uplink and downlink)

◮ Symbol duration: 231.88µs ↔ sub-carrier spacing: 4.3125

kHz ✓ 802.11a, g (48 sub-carriers) ✓ DVB-T (up to 8192 sub-carriers), DAB ✓ WiMAX ✓ LTE