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Physical layer Taekyoung Kwon

Physical layer

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Physical layer. Taekyoung Kwon. signal. physical representation of data function of time and location signal parameters of periodic signals: period T, frequency f=1/T, amplitude A, phase shift  E.g., sinewave is expressed as s(t) = A t sin(2  f t t +  t ). - PowerPoint PPT Presentation

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Page 1: Physical layer

Physical layer

Taekyoung Kwon

Page 2: Physical layer

signal

• physical representation of data

• function of time and location

• signal parameters of periodic signals: period T, frequency f=1/T, amplitude A, phase shift – E.g., sinewave is expressed as

s(t) = At sin(2 ft t + t)

Page 3: Physical layer

Signal (Fourier representation)

)2cos()2sin(2

1)(

11

nftbnftactgn

nn

n

1

0

1

0

t t

ideal periodic signal real composition

Digital signals need

• infinite frequencies for perfect transmission (UWB?)

• modulation with a carrier frequency for transmission (analog signal!)

Page 4: Physical layer

signal• Different representations of signals

– amplitude (amplitude domain)– frequency spectrum (frequency domain)– phase state diagram (amplitude M and phase in polar

coordinates)

f [Hz]

A [V]

I= M cos

Q = M sin

A [V]

t[s]

Page 5: Physical layer

Radio frequency

직진성

Page 6: Physical layer

Radio channel type

* Ground wave = surface wave + space wave

Page 7: Physical layer

Radio channel type

-> Really? 802.16

Page 8: Physical layer

Radio channel type

Page 9: Physical layer

Why 60GHz?

Page 10: Physical layer

Why 60GHz? Frequency reuse

Page 11: Physical layer

Signal propagation ranges

• Transmission range– communication possible– low error rate

• Detection range– detection of the signal

possible– no communication

possible

• Interference range– signal may not be

detected – signal adds to the

background noise

distance

Xmission

detection

interference

Page 12: Physical layer

Radio propagation

Page 13: Physical layer

Attenuation in real world

• Exponent “a” can be up to 6, 7

Page 14: Physical layer

propagation

reflection scattering diffraction

Page 15: Physical layer

Signal propagation models• Slow fading (shadowing)

– Distance between Tx-Rx– Signal strength over distance

• fast fading– Fluctuations of the signal strength– Short distance– Short time duration– LOS vs. NLOS

Page 16: Physical layer

Slow fading vs. fast fading

short term fading

long termfading

t

power

• Slow fading = long-term fading• Fast fading = short-term fading

Page 17: Physical layer

shadowing

• Real world• Main propagation mechanism: reflections• Attenuation of signal strength due to power loss

along distance traveled: shadowing• Distribution of power loss in dBs: Log-Normal• Log-Normal shadowing model• Fluctuations around a slowly varying mean

Page 18: Physical layer

shadowing

Page 19: Physical layer

Fast fading

T-R separation distances are smallHeavily populated, urban areasMain propagation mechanism: scatteringMultiple copies of transmitted signal arriving at the transmitted via different paths and at different time-delays, add vector-like at the receiver: fadingDistribution of signal attenuation coefficient: Rayleigh, Ricean.Short-term fading modelRapid and severe signal fluctuations around a slowly varying mean

Page 20: Physical layer

Fast fading

Page 21: Physical layer

Fast fading

Page 22: Physical layer

Fast fading

Page 23: Physical layer

The final propagation model

Page 24: Physical layer

Real world example

Page 25: Physical layer

Modulation and demodulation

synchronizationdecision

digitaldataanalog

demodulation

radiocarrier

analogbasebandsignal

101101001 radio receiver

digitalmodulation

digitaldata analog

modulation

radiocarrier

analogbasebandsignal

101101001 radio transmitter

UWB: no carrier-> low cost, low power

Page 26: Physical layer

modulation

• Digital modulation– digital data is translated into an analog signal (baseband)– ASK, FSK, PSK– differences in spectral efficiency, power efficiency, robustness

• Analog modulation– shifts center frequency of baseband signal up to the radio carrier– Motivation

• smaller antennas (e.g., /4)• Frequency Division Multiplexing• medium characteristics

– Basic schemes• Amplitude Modulation (AM)• Frequency Modulation (FM)• Phase Modulation (PM)

Page 27: Physical layer

Digital modulation• Modulation of digital signals known as Shift Keying• Amplitude Shift Keying (ASK):

– very simple– low bandwidth requirements– very susceptible to interference

• Frequency Shift Keying (FSK):– needs larger bandwidth

• Phase Shift Keying (PSK):– more complex– robust against interference

1 0 1

t

1 0 1

t

1 0 1

t

Page 28: Physical layer

antenna• Radiation and reception of electromagnetic waves• Isotropic radiator: equal radiation in all directions (three

dimensional) - only a theoretical reference antenna• Real antennas always have directive effects (vertically

and/or horizontally)

zy

x

z

y x idealisotropicradiator

Page 29: Physical layer

antenna

• Isotropic

• Omni-directional– Radiation in every direction on

azimuth/horizontal plane

• Directional– Narrower beamwidth, higher gain

Page 30: Physical layer

Omni vs directional

Page 31: Physical layer

Antenna (directed or sectorized)• E.g. 3 sectors per BS in cellular networks

side view (xy-plane)

x

y

side view (yz-plane)

z

y

top view (xz-plane)

x

z

top view, 3 sector

x

z

top view, 6 sector

x

z

directedantenna

sectorizedantenna

Page 32: Physical layer

Switched vs. adaptive

Page 33: Physical layer

Switched vs. adaptive

Page 34: Physical layer

MIMO?

Page 35: Physical layer

Why directional antenna?

• Wireless channel is a shared one• Transmission along a single multi-

hop path inhibits a lot of nodes• Shorter hops help, but to a certain

degree• Gupta-Kumar capacity result:

– T = O( W / sqrt(nlogn) )

• Major culprit is “omnidirectionality”

Page 36: Physical layer

Why directional antenna?

• Less energy in wrong directions

• Higher spatial reuse– Higher throughput

• Longer ranges– Less e2e delay

• Better immunity to other transmission– Due to “nulling” capability

Page 37: Physical layer

Directional vs. networks

• One-hop wireless environments– Cellular, WLAN infrastructure mode- BS, AP: directional antenna- Mobile: omni-directional

• Ad hoc, sensor networking- Every node is directional

Page 38: Physical layer

Directional antenna types

• Switched: can select one from a set of predefined beams/antennas

• Adaptive (steerable): – can point in almost any direction– can combine signals received at different

antennas– requires more signal processing

Page 39: Physical layer

Antenna model2 Operation Modes: Omni and Directional

A node may operate in any one mode at any given time

Page 40: Physical layer

Antenna modelIn Omni Mode:• Nodes receive signals with gain Go

• While idle a node stays in omni mode

In Directional Mode:• Capable of beamforming in specified direction• Directional Gain Gd (Gd > Go)

Symmetry: Transmit gain = Receive gain

Page 41: Physical layer

Potential benefits

• Increase “range”, keeping transmit power constant

• Reduce transmit power, keeping range comparable with omni mode– Reduces interference, potentially

increasing spatial reuse

Page 42: Physical layer

neighbor

• Notion of a “neighbor” needs to be reconsidered

– Similarly, the notion of a “broadcast” must also be reconsidered

Page 43: Physical layer

Directional neighbor

B

A

• When C transmits directionally

•Node A sufficiently close to receive in omni mode

•Node C and A are Directional-Omni (DO) neighbors

•Nodes C and B are not DO neighbors

C

Transmit BeamReceive Beam

Page 44: Physical layer

Directional neighbor

AB C

•When C transmits directionally

• Node B receives packets from C only in directional mode

•C and B are Directional-Directional (DD) neighbors

Transmit BeamReceive Beam

Page 45: Physical layer

Directional antenna for MAC

• Less energy consumption– Within the boundary of omni-

directional Xmission range

• Same energy consumption

• DD neighbor is possible

Page 46: Physical layer

Directional antenna for routing

• same energy consumption

• One hop directional transmission across multi-hop omnidirectional transmission

• DO neighbor will be the norm

Page 47: Physical layer

D-MAC Protocol[Ko2000Infocom]

Page 48: Physical layer

DATA DATA

RTS RTS

CTS CTS

ACKACK

B C ED

Reserved area

AF

IEEE 802.11

Page 49: Physical layer

Directional MAC (D-MAC)

• Directional antenna can limit transmission to a smaller region (e.g., 90 degrees).

• Basic philosophy: MAC protocol similar to IEEE 802.11, but on a per-antenna basis

Page 50: Physical layer

D-MAC• IEEE802.11: Node X is blocked if node X has

received an RTS or CTS for on-going transfer between two other nodes

• D-MAC: Antenna T at node X is blocked if antenna T received an RTS or CTS for an on-going transmission

• Transfer allowed using unblocked antennas• If multiple transmissions are received on

different antennas, they are assumed to interfere

Page 51: Physical layer

D-MAC Protocols

• Based on location information of the receiver, sender selects an appropriate directional antenna

• Signature table

Page 52: Physical layer

D-MAC Scheme 1

• Uses directional antenna for sending RTS, DATA and ACK in a particular direction, whereas CTS sent omni-directionally

• Directional RTS (DRTS) andOmni-directional CTS (OCTS)

Page 53: Physical layer

DATA

DRTS(B)

OCTS(B,C) OCTS(B,C)

ACK

A B C ED

DRTS(D)

DATA

ACK

OCTS(D,E)

DRTS(B) - Directional RTS includinglocation information of node B

OCTS(B,C) – Omni-directional CTSincluding location informationof nodes B and C

D-MAC Scheme 1: DRTS/OCTS

Page 54: Physical layer

DATA

DRTS(B)

OCTS(B,C) OCTS(B,C)

ACK

A B C D

DRTS(A)

?

DRTS(A)

Drawback of Scheme 1

• Collision-free ACK transmission not guaranteed

Page 55: Physical layer

D-MAC Scheme 2

• Scheme 2 is similar to Scheme 1, except for using two types of RTS

• Directional RTS (DRTS) / Omni-directional RTS (ORTS) both used – If none of the sender’s directional antennas are

blocked, send ORTS– Otherwise, send DRTS when the desired antenna

is not blocked

Page 56: Physical layer

D-MAC Scheme 2

• Probability of ACK collision lower than scheme 1

• Possibilities for simultaneous transmission by neighboring nodes reduced compared to scheme 1