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COSC 393: Lecture 2 Radio Fundamentals
40

COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Dec 23, 2015

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Page 1: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

COSC 393: Lecture 2

Radio Fundamentals

Page 2: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Radio Communication

• Radio signals

• Spectrum

• Transmitter

• Signal propagation

• Modulation

Page 3: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Radio Wave

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

Page 4: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Frequency and Wave length

• Relationship:

= c/f

• wave length ,

• speed of light c 3x108m/s,

• frequency f

Page 5: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Radio Spectrum

Page 6: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

• VLF = Very Low Frequency• LF = Low Frequency • MF = Medium Frequency• HF = High Frequency• VHF = Very High Frequency• UHF = Ultra High Frequency• SHF = Super High Frequency• EHF = Extra High Frequency• UV = Ultraviolet Light

1 Mm300 Hz

10 km30 kHz

100 m3 MHz

1 m300 MHz

10 mm30 GHz

100 m3 THz

1 m300 THz

visible lightVLF LF MF HF VHF UHF SHF EHF infrared UV

optical transmissioncoax cabletwisted pair

Page 7: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

• Isotropic radiator: Equal radiation in all directions (3D) - theoretical antenna

• Real antennas always have directive effects (vertically and/or horizontally)

• Different antennas have different radiation pattern.

Antennas

Page 8: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

• Dipoles with lengths /4 or Hertzian dipole with length /2 (length proportional to wavelength)

• Example: Radiation pattern of a simple Hertzian dipole

• Gain: maximum power in the direction of the main lobe compared to the power of an isotropic radiator (with the same average power)

side view (xy-plane)

x

y

side view (yz-plane)

z

y

top view (xz-plane)

x

z

simpledipole

/4 /2

Page 9: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

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

• Often used for base stations in a cellular system (e.g., covering a valley)

directedantenna

sectorizedantenna

Page 10: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Effect of a transmission

distance

sender

transmission

detection

interference

• 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

No effect

Page 11: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Signal propagation property

• Radio signal behaves like light in free space (straight line)

• Receiving power proportional to 1/d² (d = distance between sender and receiver)

• So ideally, the transmitter and a receiver must see each other!

Really?

Page 12: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Three means of propagation

• Ground wave

• Tropospheric wave

• Ionospheric or sky wave

Page 13: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Ground Wave

• travels in contact with earth’s surface• reflection, refraction and scattering by objects on

the ground• transmitter and receiver need NOT see each other• affects all frequencies• at VHF or higher, provides more reliable

propagation means• signal dies off rapidly as distance increases

Page 14: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Tropospheric Wave

• bending(refraction) of wave in the lower atmosphere

• VHF communication possible over a long distance

• bending increases with frequency – so higher frequency more chance of propagation

• More of an annoyance for VHF or UHF (cellular)

Page 15: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Ionospheric or Sky Wave

• Reflected back to earth by ionospheric layer of the earth atmosphere

• By repeated reflection, communication can be established over 1000s of miles

• Mainly at frequencies below 30MHz

• More effective at times of high sunspot activity

Page 16: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

reflection

scattering

diffraction

shadowing

4 possible events

Radio wave Radio wave

Radio wave

Page 17: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Multipath Characteristics

• A signal may arrive at a receiver

- many different times

- many different directions

- due to vector addition

. Reinforce

. Cancel

- signal strength differs from place to place

Page 18: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Mobile System

• Usually Base Station is not mobile

• Receiver could be moving (65mph!)

• Whenever relative motion exists

- Doppler shift

- Fading

• Even the motion of scatterers cause fading

Page 19: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Free Space Propagation

• Suppose we have unobstructed line-of-sight

Pr(d) = (Pt Gt Gr ^2)/(4)^2 d^2 L)-Pt transmitted power-Gt, Gr Antenna gain-wavelength in meters- d distance in meters- L (>= 1) system loss factor (not related to propagation.

Page 20: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Propagation Losses

• Two major components

- Long term fading m(t)

- Short term fading r(t)

Received signal s(t)

s(t) = m(t) r(t)

Page 21: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

dB - decibel

• Decibel, a logarithmic unit of intensity used to indicated power lost or gained between two signals.  Named after Alexander Graham Bell.

10 log (P1/P2)

Page 22: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Radio Signal Fading

T

Sig

nal s

tre n

g th

(dB

)

Time

Long term fading

Short term fading

Page 23: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Short term fading

• Also known as fast fading – caused by local multi paths.

• Observed over distance = ½ wave length• 30mph will experience several fast fades in a sec.• Given by Rayleigh Distribution• This is nothing but the square root of sum of the

square of two Gaussian functions.r = square root ( Ac * Ac + As * As)

Ac and As are two amplitude components of the field intensity of the signal

Page 24: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Long term fading

• Long term variation in mean signal level is also known as slow fading

• Caused by movement over large distances.• The probability density function is given by

a log-normal distribution- normal distribution on a log scale

P(m) = (1/m (m) 2) e^[-(log m – E(m))^2/(2 (m)^2)]

Page 25: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Delay Spread

• Signal follows different paths to reach same destination.

• So same signal may arrive many times at different time intervals.

Page 26: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Delay Spread

• In digital system, delay spread causes intersymbol interference.

• Therefore, there is a limit on the maximum symbol rate of a digital multipath channel.

• Obviously, delay spreads are different in different environment.

• (roughly between 0.2 to 3 microseconds)

Page 27: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Capacity of Channel

• What is the maximum transmission rate so that the channel has very high reliability?

- error free capacity of a channel

• C.E. Shannon’s work suggest that signaling scheme exists for error-free transmission if the rate of transmission is lower than the channel capacity.

Page 28: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Shannon’s work

• C - channel capacity (bits/s)• B – transmission bandwidth (Hz)• E – energy per bit of received signal (Joule)• R – information rate (bits/s)• S = E R – signal power• N – single-sided noise power spectral density (W/Hz)(C/B) = log [1+(S/(NB))] = log [1+(E/N)(R/B)]Suppose R = C we have

(C/B) = log [1+(E/N)(C/B)]

Page 29: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Shannon’s work - continued

• Solving for (E/N) (aka. signal to noise ratio)

(E/N) = (2^a –1)/a

where a = (C/B).

So given C= 19.2kb/s and bandwidth = 30kHz

What is E/N required for error-free transmission?

R/B = 19.2/30 = 0.64

Substituting we get E/N = 0.8724 = -0.593dB

So control transmission power to obtain this E/N.

Page 30: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Propagation models in built-up areas

• Propagation is strongly influenced by the environment

- building characteristics

- vegetation density

- terrain variation

• Perfect conductors reflect the wave where as nonconductors absorb some energy!

Page 31: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Empirical models to predict propagation losses

• Okumura’s model- based on free space path loss + correction

factors for suburban and rural areas, irregular terrain, street orientations

• Sakagmi and Kuboi model- extend Okumura’s model using regression

analysis of data.• Hata’s model

- empirical formula to describe Okumura’s data

Page 32: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

More models

• Ibrahim and Parsons model

- equations developed to best fit data observed at London. (freq. 168-900 MHz)

• Lee’s model– Use at 900MHZ– 3 parameters (median trasmission loss, slope of

the path loss curve and adjustment factor)

Page 33: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Freq. for mobile communication

2.2.1

• VHF-/UHF-ranges for mobile radio– simple, small antenna

• SHF and higher for directed radio links, satellite communication– small antenna, focusing– large bandwidth available

• Wireless LANs use frequencies in UHF to SHF spectrum– limitations due to absorption by water and oxygen

• weather dependent fading, signal loss due to by heavy rainfall etc.

Page 34: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Modulation

• Digital modulation– digital data is translated into an analog signal – ASK, FSK, PSK (… Shift Keying)– 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)

Page 35: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Types of Modulation

• Amplitude modulation

• Frequency modulation

• Phase modulation

• Combination modulation

Page 36: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

synchronizationdecision

digitaldataanalog

demodulation

radiocarrier

analogbasebandsignal

101101001 radio receiver

digitalmodulation

digitaldata analog

modulation

radiocarrier

analogbasebandsignal

101101001 radio transmitter

Page 37: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Amplitude Modulation

Page 38: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Frequency Modulation

Page 39: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Phase Modulation

Page 40: COSC 393: Lecture 2 Radio Fundamentals. Radio Communication Radio signals Spectrum Transmitter Signal propagation Modulation.

Digital modulation

• Amplitude Shift Keying (ASK):– simple– low bandwidth – susceptible to interference

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

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

1 0 1

t

1 0 1

t

1 0 1

t