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Cellular Mobile Communication Systems Lecture 2

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1 Cellular Mobile Communication Systems Lecture 2
Engr. Shahryar Saleem Assistant Professor Department of Telecom Engineering University of Engineering and Technology Taxila TI -1011 TI -1011

2 Wireless Issues • Wireless link implications
– communications channel is the air • poor quality: fading, shadowing, weather, etc. – regulated by governments • frequency allocated, licensing, etc. – limited bandwidth • Low bit rate, frequency planning and reuse, interference – power limitations • Power levels regulated, must conserve mobile terminal battery life – security issues • wireless channel is a broadcast medium! • Wireless link implications for communications – How to send signal? – How to clean up the signal in order to have good quality – How to deal with limited bandwidth? • Design network and increase capacity/share bandwidth in a cell TI -1011

3 Typical Wireless Communication System

4 Components of Communication System
• Source – Produces information for transmission (e.g., voice, keypad entry, etc.) • Source encoder – Removes the redundancies and efficiently encodes the information • Channel encoder – Adds redundant bits to the source bits to recover from any error that the channel may introduce • Modulator – Converts the encoded bits into a signal suitable for transmission over the channel • Antenna – A transducer for converting guided signals in a transmission line into electromagnetic radiation in an unbounded medium or vice versa • Channel – Carries the signal, but will usually distort it • Receiver – reverses the operations TI -1011

5 What is Signal Propagation
How is a radio signal transformed from the time it leaves a transmitter to the time it reaches the receiver • Important for the design, operation and analysis of wireless networks – Where should base stations/access points be placed – What transmit powers should be used – What radio frequencies need be assigned to a base station – How are handoff decision algorithms affected… • Propagation in free open space like light rays • In general make analogy to light and sound waves TI -1011

6 Signal Propagation • Received signal strength (RSS) influenced by
– Fading – signal weakens with distance - proportional to1/d² (d = distance between sender and receiver) – Frequency dependent fading – signal weakens with increase in f – Shadowing (no line of sight path) – Reflection off of large obstacles – Scattering at small obstacles – Diffraction at edges TI -1011

7 Signal Propagation Effects are similar indoors and outdoors
Several paths from Tx to Rx – Different delays, phases and amplitudes – Add motion – makes it very complicated TI -1011

8 Multipath Propagation
• Signal can take many different paths between sender and receiver due to reflection, scattering, diffraction • Time dispersion: signal is dispersed over time interference with “neighbor” symbols, Inter Symbol Interference (ISI) The signal reaches a receiver directly and phase shifted distorted signal depending on the phases of the different parts TI -1011

9 Effects of Mobility Time Variations in Signal Strength
• Channel characteristics change over time and location – signal paths change – different delay variations of different signal parts – different phases of signal parts • Quick changes in the power received (short term or fast fading) Slow changes in the average power received (long term fading) • Additional changes in; – distance to sender – obstacles further away TI -1011

10 Fading Fading refers to the Time variation of the received signal power caused by the changes in the telecommunication medium or path. When a signal is transmitted from a sender to the receiver multiple copies of the signal are formed due to the obstructions in the path between sender and receiver. Each signal copy will experience different; Attenuation Delay Phase shift This can result in either constructive or destructive interference, amplifying or attenuating the signal power as seen at the receiver. TI -1011

11 Types of Fading Slow fading/ Shadowing/ Long Term Fading/ Large Scale Fading: Caused by larger movements of the mobile or obstructions within the propagation environment. Fast Fading/ Multipath Fading/ Short Term Fading/ Small Scale Fading: Caused by the small movements of the mobile or obstruction. TI -1011

12 Communication Issues and Radio Propagation
Three main issues in radio channel – Achievable signal coverage • What is geographic area covered by the signal • Governed by path loss – Achievable channel rates (bps) • Governed by multipath delay spread – Channel fluctuations – effect data rate • Governed by Doppler spread and multipath TI -1011

13 Communication Issues and Radio Propagation

14 Coverage Determines – Transmit power required to provide service in a given area (link budget) – Interference from other transmitters – Number of base stations or access points that are required • Parameters of importance (Large Scale/ long Term Fading effects) – Path loss (long term fading) – Shadow fading (No LOS) TI -1011

15 Signal Coverage Range 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 TI -1011

16 Decibels Power (signal strength) is expressed in decibels (dB) for ease of calculation – Values relative to 1 mW are expressed in dBm – Values relative to 1 W are expressed in dBW – Other values are simply expressed in dB • Example 1: Express 2 W in dBm and dBW – dBm: 10 log10 (2 W / 1 mW) = 10 log10(2000) = 33 dBm – dBW: 10 log10 (2 W / 1 W) = 10 log10(2) = 3 dBW • In general dBm value = 30 + dBW value TI -1011

17 Free Space Loss Model Assumptions and the transmitted signal strength
– Transmitter and receiver are in free space – No obstructing objects in between – The earth is at an infinite distance! – The transmitted power is Pt – The received power is Pr – Isotropic antennas • Antennas radiate and receive equally in all directions with unit gain • The path loss is the difference between the received signal strength and the transmitted signal strength PL = Pt (dB) – Pr (dB) TI -1011

18 Free Space Loss Transmit power Pt • Received power Pr
• Wavelength of the RF carrier λ = c/f • Over a distance d the relationship between Pt and Pr is given by: • In dB, we have: • Pr (dBm)= Pt (dBm) log10 (λ) – 20 log10 (d) • Path Loss = PL = Pt – Pr = log10(λ) + 20log10 (d) TI -1011

19 Free Space Propagation
Notice that factor of 10 increase in distance => 20 dB increase in path loss (20 dB/decade) Distance Path 880 MHz d= 1km PL= dB d= 10Km PL= dB • Note that higher the frequency the greater the path loss for a fixed distance Distance 880 MHz 1960MHz 1km dB dB Thus 7 dB greater path loss for PCS band compared to cellular band TI -1011

20 Example Can use model to predict coverage area of a base station

21 A Simple Explanation of Free Space Propagation
Isotropic transmit antenna – Radiates signal equally in all directions • Assume a point source – At a distance d from the transmitter, the area of the sphere enclosing the Tx is A = 4πd2 – The “power density” on this sphere is Pt / 4πd2 • Isotropic receive antenna – Captures power equal to the density times the area of the antenna – Ideal area of antenna is Aant = λ2/4π • The received power is: Pr = Pt / 4πd2 × λ2/4π = Pt λ2/(4πd)2 TI -1011

22 Isotropic and Real Antennas
Isotropic antennas are “ideal” and cannot be achieved in practice – Useful as a theoretical benchmark • Real antennas have gains in different directions – Suppose the gain of the transmit antenna in the direction of interest is Gt and that of the receive antenna is Gr – The free space relation is: Pr = Pt Gt Gr λ2/(4πd)2 • The quantity Pt Gt is called the effective isotropic radiated power (EIRP) – This is the transmit power that a transmitter should use were it having an isotropic antenna TI -1011

23 Two-Ray Model for Mobile Radio Environment
Where; d1= line of sight path d2= ground reflected paths ht= Height of the transmitter hr= Height of the receiver TI -1011

24 Two-Ray Model for Mobile Radio Environment
Using the method of images the line-of-sight path and the ground reflected path can be calculated TI -1011

25 Received Power for Two-Ray Model
From the image diagram we have; The relationship between the transmit power and the received power is; Notice that factor of 10 increase in distance => 40 dB increase in path loss (40 dB/decade) The Received Power can be increased by raising the heights of the transmit and receive antenna TI -1011

26 Diffraction Loss Diffraction occurs when the radio path between the Tx and Rx is obstructed by surfaces that have sharp edges Edges act as a secondary line source The diffraction parameter ν is defined as • hm is the height of the obstacle • dt is distance transmitter-obstacle • dr is distance receiver-obstacle The diffraction loss Ld (dB) is approximated by TI -1011

27 Diffraction Example TI -1011

28 Path Loss Models Commonly used to estimate link budgets, cell sizes and shapes, capacity, handoff criteria etc. • “Macroscopic” or “large scale” variation of RSS • Path loss = loss in signal strength as a function of distance – Terrain dependent (urban, rural, mountainous), ground reflection, diffraction, etc. – Site dependent (antenna heights for example) – Frequency dependent – Line of site or not TI -1011

29 Environment Based Path Loss Model
Basic characterization: LP = L0 + 10α log10(d) – L0 is termed the frequency dependent component – The parameter α is called the “path loss gradient” or exponent – The value of α determines how quickly the RSS falls α determined by measurements in typical environment – For example • α = 2.5 might be used for rural area • α = 4.8 might be used for dense urban area Variations on this approach – Try and add more terms to the model – Directly curve fit data • Indoor and Outdoor Models – Okumura-Hata, COST 231, JTC TI -1011

30 Shadow Fading The signal strength for the same distance from the TX and RX is different for different locations depending upon the environment LP= L0 + 10α log (d) provides the mean value of the received signal strength at distance ‘d’ The variation of the signal strength around this value is known as Shadow fading or Slow fading The path loss equation becomes; LP= L0 + 10α log (d) + X Where X is the random variable whose distribution depends on the fading component Measurement studies show that X can be modeled with a lognormal distribution with mean = zero and standard deviation σ db TI -1011

31 Fade Margin In order to provide adequate signal strengths to locations where transmitted signal may no reach Add a Fade Margin to the path loss or the received signal strength LP= L0 + 10α log (d) + F Where F is the Fade Margin associated with the path loss to overcome the shadow fading effects Fade Margin can be applied by – Reducing cell size – Increasing transmit power – Making the receiver more sensitive TI -1011

32 Path Loss for Macrocellular Areas Okumura-Hata Model
Okumura collected measurement data ( in Tokyo) and plotted a set of curves for path loss in urban areas Frequency range 100 MHz to 1,920 MHz Identified the height of the Tx and Rx as important parameters Hata came up with an empirical model for Okumura’s curves Lp = log fc – log hte – a(hre) + (44.9–6.55 log hte)log d Where fc is in MHz, d is distance in km, and hte is the base station transmitter antenna height in meters and hre is the mobile receiver antenna height in meters for fc > 400 MHz and large city a(hre) = 3.2 (log [11.75 hre])2 – 4.97 dB • See Table 2.1 in textbook for other cases TI -1011

33 Example of Hata’s Model
Consider the case where hre = 2 m, receiver antenna’s height hte = 100 m, transmitter antenna’s height fc = 900 MHz, carrier frequency • Lp = log d – The path loss exponent for this particular case is α = 3.18 • What is the path loss at d = 5 km? – d = 5 km Lp = log 5 = dB • If the maximum allowed path loss is 120 dB,what distance can the signal travel? – Lp = 120 = log d => d =10(1.86/31.8) = 1.14 km TI -1011

34 COST Model Models developed by COST
– European Cooperative for Science and Technology – Collected measurement data – Plotted a set of curves for path loss in various areas around the 1900 MHz band – Developed a Hata-like model Lp = log fc – log hte - a(hre) + (44.9 –6.55 log hte)log d + C • C is a correction factor – C = 0 dB in dense urban; -5 dB in urban; -10 dB in suburban; -17 dB in rural • Note: fc is in MHz (between 1500 and 2000 MHz), d is in km, hte is effective base station antenna height in meters (between 30 and 200m), hre is mobile antenna height (between 1 and 10m) TI -1011

35 Path Loss Models for Microcellular Areas
Area of the microcell spans from 1m to a kilometer Supported by below the roof top antennas mounted on lampposts Streets acts as urban canyons Propagation of the signal is affected by reflection from buildings and ground Scattering from vehicles Diffraction around building and rooftops Bertoni and others have developed empirical path-loss models similar to Okumura-Hata models See table 2.2 in the text book for the Path-loss models TI -1011

36 Path Loss Models for Microcellular Areas
d is the distance between the mobile and the transmitter in Kilometers hb is the height of the base station hm is the height of the mobile fc is the centre frequency of the carrier in GHz and ranges between GHz In addition other parameters are rh, the distance of the mobile from the last rooftop in meters Δhm is the height of the nearest building above the height of the receiver Δh is the relative height of the base station compared to the average height of the buildings TI -1011

37 Path Loss Models for Picocellular Indoor Areas
Picocells correspond to radio cells covering a building or parts of a building Area of picocells spans from 30m to 100m Employed for WLANs, Wireless PBX systems and PCS operating in indoor areas Three models for Indoor Areas Multifloor Attenuation Model JTC Model => improvement to the Multifloor Attenuation Model Partition Dependant Model TI -1011

38 Multifloor Attenuation Model
Describing path loss in multistory building Signal Attenuation by the floors is a constant independent of distance The path loss is; Lp=L0 + nF+ 10 log (d) F is the signal attenuation provided by each floor L0 is the path loss at first meter, L0 = 10 log (Pt) – 10 log (P0) d is the distance between the Tx and the Rx in meters n is the number of floors through which the signal passes For indoor measurements at 900 MHz and 1.7 GHz, F=10dB and 16 dB TI -1011

39 JTC Model Lp= A + Lf (n) + B log (d) + X
• A is an environment dependent fixed loss factor (dB) • B is the distance dependent loss coefficient • d is separation distance between the base station and portable, in meters • Lf is a floor penetration loss factor (dB) • n is the number of floors between the access point and mobile terminal • Xσ is a shadowing term TI -1011

40 JTC Model (cont.) TI -1011

41 Partition Loss Model Fixing the value of the Path Loss gradient α = 2 for free space Introducing the losses for each partition mtype = the number of partitions of type wtype = the loss in dB associated with that partition d = distance between transmitter and receiver point in meter X = the shadow fading L0 = the path loss at the first meter, computed by where d0 = 1 m. f = operating frequency of the transmitter TI -1011

42 Partition Loss Model TI -1011

43 THE END TI -1011


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