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Mobile Communications

Learn about antenna radiation, propagation models, free space loss, and practical models in wireless communications systems. Explore channel codes, signal propagation, and channel models for digital communication.

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Mobile Communications

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  1. Mobile Communications Part IV- Propagation Characteristics Professor Z Ghassemlooy Faculty of Engineering and Environment University of Northumbria U.K. http://soe.unn.ac.uk/ocr

  2. Contents • Radiation from Antenna • Propagation Model (Channel Models) • Free Space Loss • Plan Earth Propagation Model • Practical Models • Summary

  3. Channel code word Message Signal Modulated Transmitted Signal Source Encoder Channel Encoder Mod- ulator Source Wireless Channel Source Decoder Channel Decoder Demod- ulator User Received Signal Estimate of Message signal Estimate of channel code word Wireless Communication System

  4. Basic Questions Tx: • What will happen if the transmitter • changes transmit power ? • changes frequency ? • operates at higher speed ? Channel: What will happen if we conduct this experiment in different types of environments? Desert Metro Street Indoor Rx: What will happen if the receiver moves?

  5. H E d Pt d Area Distance d Antenna - Ideal • Isotropics antenna: In free space radiates power equally in all direction. Not realizable physically EM fields around a transmitting antenna , a polar coordinate • d- distance directly away from the antenna. •  is the azimuth, or angle in the horizontal plane. •  is the zenith, or angle above the horizon.

  6. Antenna - Real • Not isotropic radiators, but always have directive effects (vertically and/or horizontally) • A well defined radiation pattern measured around an antenna • Patterns are visualised by drawing the set of constant-intensity surfaces

  7. /4 /2 y y z simple dipole x z x side view (xy-plane) side view (yz-plane) top view (xz-plane) Antenna – Real - Simple Dipoles • Not isotropic radiators, e.g., dipoles with lengths /4 on car roofs or /2 as Hertzian dipole • Example: Radiation pattern of a simple Hertzian dipole shape of antenna is proportional to the wavelength Largest dimension of the antenna La = /2

  8. y y z Directed x z x side view (xy-plane) side view (yz-plane) top view (xz-plane) z z Sectorized x x top view, 3 sector top view, 6 sector Antenna – Real - Sdirected and Sectorized • Used for microwave or base stations for mobile phones (e.g., radio coverage of a valley)

  9. Note: the area is for a sphere. W/m2 • Gt is the transmitting antenna gain • The product PtGt : Equivalent Isotropic Radiation Power (EIRP) which is the power fed to a perfect isotropic antenna to get the same output power of the practical antenna in hand. Antenna - Ideal - contd. • The power density of an ideal loss-less antenna at a distance d away from the transmitting antenna is:

  10. V/m Antenna - Ideal - contd. • The strength of the signal is often defined in terms of its Electric Field Intensity E, because it is easier to measure. Pa = E2/Rm where Rm is the impedance of the medium. For free space Rm = 377 Ohms..

  11. Antenna - Ideal - contd. • The receiving antenna is characterized by its effective aperture Ae, which describes how well an antenna can pick up power from an incoming electromagnetic wave • The effective aperture Ae is related to the gain Gras follows: Ae = Pr / Pa =>Ae = Gr2/4 which is the equivalent power absorbing area of the antenna. Gr is the receiving antenna gain and  = c/f

  12. Signal Propagation (Channel Models)

  13. Basic Digital Communication System Model x(t) Input data Pulse generator TX filter channel Hc(f) HT(f) + Channel noise n(t) + Tb: Symbol period Receiver filter A/D y(t) Output data HR(f)

  14. Fourier Representation of Periodic Signals 1 1 0 0 t t ideal periodic signal real composition (based on harmonics)

  15. Signals II • Different representations of signals • amplitude (amplitude domain) • frequency spectrum (frequency domain) • phase state diagram (amplitude M and phase  in polar coordinates) • Composite signals mapped into frequency domain using Fourier transformation • Digital signals need • infinite frequencies for perfect representation • modulation with a carrier frequency for transmission (->analog signal!) Q = M sin  A [V] A [V] t[s]  I= M cos   f [Hz]

  16. Channel Models • High degree of variability (in time, space etc.) • Large signal attenuation • Non-stationary, unpredictable and random • Unlike wired channels it is highly dependent on the environment, time space etc. • Modelling is done in a statistical fashion • The location of the base station antenna has a significant effect on channel modelling • Models are only an approximation of the actual signal propagation in the medium. • Are used for: • performance analysis • simulations of mobile systems • measurements in a controlled environment, to guarantee repeatability and to avoid the expensive measurements in the field.

  17. Channel Models - Classifications • System Model - Deterministic • Propagation Model- Deterministic • Predicts the received signal strength at a distance from the transmitter • Derived using a combination of theoretical and empirical method. • Stochastic Model -Rayleigh channel • Semi-empirical (Practical +Theoretical) Models

  18. Channel Models - Linear Finite delay Constant • Therefore for a linear channel is: y(t) = kx(t-td) Linear channel h(t) H(f) x(t) No Noise Amplitude distortion Phase distortion • The phase delay Describes the phase delayed experienced by each frequency component

  19. This can be modelled as an • ideal low pass filter • non-ideal low pass filter • This smears the transmitted signal x(t) in time causing the effect of a symbol to spread to adjacent symbols when a sequence of symbols are transmitted. • The resulting interference, intersymbol interference (ISI), degrades the error performance of the communication system. Channel

  20. RMS Delay Spread () = 46.4 ns Mean Excess delay () = 45 ns Maximum Excess delay < 10 dB = 110 ns Power Delay Profile -90 -90 -95 Received Signal Level (dBm) -100 Noise threshold -105 0 50 100 150 200 250 300 350 400 450 Excess delay (ns)

  21. 4.38 µs 1.37 µs Power Delay Spread - Example Pr() 0 dB -10 dB -20 dB -30 dB  0 1 2 5 (µs)

  22. Channel Models – Multipath Link • The mathematical model of the multipath can be presented using the method of the impulse response used for studying linear systems. y(t) = kx(t-td) y(n)= kx(n-N) x(t) = (t) x(n)= (n) Linear channel h(t) H(f) h(n) Channel is usually modeled as Tap-Delay-Line

  23. Channel Models – Multipath Link • Time variable multi-path channel impulse response Where a(t-)= attenuated signal • Time invariant multi-path channel impulse response • Each impulse response is the same or has the same statistics, then Where aie(.)= complex amplitude (i.e., magnitude and phase) of the generic received pulse.  = propagation delay generic ith impulse N = number signal arriving from N path (.) = impulse signal (delta function)

  24. Channel Models – Multipath Link • Channel transfer function • Multipath Time • Mostly used to denote the severity of multipath conditions. • Defined as the time delay between the 1st and the last received impulses. • Coherence bandwidth - on average the distance between two notches Bc ~ 1/TMP

  25. Freq. domain view RMS delay spread Range of freq over which response is flat Bc Time domain view For 0.9 correlation For 0.5 correlation High correlation of amplitude between two different freq. components

  26. 4.38 µs 1.37 µs Power Delay Spread - Example Pr() 0 dB -10 dB -20 dB -30 dB  0 1 2 5 (µs) Signal bandwidth for Analog Cellular = 30 KHz Signal bandwidth for GSM = 200 KHz

  27. Multipath Delay • With a 52 meter separation, in a LOS environment, a large 753.5 ns excess delay • NLOS excess delay over 423 meters extended to 1388.4 ns. • Office building: RMS delay spread = 10-60 ns

  28. Inter-symbol interference (ISI) • Channel is band limited innature • Limited frequency response  unlimited time response • Channel has multipath • Tx filter – • There are two major ways to mitigate the detrimental effect of ISI. • The first method is to design bandlimited transmission pulses (i.e., Nyquist pulses) which minimize the effect of ISI. • Equalization BS 2 1 0 Building MU

  29. Symbol time 4.38 µs ISI Pr() 0 dB -10 dB -20 dB  -30 dB  0 1 2 5 (µs) 0 1 2 5 (µs) 4.38 Symbol time > 10*  --- No equalization required Symbol time < 10*  --- Equalization will be required to deal with ISI In the above example, symbol time should be more than 14µs to avoid ISI. This means that link speed must be less than 70Kbps (approx)

  30. Propagation Path Loss • The propagation path loss is LPE = LaLlf Lsf where Lais average path loss (attenuation): (1-10 km), Llf - long term fading (shadowing): 100 m ignoring variations over few wavelengths, Lsf- short term fading (multipath): over fraction of wavelength to few wavelength. • Metrics (dBm, mW) [P(dBm) = 10 * log[ P(mW) ]

  31. Thus the free space propagation path loss is defined as: Propagation Path Loss – Free Space • Power received at the receiving antenna at far field only • Isotropic antenna has unity gain (G = 1) for both transmitter and receiver.

  32. The difference between two received signal powers in free space is: Propagation - Free Space–contd. If d2 = 2d1, the P = -6 dB i.e 6 dB/octave or 20 dB/decade

  33. Propagation - Non-Line-of-Sight • Generally the received power can be expressed as: Pr d-v • For line of sight v = 2, and the received power Pr d-2 • Average v over all NLOS could be 4 - 6. • For non-line of sight with no shadowing, received power at any distance d can be expressed as: 100 m< dref < 1000 m

  34. Propagation - Non-Line-of-Sight • Log-normal Shadowing Where Xσ: N(0,σ) Gaussian distributed random variable

  35. -70 -80 -90 v = 2,Free space -100 Received power (dBm) -110 City and urban areas v = 3Rural areas -120 v = 4, -130 -135 0 10 20 30 40 50 Distance (km) Received Power for Different Value of Loss Parameter v

  36. In terms of frequency f and the free space velocity of electromagnetic wave c = 3 x 108 m/s it is: Expressing frequency in MHz and distance d in km: Propagation Model- Free Space

  37. BS MU Propagation Model- Free Space (non-ideal, path loss) • Non-isotropic antenna gain  unity, and there are additional lossesLad , thus the power received is: d > 0 and L 0 Thus for Non-isotropic antennathe path loss is: Note: Interference margin can also be added

  38. Propagation Model- Free Space (non-ideal, path loss) • Considering loss S due to shadowing

  39. Propagation Model - Mechanisms • Reflection • Diffraction • Scattering Source: P M Shankar

  40. d dd Direct path (line of sight) hb hm Ground reflected path dr Channel Model- Plan Earth Path Loss - 2 Ray Reflection • In mobile radio systems the height of both antennas (Tx. and Rx.) <<d (distance of separation) From the geometrydd = [d2 + (hb - hm )2]

  41. Using the binomial expansion Note d >> hb or hm. Similarly The phase difference Channel Model- Plan Earth Path Loss- contd. The path differenced = dr - dd = 2(hbhm )/d

  42. Channel Model- Plan Earth Path Loss– contd. Total received power Where  is the reflection coefficient. For  = -1 (low angle of incident) and .

  43. Therefore: Assuming that d >> hm or hb, then sin x = x for small x Thus which is 4th power law Channel Model- Plan Earth Path Loss– contd.

  44. Propagation path loss (mean loss) In a more general form (no fading due to multipath), path attenuation is Channel Model- Plan Earth Path Loss– contd. Compared with the free space = Pr= 1/ d2 • LPE increases by 40 dB each time d increases by 10

  45. Channel Model- Plan Earth Path Loss– contd. • Including impedance mismatch, misalignment of antennas, pointing and polarization, and absorption The power ration is: where Gt(θt,φt) = gain of the transmit antenna in the direction (θt,φt) of receive antenna. Gr(θr,φr) = gain of the receive antenna in the direction (θr,φr) of transmit antenna. Γt and Γr = reflection coefficients of the transmit and receive antennas at and ar = polarization vectors of the transmit and receive antennas α is the absorption coefficient of the intervening medium.

  46. LOS Channel Model - Problems • Simple theoretical models do not take into account many practical factors: • Rough terrain • Buildings • Refection • Moving vehicle • Shadowing Thus resulting in bad accuracy Solution:Semi- empirical Model

  47. Outdoor Indoor Sem-iempirical Model Practical models are based on combination of measurement and theory. Correction factors are introduced to account for: • Terrain profile • Antenna heights • Building profiles • Road shape/orientation • Lakes, etc. • Okumura model • Hata model • Saleh model • SIRCIM model Y. Okumura, et al, Rev. Elec. Commun. Lab., 16( 9), 1968. M. Hata, IEEE Trans. Veh. Technol., 29, pp. 317-325, 1980.

  48. Okumura Model • Widely used empirical model (no analytical basis!) in macrocellular environment • Predicts average (median) path loss • “Accurate” within 10-14 dB in urban and suburban areas • Frequency range: 150-1500 MHz • Distance: > 1 km • BS antenna height: > 30 m. • MU antenna height: up to 3m. • Correction factors are then added.

  49. Hata Model • Consolidate Okumura’s model in standard formulas for macrocells in urban, suburban and open rural areas. • Empirically derived correction factors are incorporated into the standard formula to account for: • Terrain profile • Antenna heights • Building profiles • Street shape/orientation • Lakes • Etc.

  50. Hata Model – contd. • The loss is given in terms of effective heights. • The starting point is an urban area. The BS antennae is mounted on tall buildings. The effective height is then estimated at 3 - 15 km from the base of the antennae. P M Shankar

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