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STOCHASTIC MODELING OF COMPLEX ENVIRONMENTS FOR WIRELESS SIGNAL PROPAGATION Massimo Franceschetti
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MOTIVATION No simple solution for complex environments
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Stochastic approximation of the environment Few parameters Simple analytical solutions The true logic of this world is in the calculus of probabilities. James Clerk Maxwell WHY RANDOM MEDIA ?
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WAVE APPROACH RAY APPROACH [1] G. Franceschetti, S. Marano, and F. Palmieri, “Propagation without wave equation, toward an urban area model,” IEEE Trans. Antennas and Propagation, vol 47, no 9, pp. 1393-1404, Sept 1999 [2] M. Franceschetti, J. Bruck, and L. Schulman, “A random walk model of wave propagation,” IEEE Trans. Antennas and Propagation, vol 52, no 5, pp. 1304-1317, May 2004 STOCHASTIC MODELS
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x y x y MODEL 1. Percolation Theory Do we measure a non-zero field inside the city ?
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(yes if p > p c 0.5972 in 2D ) G.Grimmet, Percolation. New York: Springer-Verlag, 1989 SUBCRITICAL PHASE SUPERCRITICAL PHASE propagation not allowedpropagation allowed 4.0p 6.0p MODEL 1. Percolation Theory is propagation possible?
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Reflection ( Snell law ) R A Y A P P R O A C H (E,H)(E,H) Diffraction Scattering and bsorption Refraction MODEL 1. Propagation Mechanism
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1 2 3 … N-1 N 0 1 2 3 … N 0
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Pr{cell (j, i) is occupied} = f(j) = q j =1–p j. p j =p=0.7p j = p τj p = 0.6τ = 0.2 MODEL 1. Extension to inhomogeneous grid j=1 j=2 j=n
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Stochastic process rnrn MODEL 1. Mathematical formulation
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1 2 3 … N-1 N 0 1 2 3 … N 0 MODEL 1. Mathematical formulation
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Assume: x m indep. RV’s MARTINGALE THEORY
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MODEL 1. Mathematical formulation
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p ej + = p j tanθ · p j+1 q ej + = 1 - p ej + = 1 - p j tanθ · p j+1 MODEL 1. Mathematical formulation
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General formula for any obstacle density profile q j =1-p j not only the uniform grid j=1 j=2 j=n
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suburbs city center x y TX RX MODEL 1. Application: macrocells x y
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Exponential profile 0x0x MODEL 1. Application L
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MODEL 1. Ray tracing validation ERROR ANALYSIS:
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MODEL 1. Validation Analytical solution
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BUILDING PROFILE: INCREASING EXPONENTIAL BUILDING PROFILE: DECREASING EXPONENTIAL MODEL 1. Validation ERROR PLOTS
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[1] G. Franceschetti, S. Marano, and F. Palmieri, “Propagation without wave equation, toward an urban area model,” IEEE Trans. Antennas and Propagation, vol 47, no 9, pp. 1393-1404, Sept 1999 [2] S. Marano, F. Palmieri, G. Francescehetti, “Statistical characterization of wave propagation in a random lattice,” J. Optic Soc. Amer., vol 16, no 10, pp. 2459-2464, 1999. PERCOLATION MODEL REFERENCES [3] S. Marano, M. Franceschetti, “Ray propagation in a random lattice, a maximum entropy, anomalous diffusion process,” IEEE Trans. Antennas and Propagation, second revision due, 2004. [4] M. Conci, A. Martini, M. Franceschetti, and A. Massa. “Wave propagation in non-uniform random lattices,” Preprint, 2004. Homogeneous lattice pj=p Source inside lattice Inhomogeneous lattice profiles
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MODEL 2. Random walks DIFFUSIVE OBSTACLES A low transmitting antenna is immersed in an environment of small scatterers
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MODEL 2. Application: microcells
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Emitted power envelope: density of photons spreading isotropically in the environment MODEL 2. Mathematical formulation Pdf of a photon hitting an obstacle at r Each photon walks straight for a random length Stops with probability Turns in a random direction with probability RANDOM WALK FORMULATION
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MODEL 2. Mathematical formulation Amount of clutter Amount of absorption
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Channel Impulse waveform Time spread Time delay Attenuation MODEL 2. Power delay profile
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R is total path length in n steps r is the final position after n steps o r |r 0 | |r 1 | |r 2 | |r 3 | c is the speed of light MODEL 2. Power delay profile
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MODEL 2. Joint probabilty computation
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Can solve also this analytically ! MODEL 2. Power delay profile computation
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Coherent response Incoherent response Exponential tail MODEL 2. Results
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MODEL 2. Tail of the response Exponential decay in time and distance
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1m 0.95 T ~ 1nsec R ~ 6 m MODEL 2. Validation
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RANDOM WALK REFERENCES [1] M. Franceschetti, J. Bruck, and L. Schulman, “A random walk model of wave propagation,” IEEE Trans. Antennas and Propagation, vol 52, no 5, pp. 1304-1317, May 2004. [2] M. Franceschetti, “Stochastic rays pulse propagation,” IEEE Trans. Antennas and Propagation, to appear, October 2004. Path Loss Impulse power delay profile
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CONCLUSION Finding the quality of being intricate and compounded Modeling complex propagation environments
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