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A Survey of Various Propagation Models for Mobile Communication
Tapan K Sarkar, Zhong Ji, Kyungjung Kim, Abdellatif Medouri, and Magdalena Salazar-Palma IEEE Antenna and Propagation Magazine, Vol. 45, No. 3, June 2003 Presented by Lu-chuan Kung
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Outline Mobile radio propagation Models for Path Loss
Empirical (statistical) models Site-specific (deterministic) models Models for Small-scale Fading Impulse-Response Models
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Mobile Radio Propagation
EM wave Radio Wave Propagation: Reflection Diffraction Scattering Multi-path channel impulse response
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Basic Definitions Path Loss Power-Delay Profile
Friis free-space equation Metrics (dBm, mW) P(dBm) = 10 * log[ P(mW) ] Power-Delay Profile Take spatial average of |hb(t;τ)|2 over a local area
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Basic Definitions Time-Delay Spread First-arrival delay (τA)
Mean excess delay RMS delay
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Inter-symbol Interference
Slide from R. Struzak
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Basic Definitions Coherence Bandwidth Doppler spread Coherence Time
Range of frequency over which channel is “flat” Relation to delay spread Doppler spread Measure spectral broadening caused by motion of the mobile Coherence Time Time duration over which channel impulse response is invariant
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Models of Path Loss Log-distance Path Loss Model Log-normal Shadowing
Xσ: N(0,σ) Gaussian distributed rv
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Models for Path Loss Empirical Models
Okumura Model L50: median of propagation path loss LF: free-space propagation loss Amu(f,d): median attenuation G(hte), G(hre): gain factors for BS and mobile antenna GAREA: environment gain Applicable frequncies: 150 MHz to 1920 MHz (typically is extrapolated up to 3000 MHz) Disadvantage: slow response to rapid changes in terrain
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Models for Path Loss Empirical Models
Dual-slope model P1=PL(d0): the path loss at d0 dbrk: Fresnel breakpoint Lb: basic transmission-loss parameter n1,n2: slopes of the best-fit line before and after dbrk
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Models for Path Loss Empirical Models: Indoor Case
Indoor Log-distance path loss model FAF(q): floor attenuation factor WAF(p): wall attenuation factor
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Models for Path Loss Empirical Models: Indoor Case
Indoor Log-distance path loss model γ ranges from 1.5 to 4 γ depends on frequency and building materials
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Site-specific Path Loss Models Ray-tracing
Ray-tracing Technique Assume energy is radiated through infinitesimally small tubes, often called rays Model signal propagation via ray propagation
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Ray-tracing Technique: Image Method
Images of a source serve as secondary sources N reflecting planes N first-order images N(N-1) two-reflection images N(N-1)(N-1) three-reflection images Efficient but cannot handle complex environments
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Ray-tracing Technique: Brute-force Method
Considers a bundle of transmitted rays Generates reflecting and refracting rays when hits an object Generates a family of diffracting rays when hits a wedge
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Ray-tracing Model 2-D Ray-tracing model 3-D model
Each ray is a ray sector of sector angle φ Smallerφprovides higher accuracy 3-D model Each ray tube occupy the same solid angle Antenna patterns are incorporated
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Site-specific Path Loss Model: FDTD Models
Ray-tracing fails for complex lossy structures with finite dimentions Finite-Difference Time-Domain (FDTD) method Solve Maxwell’s equations numerically Complete solution for all points in the map Requires large computational resources
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Site-specific Path Loss Model: Artificial Neural-Network Models
Artificial Neural-Network Models (ANNs) Use neural network models to predict path loss from noisy measurements Pros: Better accuracy than statistical model Better computational efficiency than other site-specific models Cons: Slow convergence Unpredictable solutions during learning
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Models for Small-Scale Fading
Rayleigh fading Assume a large number of scattering sources By Central Limit Theorem, signal is a Gaussian rv with random phase between 0~2π The power (envelope) of this random Gaussian vector is Rayleigh distributed
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An Example of Rayleigh Fading
A typical Rayleigh fading envelope at 900MHz, mobile unit velocity = 120km/hr
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Models for Small-Scale Fading
Ricean Distribution A: peak amplitude of the dominant signal I0(): modified Bessel function of the first kind Add a dominant LOS signal to Rayleigh fading Ricean factor: K=A2/2σ2
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Models for Small-Scale Fading
Log-normal Fading m: median value σ: standard deviation
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Models for Small-Scale Fading
Suzuki Model Combines log-normal and Rayleight distributions
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Models for Small-Scale Fading
Nakagami Model r: envelope amplitutde Ω=<r2>: time-averaged power of received signal m: the inverse of normalized variance of r2 Get Rayleigh when m=1
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Impulse-Response Models
Complete characterization of the linear system Model the effect of multi-path fading Measurement-based Models Statistical Models Deterministic Models
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Impulse-Response Models Measurement-based Models:
Direct Pulse Measurement Minimum resolvable delay = probing pulse width Tbb Subject to interference and noise
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Impulse-Response Models: Measurement-based Models
Spread-spectrum Sliding Correlator
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Impulse-Response Models: Measurement-based Models
Swept-frequency measurements Pros: Provide both amplitude and phase information Cons: Require hardwired synchronization between TX and RX Need fast sweeping times but reduces time resolution
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Impulse-Response Models: Statistical Models
Two-ray Rayleigh Fading Model α1 & α2: independent Rayleigh r.v. θ1 & θ2 ~ Uni[0, 2π] τ: time delay between the two rays
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Impulse-Response Models: Statistical Models
SIRCIM Model Based on measurements at 1300MHz in 5 factory and other buildings Model power-delay profile as a piecewise function For LOS: For OBS:
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Conclusion With propagation models, we can
Provide installation guidelines Mitigate interference Design better wireless system
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