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Lecture 2 - EE 359: Wireless Communications - Fall 2009
Signal Propagation. Path Loss Models.
Lecture Outline
ā€¢ Overview of Signal Propagation
ā€¢ Free Space Path Loss Model
ā€¢ Ray Tracing Path Loss Models
ā€¢ Simpliļ¬ed Path Loss Model
ā€¢ Empirical Path Loss Models
1. Signal Propagation Characteristics:
ā€¢ Path loss: power falloļ¬€ relative to distance
ā€¢ Shadowing: random ļ¬‚uctuations due to obstructions
ā€¢ Flat and frequency selective fading: caused by multipath
2. Transmitted and received signals:
ā€¢ Transmitted Signal:, with power Pt, is s(t) = {u(t)ej(2Ļ€fct)} = sI(t) cos(2Ļ€fct + Ļ†0) āˆ’
sQ(t) sin(2Ļ€fct + Ļ†0), where u(t) = sI(t) + jsQ(t) is the complex baseband signal with band-
width B, fc is the carrier frequency, and Ļ†0 is the initial phase. For simplicity we assume u(t)
real for propagation model analysis.
ā€¢ Received signal:r(t) = {v(t)ej(2Ļ€fct)}, where v(t) = u(t)āˆ—c(t) for c(t) the baseband channel
model.
ā€¢ Doppler frequency shift fD = (v/Ī») cos(Īø) may also be introduced in the received signal
3. Free space path loss model:
ā€¢ Typically used for unobstructed LOS signal path.
ā€¢ Received signal is
r(t) = {
u(t)
āˆš
GlĪ»ej2Ļ€d/Ī»
4Ļ€d
ej(2Ļ€fct+Ļ†0)
}
with received power
Pr = Pt
āˆš
GlĪ»
4Ļ€d
2
.
ā€¢ Power falls oļ¬€ proportional to the ratio of wavelength over distance squared. The inverse
frequency dependence is due to the eļ¬€ective aperture of the receiver.
ā€¢ Power falls oļ¬€ proportional to net antenna gain Gl.
ā€¢ Model not accurate for general environments.
4. Ray tracing approximation:
ā€¢ Represent wavefronts as simple particles.
ā€¢ Simplest models only determine reļ¬‚ections.
ā€¢ Scattering and defraction can also be included.
5. Two path model:
ā€¢ One LOS path, one reļ¬‚ected path.
ā€¢ At small distances, power falls oļ¬€ proportional to d2 (free space loss on both paths).
ā€¢ Above some critical distance dc, received power given by
Pr ā‰ˆ Pt
āˆš
Glhthr
d2
2
.
ā€¢ Above dc, power falls oļ¬€ proportional to d4 and is independent of signal wavelength (frequency)
ā€¢ Model not generally accurate for cities or indoors.
6. General Ray Tracing:
ā€¢ Incorporates all signal components: reļ¬‚ections, scattering, and diļ¬€raction.
ā€¢ Reļ¬‚ected rays have power falloļ¬€ proportional to d2 by free space path loss model. Scattered
and refracted rays have power falloļ¬€ that depends on exact distance of scattering or refractive
object from transmitter and receiver.
ā€¢ If objects are more than a few wavelengths from receiver, typically neglect scattering and
refraction.
ā€¢ Most computer packages for channel simulation in indoor/outdoor environments use general
ray tracing for path loss.
ā€¢ Model requires detailed site information.
7. Simpliļ¬ed path loss model:
ā€¢ Capture main characteristics of ray tracing using simpliļ¬ed model Pr = PtK d0
d
Ī³
, where K
is a constant factor (Pr(d0)/Pt), d0 is a reference distance, and Ī³ is the path loss exponent.
ā€¢ Path loss exponent is function of carrier frequency, environment, obstructions, etc. Typically
ranges from 2 to 8 (at around 1 GHz).
ā€¢ Model captures main characteristics of ray tracing: good for high-level analysis.
8. Empirical Models:
ā€¢ Irregular terrain, like in cities, doesnā€™t lend itself to simple analytical path loss models.
ā€¢ Empirical path loss models based on extensive measurements.
ā€¢ Local mean attenuation: empirical measurements of local received power.
ā€¢ Okumura Model: Empirical model for irregular terrain.
ā€¢ Hata Model: Analytical approximation to Okumura model.
ā€¢ Cost 231 Extension to Hata Model: Extends Hata model to 2 GHZ and to lower mobile
antenna heights. Widely used in 2G simulations.
ā€¢ Piecewise linear models capture multiple slopes associated with path loss.
ā€¢ Models not accurate and donā€™t generalize well to other environments.
Main Points
ā€¢ Path loss models simplify Maxwellā€™s equations. The models vary in complexity and accuracy.
ā€¢ Power fallof with distance is proportional to d2 in free space model, d4 in two path model.
ā€¢ General ray tracing requires detailed site speciļ¬c information. Typically generated with computer
packages.
ā€¢ Main characteristics of ray tracing models captured in simpliļ¬ed path loss model.
ā€¢ Empirical models widely used to study cellular system performance via simulation. Typically
awkward for analysis.

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Signal propagation. path loss models

  • 1. Lecture 2 - EE 359: Wireless Communications - Fall 2009 Signal Propagation. Path Loss Models. Lecture Outline ā€¢ Overview of Signal Propagation ā€¢ Free Space Path Loss Model ā€¢ Ray Tracing Path Loss Models ā€¢ Simpliļ¬ed Path Loss Model ā€¢ Empirical Path Loss Models 1. Signal Propagation Characteristics: ā€¢ Path loss: power falloļ¬€ relative to distance ā€¢ Shadowing: random ļ¬‚uctuations due to obstructions ā€¢ Flat and frequency selective fading: caused by multipath 2. Transmitted and received signals: ā€¢ Transmitted Signal:, with power Pt, is s(t) = {u(t)ej(2Ļ€fct)} = sI(t) cos(2Ļ€fct + Ļ†0) āˆ’ sQ(t) sin(2Ļ€fct + Ļ†0), where u(t) = sI(t) + jsQ(t) is the complex baseband signal with band- width B, fc is the carrier frequency, and Ļ†0 is the initial phase. For simplicity we assume u(t) real for propagation model analysis. ā€¢ Received signal:r(t) = {v(t)ej(2Ļ€fct)}, where v(t) = u(t)āˆ—c(t) for c(t) the baseband channel model. ā€¢ Doppler frequency shift fD = (v/Ī») cos(Īø) may also be introduced in the received signal 3. Free space path loss model: ā€¢ Typically used for unobstructed LOS signal path. ā€¢ Received signal is r(t) = { u(t) āˆš GlĪ»ej2Ļ€d/Ī» 4Ļ€d ej(2Ļ€fct+Ļ†0) } with received power Pr = Pt āˆš GlĪ» 4Ļ€d 2 . ā€¢ Power falls oļ¬€ proportional to the ratio of wavelength over distance squared. The inverse frequency dependence is due to the eļ¬€ective aperture of the receiver. ā€¢ Power falls oļ¬€ proportional to net antenna gain Gl. ā€¢ Model not accurate for general environments.
  • 2. 4. Ray tracing approximation: ā€¢ Represent wavefronts as simple particles. ā€¢ Simplest models only determine reļ¬‚ections. ā€¢ Scattering and defraction can also be included. 5. Two path model: ā€¢ One LOS path, one reļ¬‚ected path. ā€¢ At small distances, power falls oļ¬€ proportional to d2 (free space loss on both paths). ā€¢ Above some critical distance dc, received power given by Pr ā‰ˆ Pt āˆš Glhthr d2 2 . ā€¢ Above dc, power falls oļ¬€ proportional to d4 and is independent of signal wavelength (frequency) ā€¢ Model not generally accurate for cities or indoors. 6. General Ray Tracing: ā€¢ Incorporates all signal components: reļ¬‚ections, scattering, and diļ¬€raction. ā€¢ Reļ¬‚ected rays have power falloļ¬€ proportional to d2 by free space path loss model. Scattered and refracted rays have power falloļ¬€ that depends on exact distance of scattering or refractive object from transmitter and receiver. ā€¢ If objects are more than a few wavelengths from receiver, typically neglect scattering and refraction. ā€¢ Most computer packages for channel simulation in indoor/outdoor environments use general ray tracing for path loss. ā€¢ Model requires detailed site information. 7. Simpliļ¬ed path loss model: ā€¢ Capture main characteristics of ray tracing using simpliļ¬ed model Pr = PtK d0 d Ī³ , where K is a constant factor (Pr(d0)/Pt), d0 is a reference distance, and Ī³ is the path loss exponent. ā€¢ Path loss exponent is function of carrier frequency, environment, obstructions, etc. Typically ranges from 2 to 8 (at around 1 GHz). ā€¢ Model captures main characteristics of ray tracing: good for high-level analysis. 8. Empirical Models: ā€¢ Irregular terrain, like in cities, doesnā€™t lend itself to simple analytical path loss models. ā€¢ Empirical path loss models based on extensive measurements. ā€¢ Local mean attenuation: empirical measurements of local received power. ā€¢ Okumura Model: Empirical model for irregular terrain.
  • 3. ā€¢ Hata Model: Analytical approximation to Okumura model. ā€¢ Cost 231 Extension to Hata Model: Extends Hata model to 2 GHZ and to lower mobile antenna heights. Widely used in 2G simulations. ā€¢ Piecewise linear models capture multiple slopes associated with path loss. ā€¢ Models not accurate and donā€™t generalize well to other environments. Main Points ā€¢ Path loss models simplify Maxwellā€™s equations. The models vary in complexity and accuracy. ā€¢ Power fallof with distance is proportional to d2 in free space model, d4 in two path model. ā€¢ General ray tracing requires detailed site speciļ¬c information. Typically generated with computer packages. ā€¢ Main characteristics of ray tracing models captured in simpliļ¬ed path loss model. ā€¢ Empirical models widely used to study cellular system performance via simulation. Typically awkward for analysis.