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Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 [email protected]
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Page 1: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Lecture 3:Propagation Modelling

Anders Västberg

08-790 44 55

[email protected]

Page 2: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Ionospheric propagation

[Slimane]

Page 3: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Refraction in an ionospheric layer

[Slimane]

Page 4: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Electron density profile

[Slimane]

Page 5: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Ray paths

Page 6: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Cellular Networks

• Network organised in cells• Each access point has a set

of channels to service the users within the cell

• The set of channels can be reused when the signal to interference ratio is low enough.

Page 7: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Macrocells

• Give services in urban, suburban and rural areas. The cell radii varies from about 1 km to many tens of km.

• Few users per area unit.

• Base stations antennas are mounted on high buildings or on masts to get better coverage.

Page 8: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Microcells

• In urban or suburban areas• Cell radii is approximately 500 m• Very high traffic density (many users per

area unit).• Antennas mounted lower than the

buildings around it to decrease the cell coverage are

• More cells/unit area can services more users.

Page 9: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Indoor Cells (Picocells)

• High data rates and high traffic densities for both mobile and fixed users

• Coverage area influenced by– Layout of the building– Construction material (wood transparent to

radio waves, well reinforced concrete is not).– Shape of rooms

Page 10: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Propagation modelling

• To predict coverage areas in mobile cellular telephone systems, simple propagation models are needed.– Empirical methods– Physical models– Hybrid methods

Page 11: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Measurements

[Saunders, 1999]

Page 12: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Emperical methods

• Models are usually based on actual path loss measurements.– Curve fitting is used to obtain an analytical function for

the model.– Parameters are given by: distance, frequency,

antenna heights, distance to nearest building.

• Validity of the model may be limited (dependent on the environment)

• Models are practical and easy to use but not very accurate.

Page 13: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Physical Models

• A physical model needs a very detailed description of the terrain and other clutter.– Large amount of data needed.– Excessive computational effort needed.

• The important parameter for the macrocell designer is the area covered, not the field strength at particular locations.

Page 14: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Computerised Planning Tools

• The enormous increase in the need to plan cellular systems accurately and quickly

• The development of fast, affordable computing resources

• The development of geographical information systems

• Example:– TEMS CellPlanner, Ericsson AB

Page 15: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Empircal Models for Macro Cells

• Power Law models

• Clutter factor models

• Okumura-Hata model

• Cost 231-Hata Model

Page 16: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Plane Earth Loss

[Saunders, 1999]

Page 17: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Physical Models for Macro Cells

• Ikegami Model

• Rooftop diffraction

• Flat Edge model

• Walfisch-Bertoni model

• COST 231/Walfisch-Ikegami model

Page 18: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Models for Micro Cells

• Dual Slope model (empirical model)

• Physical Models– Two-ray model– Street canyon models– Non-line-of-sight models

Page 19: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Picocells

• Wall and floor factor models

• COST231 Multi-wall model

• Ericsson model

• COST 231 Line-of-sight model

• Floor Gain Models

• COST 231 Non-Line-of Sight model

Page 20: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Physical Model: Two Ray Model

[Saunders, 1999]

Page 21: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Two-Ray Model

2

21

221

4

1

r

eR

r

e

L

jkrjkr

R is the Fresnel reflection coefficient

Page 22: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Raytrace

[Saunders, 1999]

Page 23: Lecture 3: Propagation Modelling Anders Västberg 08-790 44 55 vastberg@kth.se.

Indoor models