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EE359 – Lecture 2 Outline

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EE359 – Lecture 2 Outline. Announcements 1 st HW posted tomorrow, due next Thursday at 5pm. Discussion section starts next week (Monday) Lecture will end today at 10:30 Review of Last Lecture Signal Propagation Overview TX and RX Signal Models Complex baseband models Path Loss Models - PowerPoint PPT Presentation
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EE359 – Lecture 2 Outline Announcements 1 st HW posted by tonight, due next Friday at 5pm. Discussion section starts next week, day/time TBA TA OHs start next week (Thu 5-6 pm, Fri 1-2pm, Packard 109. Email OH : Thu 8-9 pm and Fri 10-11 am. Review of Last Lecture TX and RX Signal Models Path Loss Models Free-space and 2-Ray Models General Ray Tracing Simplified Path Loss Model
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Page 1: EE359 – Lecture 2 Outline

EE359 – Lecture 2 Outline

Announcements1st HW posted by tonight, due next Friday

at 5pm.Discussion section starts next week,

day/time TBATA OHs start next week (Thu 5-6 pm, Fri 1-

2pm, Packard 109. Email OH : Thu 8-9 pm and Fri 10-11 am.

Review of Last Lecture

TX and RX Signal ModelsPath Loss Models

Free-space and 2-Ray ModelsGeneral Ray TracingSimplified Path Loss ModelEmpirical ModelsmmWave Models

Page 2: EE359 – Lecture 2 Outline

Lecture 1 ReviewCourse InformationWireless VisionTechnical ChallengesCurrent/Next-Gen Wireless

SystemsSpectrum Regulation and

StandardsEmerging Wireless SystemsEmerging systems can be covered in a bonus lecture

Page 3: EE359 – Lecture 2 Outline

Propagation Characteristics

Path Loss (includes average shadowing)

Shadowing (due to obstructions)Multipath Fading

Pr/Pt

d=vt

PrPt

d=vt

v Very slow

SlowFast

Page 4: EE359 – Lecture 2 Outline

Path Loss ModelingMaxwell’s equations

Complex and impracticalFree space and 2-path models

Too simpleRay tracing models

Requires site-specific informationSimplified power falloff models

Main characteristics: good for high-level analysis

Empirical ModelsDon’t always generalize to other

environments

Page 5: EE359 – Lecture 2 Outline

Free Space (LOS) Model

Path loss for unobstructed LOS path

Power falls off :Proportional to 1/d2

Proportional to l2 (inversely proportional to f2) This is due to the effective aperature

of the antenna

d=vt

Page 6: EE359 – Lecture 2 Outline

Two Ray Model

Path loss for one LOS path and 1 ground (or reflected) bounce

Ground bounce approximately cancels LOS path above critical distance

Power falls off Proportional to d2 (small d)Proportional to d4 (d>dc) Independent of l (fc)

Two-path cancellation equivalent to 2-element array, i.e. the effective aperature of the receive antenna is changed.

Page 7: EE359 – Lecture 2 Outline

General Ray TracingModels signal components as

particlesReflectionsScatteringDiffraction

Requires site geometry and dielectric properties

Easier than Maxwell (geometry vs. differential eqns)Computer packages often used

Reflections generally dominate

10-ray reflection model explored in HW

Page 8: EE359 – Lecture 2 Outline

Simplified Path Loss Model

82,0

ddKPP tr

Used when path loss dominated by reflections.

Most important parameter is the path loss exponent , determined empirically.

Page 9: EE359 – Lecture 2 Outline

Empirical Channel Models

Cellular Models: Okumura model and extensions: Empirically based (site/freq specific), uses

graphsHata model: Analytical approximation to

OkumuraCost 231 Model: extends Hata to higher

freq. (2 GHz)Multi-slope modelWalfish/Bertoni: extends Cost 231 to

include diffraction

WiFi channel models: TGn Empirical model for 802.11n developed

within the IEEE tandards committee. Free space loss up to a breakpoint, then slope of 3.5. Breakpoint is empirically-based.

Commonly used in cellular and WiFi system simulations

Page 10: EE359 – Lecture 2 Outline

mmWave: What’s the big deal?

All existing commercial systems fit into a small fraction of the mmWave band

Page 11: EE359 – Lecture 2 Outline

mmWave Propagation (60-100GHz)

Channel models immatureBased on measurements, few accurate

analytical models Path loss proportion to l2 (huge) Also have oxygen and rain absorbtion

l is on the order of a water molecule

mmWave systems will be short range or require “massive MIMO”

mmWMassiveMIMO

Page 12: EE359 – Lecture 2 Outline

Main Points Path loss models simplify Maxwell’s

equations Models vary in complexity and

accuracy Power falloff with distance is

proportional to d2 in free space, d4 in two path model

Main characteristics of path loss captured in simple model Pr=PtK[d0/d]

Empirical models used in simulations

mmWave propagation models still immaturePath loss large due to frequency, rain,

and oxygen


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