MMUST · EEE 5th YEAR · ANTENNA & RADIO WAVE PROPAGATION

Introduction to Radio Wave Propagation

Study Guide for 5th Year Undergraduate Electrical Engineering Students
Department of Electrical & Communication Engineering, Masinde Muliro University of Science and Technology

1. Learning Objectives

By the end of this unit, the student should be able to:

  1. Explain the nature of electromagnetic (radio) waves and the relationship between frequency, wavelength and velocity of propagation.
  2. Describe the three principal radio wave propagation mechanisms: free-space (line-of-sight), ground wave and sky wave (ionospheric) propagation.
  3. Identify the layers of the ionosphere and their role in HF long-distance communication.
  4. Apply the Friis free-space path loss equation and the plane-earth (two-ray) model to compute received signal power and path loss.
  5. Define and distinguish between large-scale path loss, shadowing and small-scale (multipath) fading.
  6. Relate the radio spectrum allocation (HF, VHF, UHF, SHF) to typical propagation behaviour and applications.
  7. Use path-loss calculators to predict link budgets in practical wireless systems.

2. Introduction

Radio wave propagation is the study of how electromagnetic (EM) waves travel from a transmitting antenna to a receiving antenna through the environment. It is the physical foundation of all wireless systems — broadcast radio and television, cellular mobile networks (2G–5G), Wi-Fi, satellite links, radar and Bluetooth.

Unlike guided media (copper cables, optical fibre), radio waves travel through an unbounded medium (free space, atmosphere, or a combination of media). Their behaviour depends strongly on:

Understanding propagation allows engineers to predict the received signal strength, design link budgets, choose antenna heights and locations, and plan cellular coverage.

Why it matters: A cellular operator must know how signal strength decays with distance to decide where to place base stations and how much transmit power is needed — all of which comes directly from propagation modelling.

3. Electromagnetic Wave Fundamentals

3.1 Maxwell's Equations — the origin of radio waves

A time-varying electric field produces a time-varying magnetic field, and vice versa. Maxwell's equations show that accelerating charges radiate energy that propagates through space as a self-sustaining electromagnetic wave. An antenna converts guided currents in a conductor into radiating EM waves (transmit mode) or vice versa (receive mode).

3.2 Wave relationship: frequency, wavelength and velocity

Fundamental wave equation c = f λ   ⇒   λ = c / f

where c = 3 × 108 m/s (speed of light in free space), f = frequency (Hz), λ = wavelength (m).

BandFrequencyWavelengthTypical use
MF300 kHz – 3 MHz1 km – 100 mAM broadcasting, ground wave
HF3 – 30 MHz100 – 10 mShort-wave radio, ionospheric (sky wave)
VHF30 – 300 MHz10 – 1 mFM radio, TV, land mobile
UHF300 MHz – 3 GHz1 m – 10 cmCellular, TV, Wi-Fi, GPS
SHF3 – 30 GHz10 – 1 cmSatellite, microwave links, 5G mmWave

3.3 Polarization

Polarization describes the orientation of the electric field vector as the wave travels:

Key point: A receive antenna must match the polarization of the incoming wave; a mismatch can cause up to total signal loss (cross-polar isolation).

3.4 Power density and antenna gain

Power density at distance d (isotropic radiator) S = Pt / (4π d²)   [W/m²]

An antenna concentrates power in preferred directions. Antenna gain G (relative to an isotropic radiator, dBi) raises the power density in the direction of maximum radiation:

S = (Pt Gt) / (4π d²) = EIRP / (4π d²)

where EIRP = PtGt is the Effective Isotropic Radiated Power.

3.5 Free-space received power

The effective aperture of a receive antenna is Ae = Gr λ² / (4π). Combining with the power density gives the Friis equation:

Friis free-space transmission equation Pr = Pt Gt Gr ( λ / (4π d) )²

Signal strength therefore falls with the square of distance in free space (20 dB per decade of distance).

4. Propagation Mechanisms

Radio energy reaches the receiver by three principal mechanisms. In practice a received signal is often a combination of several of them.

4.1 Ground Wave (Surface Wave) Propagation

4.2 Sky Wave (Ionospheric) Propagation

Ionospheric layerApprox. altitudeBehaviour
D60 – 90 kmPresent by day; absorbs MF/HF energy; disappears at night
E90 – 120 kmWeak reflection of HF; sporadic-E gives VHF reflection
F (F1 & F2)150 – 400 kmMain HF reflection region; merges at night
Why short-wave stations fade at dusk: at night the D-layer (which absorbs HF) disappears and the F-layer height changes, so the best reception frequency shifts down — hence short-wave broadcasters use different day/night frequencies.

4.3 Free-Space / Line-of-Sight (LOS) Propagation

Radio horizon distance (k = 4/3 earth-radius factor) dkm = 4.12 ( √ht + √hr ),   h in metres

4.4 Auxiliary mechanisms: reflection, diffraction, scattering

5. Path Loss Models

Path loss quantifies the reduction in signal power between transmitter and receiver, usually expressed in dB. Models range from ideal free space to empirical ones fitted to measurements.

5.1 Free-space path loss (FSPL)

Free-space path loss Lfs(dB) = 20 log₁₀(4π d / λ) = 20 log₁₀ dkm + 20 log₁₀ fMHz + 32.44

5.2 Plane-earth (two-ray) model

For propagation over a reflecting ground (mobile radio), a direct ray and a ground-reflected ray combine. At large distances the received power becomes approximately independent of wavelength:

Plane-earth received power Pr ≈ Pt Gt Gr ( ht² hr² ) / d⁴

giving a path loss of 40 dB per decade of distance — much steeper than free space — and an antenna-height gain of 6 dB per doubling of height.

5.3 Empirical models (Okumura–Hata)

Real-world models (Okumura curves, Hata equations, COST-231, 3GPP models) add corrections for frequency, antenna height, and environment (urban, suburban, rural, open). They are the working tools of cellular network planning.

Worked Example 1 — Free-space link. A transmitter radiates 10 W (40 dBm) at 900 MHz with Gt = Gr = 2 (3 dBi). Find the received power at 5 km in free space.
λ = 3×10⁸ / 9×10⁸ = 0.333 m.
Pr = PtGtGr(λ/4πd)² = 10 × 2 × 2 × (0.333 / (4π × 5000))² ≈ 2.25 × 10⁻⁸ W ≈ −76.5 dBm.
Worked Example 2 — Radio horizon. A base-station antenna is 30 m high and the mobile antenna 1.5 m high. Radio horizon = 4.12(√30 + √1.5) = 4.12(5.477 + 1.225) ≈ 27.6 km.

6. Fading, Shadowing and Multipath

6.1 Large-scale vs small-scale fading

EffectCauseVariation scaleMitigation
Path lossGeometric spreadingVery slow (km)Link budget, cell planning
Shadowing (slow fading)Buildings, hills blocking LOSSlow (metres – hundreds of m); log-normal distribution (~8 dB std dev in urban areas)Margins, macro-diversity, repeaters
Multipath fading (fast/small-scale)Reflected/diffracted copies arriving with different delays and phasesRapid (fractions of a wavelength, ~λ/2)Equalization, diversity, OFDM, Rake receivers, MIMO

6.2 Multipath parameters

Doppler shift fd = (v / c) fc cos θ

where θ is the angle between the mobile's direction of motion and the incoming wave.

6.3 Flat vs frequency-selective fading; Rayleigh & Rician statistics

7. The Radio Spectrum and Propagation Behaviour

BandPropagation characteristicRepresentative services
VLF / LF
< 300 kHz
Ground wave hugs earth; very stable; huge antennasSubmarine comms, navigation (Loran), time signals
MF
0.3 – 3 MHz
Ground wave by day; sky wave at night (D-layer gone)AM broadcasting (530 – 1700 kHz)
HF
3 – 30 MHz
Ionospheric hops; long-distance with modest power; variable with sunspot cycleShort-wave broadcast, amateur radio, aviation/maritime HF
VHF
30 – 300 MHz
LOS; diffraction over obstacles; tropospheric scattering at timesFM radio (88 – 108 MHz), TV, air traffic control, land mobile
UHF
300 MHz – 3 GHz
LOS; building penetration varies; cellular multipath fadingTV, cellular (700/900/1800/2100 MHz), Wi-Fi (2.4/5 GHz), GPS
SHF
3 – 30 GHz
LOS only; rain attenuation above ~10 GHz; high bandwidthSatellite (C/Ku/Ka), microwave backhaul, 5G mmWave, radar
EHF
> 30 GHz
Very short range; absorbed by atmosphere/rain; very wide bandwidths5G/6G research, automotive radar (77 GHz), imaging
Engineering trade-off: lower frequencies propagate farther and diffract around obstacles (good for coverage) but offer little bandwidth; higher frequencies offer wide bandwidths (high data rates) but need LOS and suffer rain/oxygen absorption. This trade-off drives every wireless standard's frequency choice.

8. Interactive Calculators & Visualization

8.1 Wavelength & Free-Space Path Loss Calculator

Results will appear here.

8.2 Radio Horizon & Two-Ray Model Calculator

Results will appear here.

8.3 Doppler Shift Calculator

Results will appear here.

9. Summary of Key Points

  1. Radio waves are EM waves obeying c = fλ; their propagation depends on frequency, distance, environment and atmosphere.
  2. Three principal mechanisms: ground wave (LF/MF), sky wave via ionosphere (HF), and line-of-sight / space wave (VHF and above).
  3. The ionosphere (D, E, F layers) enables long-range HF communication; MUF and critical frequency limit usable frequencies.
  4. Free-space path loss increases with 20 dB/decade of distance and 20 dB/decade of frequency (Friis equation).
  5. Over a reflecting ground the two-ray model gives 40 dB/decade decay — real mobile links decay much faster than free space predicts.
  6. Radio horizon d(km) = 4.12(√ht + √hr) governs LOS systems.
  7. Received signals experience path loss, log-normal shadowing and small-scale multipath fading (Rayleigh/Rician); delay spread and Doppler spread characterize the channel in frequency and time.
  8. Frequency choice trades coverage and penetration (low bands) against bandwidth and data rate (high bands).

10. Review Questions

  1. State the relationship between frequency, wavelength and velocity for a radio wave, and compute the wavelength of a 2.4 GHz Wi-Fi signal.
  2. Explain why AM (MW) broadcast stations can be heard far beyond their radio horizon at night, while FM (VHF) stations cannot.
  3. Describe the role of each ionospheric layer (D, E, F) in HF propagation.
  4. A transmitter operates at 1.8 GHz with 20 W output and antenna gains of 15 dBi at each end. Calculate the free-space received power at 10 km.
  5. Derive the 40 dB/decade distance dependence of the plane-earth (two-ray) model and explain its practical implication for cellular planning.
  6. Distinguish between shadowing and multipath fading, indicating the typical spatial scale of each.
  7. Define coherence bandwidth and coherence time, and state what each implies about a transmitted signal.
  8. A mobile moving at 90 km/h receives a 1.9 GHz signal arriving at 0° to its direction of motion. Compute the maximum Doppler shift.
  9. Compare the propagation characteristics of the UHF and SHF bands with respect to coverage, penetration and bandwidth, giving one application for each.
  10. Explain why vertical polarization is preferred for ground-wave propagation at MF.
Selected answers (click to reveal)

Q1: λ = c/f = 3×10⁸ / 2.4×10⁹ = 0.125 m (12.5 cm).

Q2: At night the absorbing D-layer disappears and MW signals reflect off the F-layer (sky wave), travelling hundreds of km. FM (VHF) is above the MUF, so the ionosphere is transparent to it — only LOS/diffraction remains.

Q4: λ = 0.167 m; Pr = 20 × 31.6 × 31.6 × (0.167/(4π·10⁴))² ≈ 1.4×10⁻⁷ W ≈ −68.5 dBm.

Q8: v = 25 m/s; fd = (25/3×10⁸) × 1.9×10⁹ = 158 Hz.