- •Radio Engineering for Wireless Communication and Sensor Applications
- •Contents
- •Preface
- •Acknowledgments
- •1 Introduction to Radio Waves and Radio Engineering
- •1.1 Radio Waves as a Part of the Electromagnetic Spectrum
- •1.2 What Is Radio Engineering?
- •1.3 Allocation of Radio Frequencies
- •1.4 History of Radio Engineering from Maxwell to the Present
- •2.2 Fields in Media
- •2.3 Boundary Conditions
- •2.4 Helmholtz Equation and Its Plane Wave Solution
- •2.5 Polarization of a Plane Wave
- •2.6 Reflection and Transmission at a Dielectric Interface
- •2.7 Energy and Power
- •3 Transmission Lines and Waveguides
- •3.1 Basic Equations for Transmission Lines and Waveguides
- •3.2 Transverse Electromagnetic Wave Modes
- •3.3 Transverse Electric and Transverse Magnetic Wave Modes
- •3.4 Rectangular Waveguide
- •3.4.1 TE Wave Modes in Rectangular Waveguide
- •3.4.2 TM Wave Modes in Rectangular Waveguide
- •3.5 Circular Waveguide
- •3.6 Optical Fiber
- •3.7 Coaxial Line
- •3.8 Microstrip Line
- •3.9 Wave and Signal Velocities
- •3.10 Transmission Line Model
- •4 Impedance Matching
- •4.1 Reflection from a Mismatched Load
- •4.2 Smith Chart
- •4.3 Matching Methods
- •4.3.1 Matching with Lumped Reactive Elements
- •4.3.4 Resistive Matching
- •5 Microwave Circuit Theory
- •5.1 Impedance and Admittance Matrices
- •5.2 Scattering Matrices
- •5.3 Signal Flow Graph, Transfer Function, and Gain
- •6.1 Power Dividers and Directional Couplers
- •6.1.1 Power Dividers
- •6.1.2 Coupling and Directivity of a Directional Coupler
- •6.1.3 Scattering Matrix of a Directional Coupler
- •6.1.4 Waveguide Directional Couplers
- •6.1.5 Microstrip Directional Couplers
- •6.2 Ferrite Devices
- •6.2.1 Properties of Ferrite Materials
- •6.2.2 Faraday Rotation
- •6.2.3 Isolators
- •6.2.4 Circulators
- •6.3 Other Passive Components and Devices
- •6.3.1 Terminations
- •6.3.2 Attenuators
- •6.3.3 Phase Shifters
- •6.3.4 Connectors and Adapters
- •7 Resonators and Filters
- •7.1 Resonators
- •7.1.1 Resonance Phenomenon
- •7.1.2 Quality Factor
- •7.1.3 Coupled Resonator
- •7.1.4 Transmission Line Section as a Resonator
- •7.1.5 Cavity Resonators
- •7.1.6 Dielectric Resonators
- •7.2 Filters
- •7.2.1 Insertion Loss Method
- •7.2.2 Design of Microwave Filters
- •7.2.3 Practical Microwave Filters
- •8 Circuits Based on Semiconductor Devices
- •8.1 From Electron Tubes to Semiconductor Devices
- •8.2 Important Semiconductor Devices
- •8.2.1 Diodes
- •8.2.2 Transistors
- •8.3 Oscillators
- •8.4 Amplifiers
- •8.4.2 Effect of Nonlinearities and Design of Power Amplifiers
- •8.4.3 Reflection Amplifiers
- •8.5.1 Mixers
- •8.5.2 Frequency Multipliers
- •8.6 Detectors
- •8.7 Monolithic Microwave Circuits
- •9 Antennas
- •9.1 Fundamental Concepts of Antennas
- •9.2 Calculation of Radiation from Antennas
- •9.3 Radiating Current Element
- •9.4 Dipole and Monopole Antennas
- •9.5 Other Wire Antennas
- •9.6 Radiation from Apertures
- •9.7 Horn Antennas
- •9.8 Reflector Antennas
- •9.9 Other Antennas
- •9.10 Antenna Arrays
- •9.11 Matching of Antennas
- •9.12 Link Between Two Antennas
- •10 Propagation of Radio Waves
- •10.1 Environment and Propagation Mechanisms
- •10.2 Tropospheric Attenuation
- •10.4 LOS Path
- •10.5 Reflection from Ground
- •10.6 Multipath Propagation in Cellular Mobile Radio Systems
- •10.7 Propagation Aided by Scattering: Scatter Link
- •10.8 Propagation via Ionosphere
- •11 Radio System
- •11.1 Transmitters and Receivers
- •11.2 Noise
- •11.2.1 Receiver Noise
- •11.2.2 Antenna Noise Temperature
- •11.3 Modulation and Demodulation of Signals
- •11.3.1 Analog Modulation
- •11.3.2 Digital Modulation
- •11.4 Radio Link Budget
- •12 Applications
- •12.1 Broadcasting
- •12.1.1 Broadcasting in Finland
- •12.1.2 Broadcasting Satellites
- •12.2 Radio Link Systems
- •12.2.1 Terrestrial Radio Links
- •12.2.2 Satellite Radio Links
- •12.3 Wireless Local Area Networks
- •12.4 Mobile Communication
- •12.5 Radionavigation
- •12.5.1 Hyperbolic Radionavigation Systems
- •12.5.2 Satellite Navigation Systems
- •12.5.3 Navigation Systems in Aviation
- •12.6 Radar
- •12.6.1 Pulse Radar
- •12.6.2 Doppler Radar
- •12.6.4 Surveillance and Tracking Radars
- •12.7 Remote Sensing
- •12.7.1 Radiometry
- •12.7.2 Total Power Radiometer and Dicke Radiometer
- •12.8 Radio Astronomy
- •12.8.1 Radio Telescopes and Receivers
- •12.8.2 Antenna Temperature of Radio Sources
- •12.8.3 Radio Sources in the Sky
- •12.9 Sensors for Industrial Applications
- •12.9.1 Transmission Sensors
- •12.9.2 Resonators
- •12.9.3 Reflection Sensors
- •12.9.4 Radar Sensors
- •12.9.5 Radiometer Sensors
- •12.9.6 Imaging Sensors
- •12.10 Power Applications
- •12.11 Medical Applications
- •12.11.1 Thermography
- •12.11.2 Diathermy
- •12.11.3 Hyperthermia
- •12.12 Electronic Warfare
- •List of Acronyms
- •About the Authors
- •Index
326 Radio Engineering for Wireless Communication and Sensor Applications
The European Union has a definite plan to deploy a new satellite navigation system called Galileo starting in 2005. The Galileo system should be ready for full operation in 2008 when all 30 satellites are orbiting at the altitude of 24,000 km.
12.5.3 Navigation Systems in Aviation
In addition to hyperbolic and satellite navigation systems, many other radionavigation systems are in use in aviation.
VHF Omnidirectional Range (VOR) is based on omnidirectional beacons operating in the range of 108 to 118 MHz. The carrier is amplitude or frequency modulated at 30 Hz so that the phase of modulation depends on the azimuth angle. Two subcarriers 9,960 Hz apart from the carrier are frequency modulated at 30 Hz and are angle-independent reference signals. The receiver on an aircraft measures the phase difference of the 30-Hz signals and thus reveals the direction of the beacon.
Distance Measuring Equipment (DME) operates in the range of 962 to 1,213 MHz and is usually located with a VOR beacon. Its frequency can be ‘‘paired’’ with VOR or ILS. The distance between an interrogator on an aircraft and a transponder at a ground station is obtained from the time it takes for the signal to propagate from the aircraft to the ground station and back, as shown in Figure 12.12. The interrogator sends a pair of pulses. The transponder delays its response by 50 m s and changes the frequency by 63 MHz.
The Instrument Landing System (ILS) and Microwave Landing System
(MLS) are landing systems that give guidance for airplanes approaching a runway. ILS was introduced in the 1940s. It consists of three radio systems, as indicated in Figure 12.13: localizer, glide slope, and marker signals. The localizer signal (108–112 MHz) provides lateral guidance. The right side of the antenna pattern, as seen by an approaching aircraft, is modulated at
Figure 12.12 Operating principle of DME.
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Figure 12.13 ILS localizer, glide slope, and marker beams.
150 Hz, and the left side at 90 Hz. On the correct track, the 90 and 150 Hz signals are of equal intensity. The glide slope signal (329–335 MHz) provides vertical guidance. The upper part of the pattern is modulated at 90 Hz and the lower part at 150 Hz. The intensities of the modulating signals are equal in the optimum glide angle, which is typically 2.5° to 3°. Marker beacons at 75 MHz provide information on the distance from the runway.
MLS is a precision landing system that will replace ILS. MLS allows different glide angles and curved approach paths, and has many other advantages over ILS. Navigation is based on five signals: (1) the scanning azimuth signal, ±40° or ±60°; (2) the scanning elevation signal, maximum scan 0.9° to 30°; (3) the back-azimuth signal for missed approaches; (4) precision DME (DME/P); and (5) data signals. With the exception of DME/P, all MLS signals are transmitted on a single frequency through time-sharing. The operating range, 5,031 to 5,091 MHz, contains 200 channels. Figure 12.14 shows how the azimuth angle of an approaching plane is measured. The narrow beam produced by a phased antenna array sweeps at a fixed scan rate, and the receiver on the plane measures the time interval between sweeps,
Figure 12.14 Azimuth signal of MLS.