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Microwave Devices. Introduction. Microwaves have frequencies > 1 GHz approx. Stray reactances are more important as frequency increases Transmission line techniques must be applied to short conductors like circuit board traces Device capacitance and transit time are important

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Introduction l.jpg

  • Microwaves have frequencies > 1 GHz approx.

  • Stray reactances are more important as frequency increases

  • Transmission line techniques must be applied to short conductors like circuit board traces

  • Device capacitance and transit time are important

  • Cable losses increase: waveguides often used instead

Waveguides l.jpg

  • Pipe through which waves propagate

  • Can have various cross sections

    • Rectangular

    • Circular

    • Elliptical

  • Can be rigid or flexible

  • Waveguides have very low loss

Modes l.jpg

  • Waves can propagate in various ways

  • Time taken to move down the guide varies with the mode

  • Each mode has a cutoff frequency below which it won’t propagate

  • Mode with lowest cutoff frequency is dominant mode

Mode designations l.jpg
Mode Designations

  • TE: transverse electric

    • Electric field is at right angles to direction of travel

  • TM: transverse magnetic

    • Magnetic field is at right angles to direction of travel

  • TEM: transverse electromagnetic

    • Waves in free space are TEM

Rectangular waveguides l.jpg
Rectangular Waveguides

  • Dominant mode is TE10

    • 1 half cycle along long dimension (a)

    • No half cycles along short dimension (b)

    • Cutoff for a = c/2

  • Modes with next higher cutoff frequency are TE01 and TE20

    • Both have cutoff frequency twice that for TE10

Cutoff frequency l.jpg
Cutoff Frequency

  • For TE10 mmode in rectangular waveguide with a = 2 b

Usable frequency range l.jpg
Usable Frequency Range

  • Single mode propagation is highly desirable to reduce dispersion

  • This occurs between cutoff frequency for TE10 mode and twice that frequency

  • It’s not good to use guide at the extremes of this range

Example waveguide l.jpg
Example Waveguide

  • RG-52/U

  • Internal dimensions 22.9 by 10.2 mm

  • Cutoff at 6.56 GHz

  • Use from 8.2-12.5 GHz

Group velocity l.jpg
Group Velocity

  • Waves propagate at speed of light c in guide

  • Waves don’t travel straight down guide

  • Speed at which signal moves down guide is the group velocity and is always less than c

Phase velocity l.jpg
Phase Velocity

  • Not a real velocity (>c)

  • Apparent velocity of wave along wall

  • Used for calculating wavelength in guide

    • For impedance matching etc.

Characteristic impedance l.jpg
Characteristic Impedance

  • Z0 varies with frequency

Guide wavelength l.jpg
Guide Wavelength

  • Longer than free-space wavelength at same frequency

Impedance matching l.jpg
Impedance Matching

  • Same techniques as for coax can be used

  • Tuning screw can add capacitance or inductance

Coupling power to guides l.jpg
Coupling Power to Guides

  • 3 common methods

    • Probe: at an E-field maximum

    • Loop: at an H-field maximum

    • Hole: at an E-field maximum

Directional coupler l.jpg
Directional Coupler

  • Launches or receives power in only 1 direction

  • Used to split some of power into a second guide

  • Can use probes or holes

Passive compenents l.jpg
Passive Compenents

  • Bends

    • Called E-plane or H-Plane bends depending on the direction of bending

  • Tees

    • Also have E and H-plane varieties

    • Hybrid or magic tee combines both and can be used for isolation

Resonant cavity l.jpg
Resonant Cavity

  • Use instead of a tuned circuit

  • Very high Q

Attenuators and loads l.jpg
Attenuators and Loads

  • Attenuator works by putting carbon vane or flap into the waveguide

  • Currents induced in the carbon cause loss

  • Load is similar but at end of guide

Circulator and isolator l.jpg
Circulator and Isolator

  • Both use the unique properties of ferrites in a magnetic field

  • Isolator passes signals in one direction, attenuates in the other

  • Circulator passes input from each port to the next around the circle, not to any other port

Microwave transistors l.jpg
Microwave Transistors

  • Designed to minimize capacitances and transit time

  • NPN bipolar and N channel FETs preferred because free electrons move faster than holes

  • Gallium Arsenide has greater electron mobility than silicon

Gunn device l.jpg
Gunn Device

  • Slab of N-type GaAs (gallium arsenide)

  • Sometimes called Gunn diode but has no junctions

  • Has a negative-resistance region where drift velocity decreases with increased voltage

  • This causes a concentration of free electrons called a domain

Transit time mode l.jpg
Transit-time Mode

  • Domains move through the GaAs till they reach the positive terminal

  • When domain reaches positive terminal it disappears and a new domain forms

  • Pulse of current flows when domain disappears

  • Period of pulses = transit time in device

Gunn oscillator frequency l.jpg
Gunn Oscillator Frequency

  • T=d/v

    T = period of oscillation

    d = thickness of device

    v = drift velocity, about 1  105 m/s

  • f = 1/T

Impatt diode l.jpg

  • IMPATT stands for Impact Avalanche And Transit Time

  • Operates in reverse-breakdown (avalanche) region

  • Applied voltage causes momentary breakdown once per cycle

  • This starts a pulse of current moving through the device

  • Frequency depends on device thickness

Pin diode l.jpg
PIN Diode

  • P-type --- Intrinsic --- N-type

  • Used as switch and attenuator

  • Reverse biased - off

  • Forward biased - partly on to on depending on the bias

Varactor diode l.jpg
Varactor Diode

  • Lower frequencies: used as voltage-variable capacitor

  • Microwaves: used as frequency multiplier

    • this takes advantage of the nonlinear V-I curve of diodes

Yig devices l.jpg
YIG Devices

  • YIG stands for Yttrium - Iron - Garnet

    • YIG is a ferrite

  • YIG sphere in a dc magnetic field is used as resonant cavity

  • Changing the magnetic field strength changes the resonant frequency

Dielectric resonator l.jpg
Dielectric Resonator

  • resonant cavity made from a slab of a dielectric such as alumina

  • Makes a good low-cost fixed-frequency resonant circuit

Microwave tubes l.jpg
Microwave Tubes

  • Used for high power/high frequency combination

  • Tubes generate and amplify high levels of microwave power more cheaply than solid state devices

  • Conventional tubes can be modified for low capacitance but specialized microwave tubes are also used

Magnetron l.jpg

  • High-power oscillator

  • Common in radar and microwave ovens

  • Cathode in center, anode around outside

  • Strong dc magnetic field around tube causes electrons from cathode to spiral as they move toward anode

  • Current of electrons generates microwaves in cavities around outside

Slow wave structure l.jpg
Slow-Wave Structure

  • Magnetron has cavities all around the outside

  • Wave circulates from one cavity to the next around the outside

  • Each cavity represents one-half period

  • Wave moves around tube at a velocity much less than that of light

  • Wave velocity approximately equals electron velocity

Duty cycle l.jpg
Duty Cycle

  • Important for pulsed tubes like radar transmitters

  • Peak power can be much greater than average power

Crossed field and linear beam tubes l.jpg
Crossed-Field and Linear-Beam Tubes

  • Magnetron is one of a number of crossed-field tubes

    • Magnetic and electric fields are at right angles

  • Klystrons and Traveling-Wave tubes are examples of linear-beam tubes

    • These have a focused electron beam (as in a CRT)

Klystron l.jpg

  • Used in high-power amplifiers

  • Electron beam moves down tube past several cavities.

  • Input cavity is the buncher, output cavity is the catcher.

  • Buncher modulates the velocity of the electron beam

Velocity modulation l.jpg
Velocity Modulation

  • Electric field from microwaves at buncher alternately speeds and slows electron beam

  • This causes electrons to bunch up

  • Electron bunches at catcher induce microwaves with more energy

  • The cavities form a slow-wave structure

Traveling wave tube twt l.jpg
Traveling-Wave Tube (TWT)

  • Uses a helix as a slow-wave structure

  • Microwaves input at cathode end of helix, output at anode end

  • Energy is transferred from electron beam to microwaves

Microwave antennas l.jpg
Microwave Antennas

  • Conventional antennas can be adapted to microwave use

  • The small wavelength of microwaves allows for additional antenna types

  • The parabolic dish already studied is a reflector not an antenna but we saw that it is most practical for microwaves

Horn antennas l.jpg
Horn Antennas

  • Not practical at low frequencies because of size

  • Can be E-plane, H-plane, pyramidal or conical

  • Moderate gain, about 20 dBi

  • Common as feed antennas for dishes

Slot antenna l.jpg
Slot Antenna

  • Slot in the wall of a waveguide acts as an antenna

  • Slot should have length g/2

  • Slots and other basic antennas can be combined into phased arrays with many elements that can be electrically steered

Fresnel lens l.jpg
Fresnel Lens

  • Lenses can be used for radio waves just as for light

  • Effective lenses become small enough to be practical in the microwave region

  • Fresnel lens reduces size by using a stepped configuration

Radar l.jpg

  • Radar stands for Radio Dedtection And Ranging

  • Two main types

    • Pulse radar locates targets by measuring time for a pulse to reflect from target and return

    • Doppler radar measures target speed by frequency shift of returned signal

    • It is possible to combine these 2 types

Radar cross section l.jpg
Radar Cross Section

  • Indicates strength of returned signal from a target

  • Equals the area of a flat conducting plate facing the source that reflects the same amount of energy to the source

Radar equation l.jpg
Radar Equation

  • Expression for received power from a target

Pulse radar l.jpg
Pulse Radar

  • Direction to target found with directional antenna

  • Distance to target found from time taken for signal to return from target

    R = ct/2

Maximum range l.jpg
Maximum Range

  • Limited by pulse period

  • If reflection does not return before next pulse is transmitted the distance to the target is ambiguous

    Rmax = cT/2

Minimum range l.jpg
Minimum Range

  • If pulse returns before end of transmitted pulse, it will not be detected

    Rmin = cTP/2

  • A similar distance between targets is necessary to separate them

Doppler radar l.jpg
Doppler Radar

  • Motion along line from radar to target changes frequency of reflection

  • Motion toward radar raises frequency

  • Motion away from radar lowers frequency

Limitations of doppler radar l.jpg
Limitations of Doppler Radar

  • Only motion towards or away from radar is measured accurately

  • If motion is diagonal, only the component along a line between radar and target is measured

Stealth l.jpg

  • Used mainly by military planes, etc to avoid detection

  • Avoid reflections by making the aircraft skin absorb radiation

  • Scatter reflections using sharp angles