ece 563 / tcom 590 introduction to microwaves and e&m review

43
ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review September 2, 2004 M. Black

Upload: lucia

Post on 25-Feb-2016

27 views

Category:

Documents


0 download

DESCRIPTION

ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review. September 2, 2004 M. Black. Brief Microwave History. Maxwell (1864-73) integrated electricity and magnetism set of 4 coherent and self-consistent equations predicted electromagnetic wave propagation Hertz (1886-88) - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

ECE 563 / TCOM 590Introduction to Microwaves

and E&M Review

September 2, 2004M. Black

Page 2: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review
Page 3: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Brief Microwave History• Maxwell (1864-73)

– integrated electricity and magnetism– set of 4 coherent and self-consistent equations– predicted electromagnetic wave propagation

• Hertz (1886-88) – experimentally confirmed Maxwell’s equations – oscillating electric spark to induce similar

oscillations in a distant wire loop (=10 cm)

Page 4: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Brief Microwave History• Marconi (early 20th century)

– parabolic antenna to demonstrate wireless telegraphic communications

– tried to commercialize radio at low frequency• Lord Rayleigh (1897)

– showed mathematically that EM wave propagation possible in waveguides

• George Southworth (1930)– showed waveguides capable of small

bandwidth transmission for high powers

Page 5: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Brief Microwave History• R.H. and S.F. Varian (1937)

– development of the klystron• MIT Radiation Laboratory (WWII)

– radiation lab series - classic writings• Development of transistor (1950’s)• Development of Microwave Integrated

Circuits– microwave circuit on a chip– microstrip lines

• Satellites, wireless communications, ...

Page 6: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Microwave Applications– Wireless Applications – TV and Radio broadcast– Optical Communications– Radar– Navigation – Remote Sensing– Domestic and Industrial Applications– Medical Applications– Surveillance– Astronomy and Space Exploration

Page 7: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Radar System Comparison

Radar Characteristic wave mmwave optical tracking accuracy poor fair good identification poor fair good volume search good fair poor adverse weather perf. good fair poor perf. in smoke, dust, ... good good fair

Page 8: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Microwave Engr. Distinctions· 1 - Circuit Lengths:· Low frequency ac or rf circuits

· time delay, t, of a signal through a device· t = L/v « T = 1/f where T=period of ac signal· but f=v so 1/f= /v· so L «, I.e. size of circuit is generally much

smaller than the wavelength (or propagation times or phase shift 0)

· Microwaves: L · propagation times not negligible

· Optics: L»

Page 9: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Microwave Distinctions· 2 - Skin Depth:

· degree to which electromagnetic field penetrates a conducting material

· microwave currents tend to flow along the surface of conductors

· so resistive effect is increased, i.e.· R RDC a / 2 , where = skin depth = 1/ ( f o cond)1/2

– where, RDC = 1/ ( a2 cond)– a = radius of the wire• R waves in Cu >R low freq. in Cu

Page 10: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Microwave Engr. Distinctions

· 3 - Measurement Technique· At low frequencies circuit properties

measured by voltage and current· But at microwaves frequencies, voltages

and currents are not uniquely defined; so impedance and power are measured rather than voltage and current

Page 11: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Circuit Limitations• Simple circuit: 10V, ac driven, copper wire,

#18 guage, 1 inch long and 1 mm in diameter: dc resistance is 0.4 m, L=0.027μH– f = 0; XL = 2 f L 0.18 f 10-6 =0– f = 60 Hz; XL 10-5 = 0.01 m– f = 6 MHz; XL 1 – f = 6 GHz; XL 103 = 1 k – So, wires and printed circuit boards cannot be

used to connect microwave devices; we need transmission lines, waveguides, striplines, and microstrip

Page 12: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

High-Frequency Resistors• Inductance and resistance of wire resistors

under high-frequency conditions (f 500 MHz): L/RDC a / (2 )– R /RDC a / (2 )– where, RDC = /( a2 cond)– a = radius of the wire = skin depth = 1/ ( f o cond)-1/2

Page 13: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Reference: Ludwig & Bretchko, RF Circuit Design

Page 14: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

High Frequency Capacitor

• Equivalent circuit consists of parasitic lead conductance L, series resistance Rs describing the losses in the the lead conductors and dielectric loss resistance Re = 1/Ge (in parallel) with the Capacitor.

• Ge = C tan s, where – tan s = (/diel) -1 = loss tangent

Page 15: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Reference: Ludwig & Bretchko, RF Circuit Design

Page 16: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Reference: Ludwig & Bretchko, RF Circuit Design

Page 17: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Transit Limitations

• Consider an FET• Source to drain spacing roughly 2.5 microns• Apply a 10 GHz signal:

– T = 1/f = 10-10 = 0.10 nsec– transit time across S to D is roughly 0.025 nsec

or 1/4 of a period so the gate voltage is low and may not permit the S to D current to flow

Page 18: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Ref: text by Pozar

Page 19: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Wireless Communications Options

• Sonic or ultrasonic - low data rates, poor immunity to interference

• Infrared - moderate data rates, but easily blocked by obstructions (use for TV remotes)

• Optical - high data rates, but easily obstructed, requiring line-of-sight

• RF or Microwave systems - wide bandwidth, reasonable propagation

Page 20: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Cellular Telephone Systems (1)• Division of geographical area into non-

overlapping hexagonal cells, where each has a receiving and transmitting station

• Adjacent cells assigned different sets of channel frequencies, frequencies can be reused if at least one cell away

• Generally use circuit-switched public telephone networks to transfer calls between users

Page 21: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Cellular Telephone Systems (2)• Initially all used analog FM modulation and

divided their allocated frequency bands into several hundred channels, Advanced Mobile Phone Service (AMPS) – both transmit and receive bands have 832, 25

kHz wide bands. [824-849 MHz and 869-894 MHz] using full duplex (with frequency division)

• 2nd generation uses digital or Personal Communication Systems (PCS)

Page 22: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Satellite systems• Large number of users over wide areas• Geosynchronous orbit (36,000 km above earth)

– fixed position relative to the earth– TV and data communications

• Low-earth orbit (500-2000 km)– reduce time-delay of signals– reduce the need for large signal strength– requires more satellites

• Very expensive to maintain & often needs line-of sight

Page 23: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Global Positioning Satellite System (GPS)

• 24 satellites in a medium earth orbit (20km)• Operates at two bands, L1 at 1575.42 and

L2 at 1227.60 MHz , transmitting spread spectrum signals with binary phase shift keying.

• Accurate to better that 100 ft and with differential GPS (with a correcting known base station), better than 10 cm.

Page 24: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Frequency choices• availability of spectrum• noise (increases sharply at freq. below 100

MHz and above 10 GHz)• antenna gain (increases with freq.)• bandwidth (max. data rate so higher freq.

gives smaller fractional bandwidth)• transmitter efficiency (decreases with freq.)• propagation effects (higher freq, line-of sight)

Page 25: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Propagation

• Free space power density decreases by 1/R2

• Atmospheric Attenuation• Reflections with multiple propagation paths

cause fading that reduces effective range, data rates and reliability and quality of service

• Techniques to reduce the effects of fading are expensive and complex

Page 26: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Antennas• RF to an electromagnetic wave or the inverse• Radiation pattern - signal strength as a function

of position around the antenna• Directivity - measure of directionality• Relationship between frequency, gain, and size

of antenna, = c/f– size decreases with frequency– gain proportional to its cross-sectional area \ 2

– phased (or adaptive) array - change direction of beam electronically

Page 27: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

berikutnya coordinate systemsUntuk zx

anmenghasilkx / partialoleh n didefisika ygPerubahan

C sinABA

lainnya r terhadapsatu vecto projeksi

product,dot atau scalar : cosABA

on vectorsinterseksi Bdan AMisalkan

Review

zyy

x

B

B

Math

Page 28: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

sungai) dimengalir ygdaun (pusaran rotation

(Russian) ROTor ;)()A(

flow outwardnet :Divergence ; A

change of rate :gradient ;u

(Space) ruang dalam bervariasi z)y,u(x,uscalar memiliki fieldsebuah jika

z CurlyA

xA

zA

yA

xA

zzuy

yux

xu

zxy

zyx

Page 29: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

theorem(batu) Stokes ;)(

theoremDivergence ;)(

0 curl of divor 0)()( ;)()(

0 gradient of curlor 0 ;0

s

vs

dsAdA

dVAdsA

CCCBACBA

uAA

Page 30: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Maxwell’s Equations

tDJHtBE

BD

//

0 • Gauss

• No Magnetic Poles• Faraday’s Laws• Ampere’s Circuit Law

Page 31: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Characteristics of MediumConstitutive Relationships

npropagatio ofdirection z constant, phase constanton attentuati ,j where

z)-texp(j toalproportion HE,plasma ferrites,except scalars,,

surfaceson sonot itself, medium in the 0,JsAssumption

Current ConvectiveJJJJ E,JtyPermeabili Magnetic ,H,B

yPermitivit Dielectric,ED

v v,cc

ro

,or

Page 32: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Fields in a Dielectric Materials

0on conservatientergy todue negative(heat) medium in the lossfor accounts

magnitude) of orders 4or (3 dielectric goodfor ,j)1(EE)1(D

itysuceptibil dielectric ,E density moment dipole Pdensity)nt displacemeor flux electric(D 0J and

so magnetic,non and ,PED Assume

eo

eo

eoe

oo

Page 33: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Fields in a Conductive Materials

tan tangent loss effective

tyconductivi effective theis where

E)](j[E)jj(j

E))j(jj(E)j

(j

EjEtEE

tDJH

e as vary fields E where,EJJ tjc

Page 34: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Wave Equation

and by described mediumin wavesofconstant n propagatio :

;H - H

;E - E

E))(()H( E -E)(E)(

EjH H,-jEjt/Consider

2

22

22

2

kdefine

similarly

jjj

Page 35: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

General Procedure to Find Fields in a Guided Structure

• 1- Use wave equations to find the z component of Ez and/or Hz

– note classifications – TEM: Ez = Hz= 0

– TE: Ez = 0, Hz 0

– TM: Hz = 0, Ez 0

– HE or Hybrid: Ez 0, Hz 0

Page 36: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

General Procedure to Find Fields in a Guided Structure

• 2- Use boundary conditions to solve for any constraints in our general solution for Ez and/or Hz

conductor of surface the tonormaln whereconductorperfect of surfaceon 0Hor ,0Hn

JHn

/E n

conductorperfect of surfaceon 0Eor 0,En

n

s

t

s

Page 37: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Plane Waves in Lossless Medium

direction z in the movingconstantkztω))kzt(cos(E))kzt(cos(E)t,z(E

:domain timein theor

eEeE)z(E0EkzE

0y/x/ and E Emedium lossless ain

real are and since real is ωk where0,EkE

x

jkzjkzxx

22x

2

x

22

Page 38: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Phase Velocity

cfv

fvfvv

c

kdtd

dtdz

p

ppp

oo

:space freein

or 2

k2

k2))k(z-t(-kz)-t(maxima successive 2between distance :Wavelength

m/sec 1031 vspace freein

1)k

constant-t(v

velocityaat elspoint trav phase Fixed

8p

p

Page 39: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Wave Impedance

E/Hor k

where

)eEeE(kH

HjejkEejkE

yz

ExEzz

so ;0yx

HjtH-E :eqn sMaxwell'By

jkzjkzy

yjkzjkz

xx

Page 40: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Plane Waves in a Lossy Medium

k and j and

0,0 note)j1(jj

complex now,number ewav)j1(

0E)j1(E

E)E(E

)EEj(j)H(jEEEjH and HjE

22

22

2

Page 41: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Wave Impedance in Lossy Medium

losses with impedance wavej where

)eEeE(jH

)ztcos(edomain timeeee

eEeE)z(E0EzE

0y/x/ and xEE before as

zzy

zzjzz

zzxx

22x

2

x

Page 42: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Plane Waves in a good Conductor

surface on the flow currents s,frequencie microwaveat Au)Ag,Cu,(Al, metalsmost for m1 GHz, 10at

depth skin/2/1

2/2/)j1(

/jj/jj

case practical

s

s

2

Page 43: ECE 563 / TCOM 590 Introduction to Microwaves and E&M Review

Energy and Power

ed transmittpowerdszHERe2/1P

)WW(j2PP sourcesby generated powerP

dvHH4/dvBHRe4/1W

dvEE4/dvDERe4/1W

loss as dissipatedor ed transmittbemay that powercarry andenergy magnetic and electric store

thatfields up setsenergy neticelectromag of sourceA

*

so

emo

s

v

*

v

*m

v

*

v

*e