Yungui MA ( 马云贵 ) E-mail: [email protected]@zju.edu.cn Office: Room 209, East Building...
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Transcript of Yungui MA ( 马云贵 ) E-mail: [email protected]@zju.edu.cn Office: Room 209, East Building...
Yungui MA ( 马云贵 )E-mail: [email protected]
Office: Room 209, East Building 5, Zijin’gang campus
Microwave Microwave FundamentalsFundamentals
Electromagnetic spectrum
Band P L S C X Ku K Ka
Freq (GHz)
0.23-1 1-2 2-4 4-8 8-12.5 12.5-18 18-26.5 26.5-40
300 MHz 3 GHz 30 GHz 300 GHz 3 THz 30 THz 300 THz
Photonic devices
Electronic devices
Microwaves THz gap visibleRadio waves UV
Microwave bands
Millimeter waves
Infrared
Microwave applicationsWireless communications (cell phones, WLAN,
…)Global positioning system (GPS)Computer engineering (bus systems, CPU, …)Microwave antennas (radar, communication,
remote sensing, …)Other applications (microwave heating, power
transfer, imaging, biological effect and safety)
课件下载
SyllabusChapter 1: Transmission line theory
Chapter 2: Transmission lines and waveguides
Chapter 3: Microwave network analysis
Chapter 4: Microwave resonators
Reference books : 1.David M. Pozar, Microwave Engineering, third edition (Wiley, 2005)2.Robert E. Collin, Foundations for microwave engineering, second edition (Wiley, 2007) 3.J. A. Kong , Electromagnetic theory (EMW, 2000)
Chapter 1: Transmission line theory 1.1 Why from lumped to distributed
theory?
1.2 Examples of transmission lines
1.3 Distributed network for a
transmission line
1.4 Field analysis of transmission lines
1.5 The terminated lossless
transmission line
1.6 Sourced and loaded transmission
lines
1.1 Why from lumped to distributed theory?
At low frequencies: Can simply use a wire to connect two components
f =50 HZ, wavelength = 6 x 106m;
At high frequencies: Cannot simply use a wire to connect two components
f =500 MHZ, wavelength = 0.6 m;
1.1 Why from lumped to distributed theory?
1.1 Why from lumped to distributed theory?
E field
H field
Microwave component: electric size << the operating wavelength
R = series resistance per unit length, for both conductors, in /m;L = series inductance per unit length, for both conductors, in H/m;G = parallel conductance per unit length, in S/m;C = parallel capacitance per unit length, in F/m.
Loss: R (due to the finite conductivity) + G (due to the dielectric loss)
Transmission line theory
Transmission line theory
Bridges the gap between field analysis and basic circuit theory
Extension from lumped to distributed theoryA specialization of Maxwell’s equationsSignificant importance in microwave network
analysis
The key difference between circuit theory and transmission line theory is electrical size. Circuit analysis assumes that the physical dimensions of a network are much smaller than the electrical wavelength, while transmission lines may be a considerable fraction of a wavelength, or many wavelengths, in size. Thus a transmission line is a distributed-parameter network, where voltages and currents can vary in magnitude and phase over its length.
1.2 Examples of transmission lines
(2) Coaxial line
Magnetic field
(dashed lines)
Electric field
(solid lines)
(3) Microstrip line
(1)Two-wire line
Review: Kerchhoff’s law
1.3 Distributed network for a transmission line
KCL: 01
n
kki KVL: 0
1
n
kkv
1.3 Distributed network for a transmission line
1.3 Distributed network for a transmission line
Derivation of differential transmission line equation
KVL:
Derivation of differential transmission line equation
KCL:
Derivation of differential transmission line equation
Phasor form of sinusoid haromic wave
Time factor convention
Derivation of differential transmission line equation
ki, Phase constant, rad/m
kr, attenuation constant, nep/m
Impedance, wavelength and phase velocity
Wavelength:
Phase velocity:
)cos()cos(),( 00 zktVzktVtzv ii
Voltage in the time domain:
ik/2
fk
vi
p
Characteristic impedance:
TL current:
Characteristic impedance:
Phase velocity:
Wavelength: (what happens if exchange L and C ?)
LC /2
LCvp /1
Propagation constant: