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4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.
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MICROWAVE ENGINEERING
CONTENTS Lumped-Element Circuit Model Field Analysis of Transmission Lines Terminated Lossless Transmission Line Smith Chart Slotted Line Quarter-Wave Transformer Generator and Load Mismatches Lossy Transmission Lines MICROWAVE ENGINEERING David M . Pozar Antennas & RF Devices Lab.
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Lumped-Element Circuit Model
Transit Time Effect At some instant let the voltage at ππβ² be π½ π· . Then π½ π· will appear at π π β² only after π π . However, during this time the voltage at ππβ² changes to π½ πΈ . Transit time π π = π π The transit time effect can be neglected if π»β« π π β πβ«π Antennas & RF Devices Lab.
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π
=Ξ©/m , πΏ=H/m , πΊ=S/m , πΆ=F/m
Lumped-Element Circuit Model Transmission line Equations FIGURE 2.1 Voltage and current definitions and equivalent circuit for an incremental length of transmission line. (a) Voltage and current definitions. (b) Lumped-element equivalent circuit. KVL (Kirchhoffβs voltage law) KCL (Kirchhoffβs current law) Antennas & RF Devices Lab.
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Lumped-Element Circuit Model
Transmission line Equations Phasor General solution (2.3a) , (2.6a) Characteristic impedance Complex propagation constant Antennas & RF Devices Lab.
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Lumped-Element Circuit Model
Transmission line Equations (Lossless Line) General Lossless βRealβ Antennas & RF Devices Lab.
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Field Analysis of Transmission Lines
Parameters Chapter 1 Circuit theory FIGURE 2.2 Field lines on an arbitrary TEM transmission line. Magnetic energy Conductivity power loss Electric energy Dielectric power loss Antennas & RF Devices Lab.
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Field Analysis of Transmission Lines
Parameters TABLE 2.1 Transmission Line Parameters for Some Common Lines Antennas & RF Devices Lab.
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Field Analysis of Transmission Lines
Coaxial Line (TEM Wave) π/ππ=0 πΈ π§ = π» π§ =0 π ππ π πΈ π =0 Independent of π Antennas & RF Devices Lab.
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Field Analysis of Transmission Lines
Coaxial Line (TEM Wave) Voltage between the two conductors Eliminate π(π) and π(π) Current on the inner conductor (π=π) TABLE 2.1 Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Total Voltage and Current FIGURE 2.4 A transmission line terminated in a load impedance π πΏ . Load impedance Rearrange Reflection coefficient Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Return Loss Complex conjugate β zero Incident power Reflected power Return loss π π 0 π π 0 π€ 2 πͺ=π β RL =β πͺ=π β RL =0 Second order! Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Standing Wave Ratio π π§ = π 0 + π βππ½π§ +π€ π 0 + π ππ½π§ Euler formula Standing Wave Ratio Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Input Impedance π ππ = cos π +π sin π Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Short Circuit FIGURE 2.5 A transmission line terminated in a short circuit. =β Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Open Circuit FIGURE 2.6 A transmission line terminated in a open circuit. =β Antennas & RF Devices Lab. Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Half-Wavelength Line & Quarter-Wavelength Line Half-Wavelength Line π½= 2π π Quarter-Wavelength Line βQuarter-wave transformerβ =βπ€(0) 180Β° phase shift ! Antennas & RF Devices Lab.
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Terminated Lossless Transmission Line
Junction of Two Transmission Lines FIGURE 2.9 Reflection and transmission at the junction of two transmission lines with different characteristic impedances. Equal when π§=0 Return loss Transmission coefficient Insertion loss Antennas & RF Devices Lab.
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Smith Chart Normalize Rearrange Rearrange Antennas & RF Devices Lab.
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Smith Chart Antennas & RF Devices Lab.
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Smith Chart Antennas & RF Devices Lab.
Rotate the point clockwise an amount 2π½β FIGURE 2.11 Smith chart for Example 2.2. Antennas & RF Devices Lab.
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Slotted Line Antennas & RF Devices Lab.
SWR, distance of the first voltage minimum from the load can be measured. Load impedance Antennas & RF Devices Lab.
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Quarter-Wave Transformer
The Impedance Viewpoint π πΏ , π 0 are both real FIGURE 2.16 The quarter-wave matching transformer. β= π 4 Antennas & RF Devices Lab.
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Quarter-Wave Transformer
Multiple Reflection Viewpoint 180Β° phase shift ! numerator FIGURE 2.18 Multiple reflection analysis of the quarter-wave transformer. Antennas & RF Devices Lab.
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Quarter-Wave Transformer
Multiple Reflection Viewpoint numerator =0 numerator =0 This is the same result as (2.63) Antennas & RF Devices Lab.
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Generator and Load Mismatches
FIGURE 2.19 Transmission line circuit for mismatches load and generator. Voltage distribution Antennas & RF Devices Lab.
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Generator and Load Mismatches
FIGURE 2.19 Transmission line circuit for mismatches load and generator. Standing wave ratio Power delivered to the load Antennas & RF Devices Lab.
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Generator and Load Mismatches
Load Matched to Line Lossless line β π 0 is real β π in is real Antennas & RF Devices Lab.
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Generator and Load Mismatches
Generator Matched to Loaded Line The power delivered to the load may be less than βLoad Matched to Lineβ Load Matched to Line Antennas & RF Devices Lab.
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Generator and Load Mismatches
Conjugate Matching *Find the maximum value through derivative. Antennas & RF Devices Lab.
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Lossy Transmission Lines
Low-Loss Line Taylor series expansion Low-loss line can be closely approximated by considering the line as lossless. Antennas & RF Devices Lab.
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Lossy Transmission Lines
Terminated Lossy Line FIGURE 2.20 A lossy transmission line terminated in the impedance π πΏ . Lossless tanh π§ = π π§ β π βπ§ π π§ + π βπ§ Antennas & RF Devices Lab.
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Lossy Transmission Lines
Terminated Lossy Line FIGURE 2.20 A lossy transmission line terminated in the impedance π πΏ . Both terms increase as πΌ increses. Antennas & RF Devices Lab.
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Lossy Transmission Lines
Perturbation Method for Calculating Attenuation *No use Transmission line parameters ( πΏ, πΆ, π
, πΊ ). *Assume that the fields of the lossy line are not greatly different from the fields of the lossless line. Antennas & RF Devices Lab.
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THANK YOU
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