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4th Week Seminar Sunryul Kim 2018.08.01 Antennas & RF Devices Lab.

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Presentation on theme: "4th Week Seminar Sunryul Kim 2018.08.01 Antennas & RF Devices Lab."β€” Presentation transcript:

1 4th Week Seminar Sunryul Kim Antennas & RF Devices Lab.

2 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.

3 Lumped-Element Circuit Model
Transit Time Effect At some instant let the voltage at 𝐀𝐀′ be 𝑽 𝑷 . Then 𝑽 𝑷 will appear at 𝐁 𝐁 β€² only after 𝒕 𝒓 . However, during this time the voltage at 𝐀𝐀′ changes to 𝑽 𝑸 . Transit time 𝒕 𝒓 = 𝒍 𝒗 The transit time effect can be neglected if 𝑻≫ 𝒕 𝒓 β†’ π›Œβ‰«π’ Antennas & RF Devices Lab.

4 𝑅=Ξ©/m , 𝐿=H/m , 𝐺=S/m , 𝐢=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 (Kirchhoff’s voltage law) KCL (Kirchhoff’s current law) Antennas & RF Devices Lab.

5 Lumped-Element Circuit Model
Transmission line Equations Phasor General solution (2.3a) , (2.6a) Characteristic impedance Complex propagation constant Antennas & RF Devices Lab.

6 Lumped-Element Circuit Model
Transmission line Equations (Lossless Line) General Lossless β€˜Real’ Antennas & RF Devices Lab.

7 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.

8 Field Analysis of Transmission Lines
Parameters TABLE 2.1 Transmission Line Parameters for Some Common Lines Antennas & RF Devices Lab.

9 Field Analysis of Transmission Lines
Coaxial Line (TEM Wave) πœ•/πœ•πœ™=0 𝐸 𝑧 = 𝐻 𝑧 =0 πœ• πœ•πœŒ 𝜌 𝐸 πœ™ =0 Independent of 𝜌 Antennas & RF Devices Lab.

10 Field Analysis of Transmission Lines
Coaxial Line (TEM Wave) Voltage between the two conductors Eliminate 𝒉(𝒛) and π’ˆ(𝒛) Current on the inner conductor (𝜌=π‘Ž) TABLE 2.1 Antennas & RF Devices Lab.

11 Terminated Lossless Transmission Line
Total Voltage and Current FIGURE 2.4 A transmission line terminated in a load impedance 𝑍 𝐿 . Load impedance Rearrange Reflection coefficient Antennas & RF Devices Lab.

12 Terminated Lossless Transmission Line
Return Loss Complex conjugate β†’ zero Incident power Reflected power Return loss 𝑉 𝑍 0 𝑉 𝑍 0 𝛀 2 πšͺ=𝟎 β†’ RL =∞ πšͺ=𝟏 β†’ RL =0 Second order! Antennas & RF Devices Lab.

13 Terminated Lossless Transmission Line
Standing Wave Ratio 𝑉 𝑧 = 𝑉 0 + 𝑒 βˆ’π‘—π›½π‘§ +𝛀 𝑉 0 + 𝑒 𝑗𝛽𝑧 Euler formula Standing Wave Ratio Antennas & RF Devices Lab.

14 Terminated Lossless Transmission Line
Input Impedance 𝑒 π‘—πœƒ = cos πœƒ +𝑗 sin πœƒ Antennas & RF Devices Lab.

15 Terminated Lossless Transmission Line
Short Circuit FIGURE 2.5 A transmission line terminated in a short circuit. =∞ Antennas & RF Devices Lab.

16 Terminated Lossless Transmission Line
Open Circuit FIGURE 2.6 A transmission line terminated in a open circuit. =∞ Antennas & RF Devices Lab. Antennas & RF Devices Lab.

17 Terminated Lossless Transmission Line
Half-Wavelength Line & Quarter-Wavelength Line Half-Wavelength Line 𝛽= 2πœ‹ πœ† Quarter-Wavelength Line β€œQuarter-wave transformer” =βˆ’π›€(0) 180Β° phase shift ! Antennas & RF Devices Lab.

18 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 𝑧=0 Return loss Transmission coefficient Insertion loss Antennas & RF Devices Lab.

19 Smith Chart Normalize Rearrange Rearrange Antennas & RF Devices Lab.

20 Smith Chart Antennas & RF Devices Lab.

21 Smith Chart Antennas & RF Devices Lab.
Rotate the point clockwise an amount 2𝛽ℓ FIGURE 2.11 Smith chart for Example 2.2. Antennas & RF Devices Lab.

22 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.

23 Quarter-Wave Transformer
The Impedance Viewpoint 𝑍 𝐿 , 𝑍 0 are both real FIGURE 2.16 The quarter-wave matching transformer. β„“= πœ† 4 Antennas & RF Devices Lab.

24 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.

25 Quarter-Wave Transformer
Multiple Reflection Viewpoint numerator =0 numerator =0 This is the same result as (2.63) Antennas & RF Devices Lab.

26 Generator and Load Mismatches
FIGURE 2.19 Transmission line circuit for mismatches load and generator. Voltage distribution Antennas & RF Devices Lab.

27 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.

28 Generator and Load Mismatches
Load Matched to Line Lossless line β†’ 𝑍 0 is real β†’ 𝑍 in is real Antennas & RF Devices Lab.

29 Generator and Load Mismatches
Generator Matched to Loaded Line The power delivered to the load may be less than β€˜Load Matched to Line’ Load Matched to Line Antennas & RF Devices Lab.

30 Generator and Load Mismatches
Conjugate Matching *Find the maximum value through derivative. Antennas & RF Devices Lab.

31 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.

32 Lossy Transmission Lines
Terminated Lossy Line FIGURE 2.20 A lossy transmission line terminated in the impedance 𝑍 𝐿 . Lossless tanh 𝑧 = 𝑒 𝑧 βˆ’ 𝑒 βˆ’π‘§ 𝑒 𝑧 + 𝑒 βˆ’π‘§ Antennas & RF Devices Lab.

33 Lossy Transmission Lines
Terminated Lossy Line FIGURE 2.20 A lossy transmission line terminated in the impedance 𝑍 𝐿 . Both terms increase as 𝛼 increses. Antennas & RF Devices Lab.

34 Lossy Transmission Lines
Perturbation Method for Calculating Attenuation *No use Transmission line parameters ( 𝐿, 𝐢, 𝑅, 𝐺 ). *Assume that the fields of the lossy line are not greatly different from the fields of the lossless line. Antennas & RF Devices Lab.

35 THANK YOU


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