Analytic Solution for Shunt Stub

Slides:



Advertisements
Similar presentations
Microwave Engineering, 3rd Edition by David M. Pozar
Advertisements

ELCT564 Spring /13/20151ELCT564 Chapter 5: Impedance Matching and Tuning.
ENE 428 Microwave Engineering
3 February 2004K. A. Connor RPI ECSE Department 1 Smith Chart Supplemental Information Fields and Waves I ECSE 2100.
Smith Chart Impedance measured at a point along a transmission line depends not only on what is connected to the line, but also on the properties of the.
Lecture 4 Antenna Impedance Matching
EKT241 – ELECTROMAGNETICS THEORY
Microwave Devices E511 Lecture 13 Amr Al.Awamry. Agenda Filter Implementation.
UNIVERSITI MALAYSIA PERLIS
UNIVERSITI MALAYSIA PERLIS
Design and Analysis of RF and Microwave Systems IMPEDANCE TRANSFORMERS AND TAPERS Lecturers: Lluís Pradell Francesc.
Chebyshev Multi-section Matching
ELEC 412 -Lecture 171 ELEC 412 RF & Microwave Engineering Fall 2004 Lecture 17.
Introduction The input network of the power amplifier will be designed in the example. The network synthesized will be expanded to allow for biasing of.
ELCT564 Spring /9/20151ELCT564 Chapter 2: Transmission Line Theory.
Chapter 2: Transmission Line Theory
ELEC 412Lecture 51 ELEC 412 RF & Microwave Engineering Fall 2004 Lecture 5.
ENEE482-Dr. Zaki1 Impedance Matching with Lumped Elements YLYL jX 1 jB 2.
Lecture 9 Last lecture Parameter equations input impedance.
Electromagnetics (ENGR 367) The Smith Chart: A Graphical Method for T-lines.
Impedance Matching Improvement for a Class of Wideband Antennas Dr. Galal Nadim.
LECTURE 2. IMPEDANCE MATCHING
Chapter 5: Impedance Matching and Tuning
Prof. Ji Chen Notes 13 Transmission Lines (Impedance Matching) ECE Spring 2014.
Figure 8. 1 (p. 371) Examples of periodic structures
Lecture 8 Periodic Structures Image Parameter Method
Impedance Matching and Tuning
서강대학교 전자공학과 윤상원 교수 2. Smith Chart. Microwave & Millimeter-wave Lab. 2 차 례차 례 1. Smith chart ; introduction Reflection.
ENE 428 Microwave Engineering
EKT 441 MICROWAVE COMMUNICATIONS
EKT 441 MICROWAVE COMMUNICATIONS
Introduction to Controlling the Output Power of a Transistor Stage A load network will be designed to maximize the output power obtainable from the Mitsubishi.
5. Impedance Matching and Tuning
ENE 490 Applied Communication Systems Lecture 3 Stub matching, single- and two-port networks DATE: 27/11/06.
Chapter 2. Transmission Line Theory
IMPEDANCE MATCHING IN HIGH FREQUENCY LINES UNIT - III.
CHAPTER 4 TRANSMISSION LINES.
Lecture 9 Smith Chart Normalized admittance z and y are directly opposite each other on.
Prof. David R. Jackson Dept. of ECE Notes 3 ECE Microwave Engineering Fall 2011 Smith Chart Examples 1.
1 RS ENE 428 Microwave Engineering Lecture 5 Discontinuities and the manipulation of transmission lines problems.
116/11/50 ENE 490 Applied Communication Systems Lecture 2 circuit matching on Smith chart.
Prof. David R. Jackson Notes 13 Transmission Lines (Impedance Matching) ECE 3317 [Chapter 6]
Chapter 5. Impedance matching and tuning
1 EKT 441 MICROWAVE COMMUNICATIONS CHAPTER 1: TRANSMISSION LINE THEORY (PART III)
ENE 490 Applied Communication Systems
The Smith Chart Developed in 1939 by P. W. Smith as a graphical tool to analyze and design transmission-line circuits Today, it is used to characterize.
ENE 428 Microwave Engineering
Chapter 2. Transmission Line Theory
1.  Transmission lines or T-lines are used to guide propagation of EM waves at high frequencies.  Distances between devices are separated by much larger.
Hanyang University 1/24 Microwave Engineering Chapter 8.8 Wonhong Jeong
ANTENNA THEORY : Analysis and design Third edition
Notes 17 ECE Microwave Engineering Multistage Transformers
Microwave Engineering Chapter 5.7 ~ 5.9
Notes 16 ECE Microwave Engineering Fall 2015 Impedance Matching Prof. David R. Jackson Dept. of ECE 1.
Antenna Matching Techniques
ELEC 401 MICROWAVE ELECTRONICS Lecture on Matching
Dave Glawson – WA6CGR SBMS – October 6, 2011
Chapter 10. Transmission lines
Determining Input Impedance of given lumped circuit elements with TL segments. A lossless TL, with a characteristic load impedance of ZL=100+j75Ω is shown.
Non-ideal property – crosstalk
ENE 429 Antenna and Transmission lines Theory
ENE 429 Antenna and Transmission lines Theory
IMPEDANCE MATCHING & SMITH CHART
Supplemental Information Fields and Waves I ECSE 2100
Microwave Engineering
Notes 13 Transmission Lines (Impedance Matching)
Chapter II Resonators and Impedance Matching
N-port Network Port reference Line Impedance Port Voltage & Current.
Chapter 5.2 Chapter 5.3 SINGLE-STUB TUNING DOUBLE-STUB TUNING
ENE 428 Microwave Engineering
Presentation transcript:

Analytic Solution for Shunt Stub

Problem 1: Repeat example 5.5 using analytic solution.

Example5.6: Design two single-stub (open circuit) series tuning networks to match this load ZL = 100+j 80 to a 50 line, at a frequency of 2 GHz? Solution 1. The normalized load impedance ZL= 2-j1.6. 2. SWR circle intersects the 1+jx circle at both points z1 = 1.0-j1.33 z2 = 1.0+j1.33. Reading WTG can obtain: d1= 0.328-0.208=0.12 d2= 0.672-0.208=0.463. 3. The stub length for tuning z1 to 1 requires l1 = 0.397, and for tuning z1 to 1 needs l2 = 0.103.

1. ZL = 100+j 80 at 2 GHz can find R= 100,L=6.37nH.

Analytic Solution for Series Stub

Problem 2: Repeat example 5.6 using analytic solution.

Shunt stubs are easier to implement in practice than series stubs. Double-Stub Matching adjustable tuning Variable length of length d between load and stub to have adjustable tuning between load and the first stub. Shunt stubs are easier to implement in practice than series stubs. In practice, stub spacing is chosen as /8 or 3/8 and far away 0 or /2 to reduce frequency sensitive. Original circuit Equivalent circuit

Disadvantage is the double-stub tuner cannot match all load impedances Disadvantage is the double-stub tuner cannot match all load impedances. The shaded region forms a forbidden range of load admittances. Two possible solutions b1,b2 and b1’,b2’ with the same distance d.

Example5.7: Design a double-stub (open circuit) shunt tuning networks to match this load ZL = 60-j 80 to a 50 line, at a frequency of 2 GHz? Solution 1. The normalized load impedance YL= 0.3+j0.4 (ZL= 1.2-j1.6). 2. Rotating /8 toward the load (WTL) to construct 1+jb circle can find two values of first stub b1 = 1.314 b’1 = -0.114. 3. Rotating /8 toward the generator (WTG) can obtain y2= 1-j3.38 y’2= 1+j1.38.

4. The susceptance of the second stubs should be 5. The lengyh of the open-circuited stubs are found as l1 = 0.146, l2 = 0.204, or l1 = 0.482, l2 = 0.350. 6.ZL = 60-j 80 at 2 GHz can find R= 60, C=0.995pF.

Analytic Solution for Double Stub

Problem 3: Repeat example 5.7 using analytic solution.

Quarter-Wave transformer It can only match a real load impedance. The length l= /4 at design frequency f0. The important characteristics

Example5.8: Design a quarter-wave matching transformer to match a 10 load to a 50 line? Determine the percent bandwidth for SWR1.5? Solution 

Binomial Multi-section Matching The passband response of a binomial matching transformer is optimum to have as flat as possible near the design frequency, and is known as maximally flat. The important characteristics

Binomial Transformer Design If ZL<Z0, the results should be reversed with Z1 starting at the end.

Example5.9: Design a three-section binomial transformer to match a 50 load to a 100 line? and calculate the bandwidth for m=0.05? Solution 

Using table design for N=3 and ZL/Z0=2(reverse) can find coefficient as 1.8337, 1.4142, and 1.0907.