ECE 344 Microwave Fundamentals

Similar documents
ECE Microwave Engineering

Lecture 26: Quadrature (90º) Hybrid.

Y 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall

ECE 2210 / 00 Phasor Examples

Chapter 6: Polarization and Crystal Optics

Linear-Phase FIR Transfer Functions. Functions. Functions. Functions. Functions. Functions. Let

Impedance Transformation and Parameter Relations

Lecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e

Voltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes

Addition of angular momentum

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

The pn junction: 2 Current vs Voltage (IV) characteristics

Definition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.

Addition of angular momentum

That is, we start with a general matrix: And end with a simpler matrix:

ECEN 5004, Spring 2018 Active Microwave Circuits Zoya Popovic, University of Colorado, Boulder LECTURE 2 SOME PASSIVE CIRCUITS

Lecture 27: The 180º Hybrid.

2/12/2013. Overview. 12-Power Transmission Text: Conservation of Complex Power. Introduction. Power Transmission-Short Line

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

Even/Odd Mode Analysis of the Wilkinson Divider

General Notes About 2007 AP Physics Scoring Guidelines

EEO 401 Digital Signal Processing Prof. Mark Fowler

Last time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same

The Transmission Line Wave Equation

ME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002

MCE503: Modeling and Simulation of Mechatronic Systems Discussion on Bond Graph Sign Conventions for Electrical Systems

2. Background Material

Classical Magnetic Dipole

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Function Spaces. a x 3. (Letting x = 1 =)) a(0) + b + c (1) = 0. Row reducing the matrix. b 1. e 4 3. e 9. >: (x = 1 =)) a(0) + b + c (1) = 0

The Matrix Exponential

Section 11.6: Directional Derivatives and the Gradient Vector

Exam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.

EE243 Advanced Electromagnetic Theory Lec # 23 Scattering and Diffraction. Reading: Jackson Chapter , lite

The Matrix Exponential

A Propagating Wave Packet Group Velocity Dispersion

Massachusetts Institute of Technology Department of Mechanical Engineering

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

orbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the

SAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS

There is an arbitrary overall complex phase that could be added to A, but since this makes no difference we set it to zero and choose A real.

6. The Interaction of Light and Matter

Einstein Equations for Tetrad Fields

Thus, because if either [G : H] or [H : K] is infinite, then [G : K] is infinite, then [G : K] = [G : H][H : K] for all infinite cases.

Lie Groups HW7. Wang Shuai. November 2015

α I I R α N I F I F i C i E R Cx R Ex C Cx i B R Bx

Theory and Applications of Transmission Lines

u 3 = u 3 (x 1, x 2, x 3 )

PH300 Modern Physics SP11 Final Essay. Up Next: Periodic Table Molecular Bonding

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

A 1 A 2. a) Find the wavelength of the radio waves. Since c = f, then = c/f = (3x10 8 m/s) / (30x10 6 Hz) = 10m.

Quasi-Classical States of the Simple Harmonic Oscillator

Impedance (T) EELE 461/561 Digital System Design. Module #3 Interconnect Modeling with Distributed Elements Topics. Transmission Lines

22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.

The Frequency Response of a Quarter-Wave Matching Network

10. The Discrete-Time Fourier Transform (DTFT)

What are those βs anyway? Understanding Design Matrix & Odds ratios

Sinusoidal Response Notes

EIE 332 Electromagnetics

4. (5a + b) 7 & x 1 = (3x 1)log 10 4 = log (M1) [4] d = 3 [4] T 2 = 5 + = 16 or or 16.

Scattering Parameters. Scattering Parameters

VII. Quantum Entanglement

Basic Polyhedral theory

5.80 Small-Molecule Spectroscopy and Dynamics

Synchronous machines

Chapter 6 Folding. Folding

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

Background: We have discussed the PIB, HO, and the energy of the RR model. In this chapter, the H-atom, and atomic orbitals.

Introduction to the quantum theory of matter and Schrödinger s equation

cycle that does not cross any edges (including its own), then it has at least

u x v x dx u x v x v x u x dx d u x v x u x v x dx u x v x dx Integration by Parts Formula

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, April 04, 2005, 8:35 AM) PART I: CHAPTER TWO COMB MATH.

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

System variables. Basic Modeling Concepts. Basic elements single and. Power = effort x flow. Power = F x v. Power = V x i. Power = T x w.

EXST Regression Techniques Page 1

Principles of active remote sensing: Lidars. 1. Optical interactions of relevance to lasers. Lecture 22

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

CHAPTER 10. Consider the transmission lines for voltage and current as developed in Chapter 9 from the distributed equivalent circuit shown below.

2F1120 Spektrala transformer för Media Solutions to Steiglitz, Chapter 1

Alpha and beta decay equation practice

Coupled Pendulums. Two normal modes.

EAcos θ, where θ is the angle between the electric field and

Hydrogen Atom and One Electron Ions

Electronic Circuits. BJT Amplifiers. Manar Mohaisen Office: F208 Department of EECE

1 Isoparametric Concept

Ch. 24 Molecular Reaction Dynamics 1. Collision Theory

Contemporary, atomic, nuclear, and particle physics

Optics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007

1 1 1 p q p q. 2ln x x. in simplest form. in simplest form in terms of x and h.

From Elimination to Belief Propagation

2. Laser physics - basics

Seebeck and Peltier Effects

TRANSISTOR AND DIODE STUDIES. Prof. H. J. Zimmermann Prof. S. J. Mason C. R. Hurtig Prof. R. B. Adler Dr. W. D. Jackson R. E.

Derivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian

Higher order derivatives

Thomas Whitham Sixth Form

Title: Vibrational structure of electronic transition

Math 34A. Final Review

Gradebook & Midterm & Office Hours

Transcription:

ECE 44 Microwav Fundamntals Lctur 08: Powr Dividrs and Couplrs Part Prpard By Dr. hrif Hkal 4/0/08

Microwav Dvics 4/0/08

Microwav Dvics 4/0/08

Powr Dividrs and Couplrs Powr dividrs, combinrs and dirctional couplrs ar passiv structurs that divid RF input powr among svral outputs or combin powr from svral inputs. Powr Dividrs and Combinrs Usd to split input powr into roughly qual outputs, or vic vrsa. Dirctional Couplrs Usd to sampl a fraction of input powr and/or to sparat forward and rvrs travling wavs. 4/0/08 4

Powr Dividrs and Couplrs Ths ar xampls of a thr-port ntwork. A powr dividr is usd to split a signal. P P P P P A couplr/combinr is usd to combin a signal. P P P P P Goal: Distribut powr from on input among svral outputs, or combin powr from svral inputs to on output. Problms for RF and microwav dsigns Impdanc match Isolation Phas rlationships among signals 4/0/08 5

Thr Port Ntworks Gnral -port ntwork: 4/0/08 6

Thr Port Ntworks (cont.) If all thr ports ar matchd, and th dvic is rciprocal and losslss, w hav: 0 0 0 (Th matrix is also unitary.) (Thr ar thr distinct valus.) This is not physically possibl! (s nxt slid) 4/0/08 7

Powr Dividrs and Couplrs (cont.) 0 0 0 Unitary: not physically possibl Losslss [] is unitary Ths cannot all b satisfid. (If only on is nonzro, w cannot satisfy all thr.) 4/0/08 0 0 0 At last of,, must b zro. (If only on is zro (or non is zro), w cannot satisfy all thr.) 8

Unitary Matrix It can b don in an asy way: Th dot product of any column of [] with th conjugat of that column givs unity. Th dot product of any column with th conjugat of a diffrnt column givs zro (orthogonal). 4/0/08 9

Circulators Now considr a -port ntwork that is non-rciprocal, with all ports matchd, and is losslss: 0 0 0 (Thr ar six distinct valus.) Circulator Ths quations will b satisfid if: Losslss 0 4/0/08 0 0 0 or Not that ij ji. 0 0

Circulators (cont.) 0 0 0 0 0 0 Not: W hav assumd hr that th phass of all th paramtrs ar zro. Clockwis (LH) circulator 0 0 0 0 0 0 Circulators can b mad using biasd frrit matrials. 4/0/08 Countr-clockwis (RH) circulator

Powr Dividrs T-Junction: losslss dividr Y in 0 0 Y in 0 0 To match: Not, howvr, Y 0 0 0 in 0 0 0 0 Thus, Yi n Also, Y 0 Y in 0 0 0 0 0 0 0 0 00 0 00 0 0 in 0 0 4/0/08 If w match at port, w cannot match at th othr ports!

Powr Dividrs (cont.) Assuming port matchd: P 0 0 0 0 0 0 in 0 0 0 out in in in 0 0 0 0 P P P K P 0 0 out in in in 0 0 0 0 P P P K P 0 0 4/0/08 W can dsign th splittr to control th powrs into th two output lins.

Powr Dividrs (cont.) Examin th rflction at ach port ( ii ): 0 / 0 / 0 a a 0 aa0 0 0 in 0 0 0 0 in 0 0 0 0 a a 0 a a 0 0 0 0 0 0 0 0 0 0 0 0 0 4/0/08 zro if port is matchd Not: A match on port rquirs 0 0 0 0 (sinc th two output lins combin in paralll) 0, 0 4

Powr Dividrs (cont.) Also, w hav: 0 0 a a 0 0 0 0 ; / / 0 0 imilarly, and 0 0 0 0 4/0/08 5

Powr Dividrs (cont.) If port is matchd: 0 0 0 0 0 0 ; ; 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 Only 0 4/0/08 Th output ports ar not isolatd. 6

Output powrs: Powr Dividrs (cont.) P 0 P 0 0 P 0 P 0 0 Not: P is th input powr on port. Hnc P P 0 0 Chck : P P P P P P 0 0 0 0 0 0 4/0/08 7

Powr Dividrs (cont.) ummary 0 0 0 0 0 0 0 P P 0 0 0; ; 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 4/0/08 0 0 0 Th input port is matchd, but not th output ports. Th output ports ar not isolatd. Wavs rflctd from dvics on ports and with caus intrfrnc with th dvics. 8

Powr Dividrs (cont.) Exampl: Microstrip T-junction powr dividr 0 0 50 [ ] Incidnt 0 00 [ ] 0 0 0 0 50 00. [ ] 0 00 [ ] 4/0/08 9

Powr Dividrs (cont.) Th matchd powr dividr also works as a match powr combinr 0 0 50 [ ] 0 00 [ ] Incidnt 0 0 0 0 50 00. [ ] 0 00 [ ] b a a 0 a Equal wavs ar incidnt from ports and. 4/0/08 0

Rsistiv Powr Dividr in 4 4 0 0 0 0 0 (Th sam for in and in.) 0 0 in 0 0 0 0 0 All ports ar matchd. 0 4/0/08

Rsistiv Powr Dividr (cont.) 0 0 a a 0 0 0 0 0 0 0 4 0 in 0 0 0 By rciprocity and symmtry 0 0 4/0/08

Rsistiv Powr Dividr (cont.) Hnc w hav 0 0 0 P P a in 0 0 in 0 0 0 0 0 P P P b a P P 4 in All ports ar matchd, but / P in is dissipatd by rsistors, and th output ports ar not isolatd. 4/0/08

Evn-Odd Mod Analysis (This is ndd for analyzing th Wilkinson) Exampl: W want to solv for. W do this using vn/odd mod analysis. (This works bcaus th circuit itslf is symmtric.) Corrct answr : 4/0/08 4

Evn-Odd Mod Analysis Lt o Plan of symmtry o o o Evn problm Odd problm o 4/0/08 5

Evn-Odd Mod Analysis (cont.) Evn problm PO I 0 4 4 4 4 4 4/0/08 6

Evn-Odd Mod Analysis (cont.) Odd problm o o o o 0 4 4 hort circuit (C) plan of symmtry 4 o o 0 4/0/08 7

Evn-Odd Mod Analysis (cont.) By suprposition: o 0 Hnc w hav 4/0/08 8

Wilkinson Powr Dividr Equal-split ( db) powr dividr (Th Wilkinson can b dsignd to hav an unqual split.) g / 4 0 0 0 0 All ports matchd ( = = = 0) Output ports ar isolatd ( = = 0) g / 4 0 0 Not: No powr is lost in going from port to ports and. 0 j 0 0 0 0 4/0/08 Obviously not unitary 9

Wilkinson Powr Dividr (cont.) Exampl: Microstrip Wilkinson powr dividr 0 50 [ ] 0 50 [ ] 0T 70.7 [ ] 0T 70.7 [ ] R 00 [ ] 0 50 [ ] 4/0/08 0

Wilkinson Powr Dividr (cont.) Evn and odd analysis is usd to analyz th structur whn port is xcitd. To dtrmin, Only vn analysis is ndd to analyz th structur whn port is xcitd. To dtrmin, Th othr componnts can b found by using symmtry and rciprocity. 4/0/08

Wilkinson Powr Dividr (cont.) Top viw 0 / 4 g g 0 / 4 0 0 Plan of symmtry 0 0 A microstrip ralization is shown. plit structur along plan of symmtry (PO) Evn voltag vn about PO plac OC along PO Odd voltag odd about PO plac C along PO 4/0/08

Wilkinson Powr Dividr (cont.) 0 / 4 0 g g 0 / 4 0 0 0 How do you split a transmission lin? (This is ndd for th vn cas.) Top viw I / 0 oltag is th sam for ach half of lin () Currnt is halvd for ach half of lin (I/) I / (magntic wall) I h 0 0 0 microstrip lin 4/0/08 For ach half

Wilkinson Powr Dividr (cont.) Evn Problm g / 4 0 Not: Th 0 rsistor has bn split into two 0 rsistors in sris. 0 0 0 0 OC Ports and ar xcitd in phas. OC 0 0 g / 4 0 4/0/08 Not : 4

Wilkinson Powr Dividr (cont.) Odd problm g / 4 0 o 0 0 o Not: Th 0 rsistor has bn split into two 0 rsistors in sris. 0 o o Ports and ar xcitd 80 o out of phas. 0 0 0 g / 4 o 0 o 4/0/08 Not : 0, o o o 5

Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation g / 4, in 0 Port 0 0 OC 0 in 0 0 in 0 in 0 0 Rcall: in T (quartr-wav transformr) L Also, by symmtry, 0 4/0/08 6

Wilkinson Powr Dividr (cont.) Odd Problm Port xcitation g / 4 0 o, o o in 0 0 o Port 0 o o 0 hort o in 0 0 o o in 0 o in 0 0 4/0/08 Also, by symmtry, o 0 7

Wilkinson Powr Dividr (cont.) W add th rsults from th vn and odd cass togthr: a a 0 o o o 0 0 0 0 (by symmtry) a a 0 o o o 0 0 0 0 (by rciprocity) Not: inc all ports hav th sam 0, w ignor th normalizing factor 0 in th paramtr dfinition. 4/0/08 In summary, for port xcitation, w hav: 0 0 0 8

Wilkinson Powr Dividr (cont.) Port xcitation Port g / 4 0 0 g / 4 0 0 0 0 Whn port is xcitd, th rspons, by symmtry, is vn. (Hnc, th total filds ar th sam as th vn filds.) 4/0/08 9

Wilkinson Powr Dividr (cont.) Evn Problm Port 0 g / 4 0 0 0 0 0 O.C. symmtry plan 0 g / 4 0 OC 0 g / 4 4/0/08 40

Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation Port 0 g / 4 0 OC 0 0 in 0 0 in 0 in 0 0, in Hnc a a 0 a 0 0 0 4/0/08 4

Wilkinson Powr Dividr (cont.) Evn Problm Port xcitation a a 0 Port 0 g / 4 0 0 z OC j j 4/0/08 j (rciprocal) Along g /4 wav transformr: jz jz 0 z z 0 0 g /4 j 0 0 0 0 0 distanc from port 4

Wilkinson Powr Dividr (cont.) For th othr componnts: By symmtry: j By rciprocity: j 4/0/08 4

Wilkinson Powr Dividr (cont.) 0 j 0 0 0 0 g / 4 0 0 0 0 0 g / 4 0 0 0 All thr ports ar matchd, and th output ports ar isolatd. 4/0/08 44

Wilkinson Powr Dividr (cont.) 0 j 0 0 0 0 g / 4 0 0 j 0 0 g / 4 0 0 j Whn a wav is incidnt from port, half of th total incidnt powr gts transmittd to ach output port (no loss of powr). Whn a wav is incidnt from port or port, half of th powr gts transmittd to port and half gts absorbd by th rsistor, but nothing gts through to th othr output port. 4/0/08 45

Wilkinson Powr Dividr (cont.) Figur 7.5 of Pozar Photograph of a four-way corporat powr dividr ntwork using thr microstrip Wilkinson powr dividrs. Not th isolation chip rsistors. Courtsy of M.D. Abouzahra, MIT Lincoln Laboratory. 4/0/08 46

Wilkinson Powr Dividr (cont.) Figur 7. of Pozar Frquncy rspons of an qual-split Wilkinson powr dividr. Port is th input port; ports and ar th output ports. 4/0/08 47