GUC (Dr. Hany Hammad) 4/20/2016

Similar documents
Periodic Structures. Filter Design by the Image Parameter Method

Lectur 22. RF and Microwave Circuit Design Γ-Plane and Smith Chart Analysis. ECE 303 Fall 2005 Farhan Rana Cornell University

Lecture 26: Quadrature (90º) Hybrid.

Some Families of Higher Order Three-Step Iterative Techniques. where is a real number and y (5)

Scattering Parameters. Scattering Parameters

Bohr type models of the atom give a totally incorrect picture of the atom and are of only historical significance.

Chapter 2 Linear Waveshaping: High-pass Circuits

Option 3. b) xe dx = and therefore the series is convergent. 12 a) Divergent b) Convergent Proof 15 For. p = 1 1so the series diverges.

Worksheet: Taylor Series, Lagrange Error Bound ilearnmath.net

PREPARATORY MATHEMATICS FOR ENGINEERS

07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n

Lecture 27: The 180º Hybrid.

How much air is required by the people in this lecture theatre during this lecture?

2. Finite Impulse Response Filters (FIR)

Chapter 2 Infinite Series Page 1 of 11. Chapter 2 : Infinite Series

1985 AP Calculus BC: Section I

z 1+ 3 z = Π n =1 z f() z = n e - z = ( 1-z) e z e n z z 1- n = ( 1-z/2) 1+ 2n z e 2n e n -1 ( 1-z )/2 e 2n-1 1-2n -1 1 () z

SAFE OPERATION OF TUBULAR (PFR) ADIABATIC REACTORS. FIGURE 1: Temperature as a function of space time in an adiabatic PFR with exothermic reaction.

Modern Physics. Unit 5: Schrödinger s Equation and the Hydrogen Atom Lecture 5.6: Energy Eigenvalues of Schrödinger s Equation for the Hydrogen Atom

Transmission Lines. Introduction to Transmission Lines (T.L.) Exercise Common Transmission Lines. Transmission Lines (TL) Don t worry about the

Lectures 9 IIR Systems: First Order System

ECE594I Notes set 6: Thermal Noise

Topic 5:Discrete-Time Fourier Transform (DTFT)

Even/Odd Mode Analysis of the Wilkinson Divider

Statistics 3858 : Likelihood Ratio for Exponential Distribution

Windowing in FIR Filter Design. Design Summary and Examples

MONTGOMERY COLLEGE Department of Mathematics Rockville Campus. 6x dx a. b. cos 2x dx ( ) 7. arctan x dx e. cos 2x dx. 2 cos3x dx

Narayana IIT Academy

x 2 x 3 x b 0, then a, b, c log x 1 log z log x log y 1 logb log a dy 4. dx As tangent is perpendicular to the x axis, slope

PURE MATHEMATICS A-LEVEL PAPER 1

ELEG 413 Lecture #6. Mark Mirotznik, Ph.D. Professor The University of Delaware

ELEC9721: Digital Signal Processing Theory and Applications

Probability & Statistics,

Washington State University

Exercises for lectures 23 Discrete systems

Impedance Transformation and Parameter Relations

ACTIVE FILTERS EXPERIMENT 2 (EXPERIMENTAL)

15/03/1439. Lectures on Signals & systems Engineering

Microwave Engineering

Another Explanation of the Cosmological Redshift. April 6, 2010.

MATH Midterm Examination Victor Matveev October 26, 2016

3. Electromagnetic Propagation in Anisotropic Media 3.1 Maxwell s Equations and Dielectric Tensor _

A Review of Complex Arithmetic

Time : 1 hr. Test Paper 08 Date 04/01/15 Batch - R Marks : 120

Chapter 3 Fourier Series Representation of Periodic Signals

(Reference: sections in Silberberg 5 th ed.)

Linear Algebra Existence of the determinant. Expansion according to a row.

Part B: Transform Methods. Professor E. Ambikairajah UNSW, Australia

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

Thomas Whitham Sixth Form

( ) ( ) (a) w(x) = a v(x) + b. (b) w(x) = a v(x + b) w = the system IS linear. (1) output as the sum of the outputs from each signal individually

Discrete Fourier Transform (DFT)

Impedance matching concept given ZL, design a matching network to have in=0 or selected value. matching. Zin (=Z Z o )

LECTURE 5 Guassian Wave Packet

ENGO 431 Analytical Photogrammetry

6. Negative Feedback in Single- Transistor Circuits

Digital Signal Processing, Fall 2006

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

EE 232 Lightwave Devices Lecture 3: Basic Semiconductor Physics and Optical Processes. Optical Properties of Semiconductors

. This is made to keep the kinetic energy at outlet a minimum.

Session : Plasmas in Equilibrium

H2 Mathematics Arithmetic & Geometric Series ( )

Continuous-Time Fourier Transform. Transform. Transform. Transform. Transform. Transform. Definition The CTFT of a continuoustime

Thomas Whitham Sixth Form

Taylor and Maclaurin Series

Operating parameters for representative BWR and PWR designs are given below. For the PWR hot channel and the BWR average channel compute and plot:

Frequency Measurement in Noise

IIT JEE MATHS MATRICES AND DETERMINANTS

Series and Parallel Resonances

Journal of Modern Applied Statistical Methods

Signals & Systems - Chapter 3

European Business Confidence Survey December 2012 Positive expectations for 2013

Math 656 Midterm Examination March 27, 2015 Prof. Victor Matveev

Discrete Fourier Transform. Nuno Vasconcelos UCSD

Solid State Device Fundamentals

Bipolar Junction Transistors

National Quali cations

Chapter 3. Hence, 3.2 (a) ( ) dt. (b) (d) using the. linearity property of the CTFT. Next, using the shifting property of the CTFT we get

Hadamard Exponential Hankel Matrix, Its Eigenvalues and Some Norms

Chapter Five. More Dimensions. is simply the set of all ordered n-tuples of real numbers x = ( x 1

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

(b) y(t) is not periodic although sin t and 4 cos 2πt are independently periodic.

The Frequency Response of a Quarter-Wave Matching Network

Further Results on Pair Sum Graphs

ASSERTION AND REASON

Analysis of the power losses in the three-phase high-current busducts

Equation Sheet Please tear off this page and keep it with you

ADORO TE DEVOTE (Godhead Here in Hiding) te, stus bat mas, la te. in so non mor Je nunc. la in. tis. ne, su a. tum. tas: tur: tas: or: ni, ne, o:

DISCRETE TIME FOURIER TRANSFORM (DTFT)

LECTURE 13 Filling the bands. Occupancy of Available Energy Levels

Class #24 Monday, April 16, φ φ φ

Power Spectrum Estimation of Stochastic Stationary Signals

GUC (Dr. Hany Hammad)

Numerical Method: Finite difference scheme

9.5 Complex variables

Motivation. We talk today for a more flexible approach for modeling the conditional probabilities.

The Acoustical Physics of a Standing Wave Tube

A Simple Proof that e is Irrational

COLLECTION OF SUPPLEMENTARY PROBLEMS CALCULUS II

READING ASSIGNMENTS. Signal Processing First LECTURE OBJECTIVES TIME & FREQUENCY. This Lecture: Lecture 13 Digital Filtering of Analog Signals

Transcription:

GU (r. Hay Hamma) 4/0/06 Lctur # 0 Filtr sig y Th srti Lss Mth sig Stps Lw-pass prttyp sig. () Scalig a cvrsi. () mplmtati. Usig Stus. Usig High-Lw mpac Sctis. Thry f priic structurs. mag impacs a Trasfr fuctis fr tw-prt twrks. r. Hay Hamma, Grma Uivrsity i air Stpp mpac Lw-Pass Filtrs y usig altratig sctis f vry high a vry lw charactristic impac lis. Kw as Stpp-impac r hi-, lw- filtrs. cs l j si l l j si l cs l, Rciprcal twrk j ct l j si l li j ct l j si l j si l j l ct OMM (603) Lctur #0

GU (r. Hay Hamma) 4/0/06 Stpp mpac Lw-Pass Filtrs T-Equivalt ircuit cs l j j si l j j si l si cs l / l X j ta j l / Stpp mpac Lw-Pass Filtrs X l ta si l l 4 f w hav a shrt lgth f li a larg charactristic impac f w hav a shrt lgth f li a small charactristic impac X l 0 highimpac X 0 Yl lwimpac h l l LR h (iuctr) l R l (capacitr) h l Rati shul as high as pssil OMM (603) Lctur #0

GU (r. Hay Hamma) 4/0/06 Exampl 8.6 sig a stpp-impac lw-pass filtr havig a maximally flat rsps a a cutff frqucy f.5 GHz. t is cssary t hav mr tha 0 isrti lss at 4 GHz. Th filtr impac is 50 ; th highst practical li impac is 0, a th lwst is 0. sir th ffct f lsss wh this filtr is implmt with a micrstrip sustrat havig =0.58 cm, r =4., ta = 0.0, a cppr cuctrs f 0.5 mil thickss. aswr c.5 GHz R 50 L 0 h 0 4 @ 4GHz 0.6 c.5 h l 0 6 l Exampl 8.6 6 OMM (603) Lctur #0 3

GU (r. Hay Hamma) 4/0/06 Exampl 8.6 g 0.57 g g g g g 3 4 5 6.44 L.93.93 L.44 3 4 5 0.57 L 6 Exampl 8.6 l l L R 0.57 0 50 l R.4450 0 h 0.068 0.589.849 33.759 OMM (603) Lctur #0 4

GU (r. Hay Hamma) 4/0/06 Exampl 8.6 Thry f priic structurs Priic structurs ifiit trasmissi li priically la with ractiv lmts is rfrr t as a priic structur. OMM (603) Lctur #0 5

GU (r. Hay Hamma) 4/0/06 alysis f ifiit priic structurs Lt k,k Y Whr k is th prpagati cstat f th ula li l cs kl jy si kl j si kl cs kl Y 0 ls assum rmaliz valu t alysis f ifiit priic structurs cs j si 0 cs j si si cs j j j si cs cs j si cs j si j si cs j cs j si si cs cs si cs si jcs si j si jcs si si cs cs si cs si cs si j j j cs cs si si cs si cs j j cs cs si cs si cs si jcs si j si cs si cs si cs cs si cs OMM (603) Lctur #0 6

GU (r. Hay Hamma) 4/0/06 OMM (603) Lctur #0 7 alysis f ifiit priic structurs si cs cs si cs si si cs j j alysis f ifiit priic structurs z z z z (0) ) ( (0) ) ( Or 0 Fr a wav prpagatig i th +v ircti. 0 0

GU (r. Hay Hamma) 4/0/06 alysis f ifiit priic structurs Fr a Rciprcal twrk i trms f S-paramtrs S S trm f Trasmissi paramtrs, usig cvrsi tals Fr a trivial sluti, th trmiat f th matrix must vaish 0 0 ( ) 0 ( ) 0 ivi y 0 csh ut a cs si hc alysis f ifiit priic structurs csh cs si assum j csh csh cs j sih si cs si Th ccrigly, Must hav ithr =0, r =0 as 0, 0, as 0, 0 j -attuatig (pass-a) (mplx ) cs cs si ttuatig (stp-a) (Ral ) csh cs si Sic cs Sic csh cs si cs si t li is lsslss, s pwr is t issipat it is just rflct ack t th iput. OMM (603) Lctur #0 8

GU (r. Hay Hamma) 4/0/06 alysis f ifiit priic structurs ttuatig (stp-a) (Ral ) -attuatig (pass-a) (mplx ) alysis f ifiit priic structurs OMM (603) Lctur #0 9

GU (r. Hay Hamma) 4/0/06 OMM (603) Lctur #0 0 alysis f ifiit priic structurs alysis f ifiit priic structurs haractristic impac (lch mpac) at th uit cll trmials is giv y 0 0 0 0 ) ( 4 ) ( ) ( 4 Fr symmtrical clls + Fr psitiv travlig wavs. Fr gativ travlig wavs. Frm th trmiat f th matrix 0 ) ( x x 4 t: th valus wr rmaliz

GU (r. Hay Hamma) 4/0/06 alysis f ifiit priic structurs t that is always imagiary Hc as 0, 0, as 0, 0 -attuatig (pass-a) jsi cs cs si ttuatig (stp-a) cs si cs si magiary Ral Ral magiary Similar t Prpagatig Ms Similar t Evasct ms ( prpagatig ms) Trmiat Priic Structurs j z z j z j (ssum passa) 0 z Scti j j j Th icit a rflct vltags at th th uit cll j j j OMM (603) Lctur #0

GU (r. Hay Hamma) 4/0/06 OMM (603) Lctur #0 Trmiat Priic Structurs t th la whr = L L (=) i cas f symmtrical clls L L L T avi trmial rflctis yu must hav L & als L & Hc L L Exampl 9. priic la li, if =50, =.0 cm, a =.666 pf, sktch th k- iagram a cmput th prpagati cstat, phas vlcity, a lch impac at f = 3.0 GHz. ssum k=k. swr si cs cs k k k k si cs cs is rmaliz t Y k k si cs cs Y Y & t k is fucti f S w will rwrit th fucti i trm f k

GU (r. Hay Hamma) 4/0/06 Exampl 9. k c k c c cs cs k k si k c.6660 5030 0 cs cs k k si k 8 Passa Stpa cs k k si k cs k k si k Th av quati ca valuat umrically fr giv valus f k k c Sic c a ar cstats yu ar plttig agaist frqucy Exampl 9. 0 0.96 k OMM (603) Lctur #0 3

GU (r. Hay Hamma) 4/0/06 Exampl 9. t 3.0 GHz, w hav 9 3 0 k (0.0) 0.683 36 8 30 cs cs(36) (0.683) si(36 ). 5 50 kc 0.683 vp 0. 4c.5 lch impac.56 k 0.683 cs si 0.0707 jsi cs j0.3479 j0.347950 0.0707 7. 4 j mag impacs & Trasfr fuctis f tw prt twrk Fi mag mpac a trasfr fucti if a tw prt twrk? mag mpac as fucti f th Paramtrs i = iput impac at prt wh prt is trmiat with i i = iput impac at prt wh prt is trmiat with i t that th rfrc ircti fr th currt at prt has chs accrig t th cvti fr trasmissi paramtrs. r. Hay Hamma, Grma Uivrsity i air OMM (603) Lctur #0 4

GU (r. Hay Hamma) 4/0/06 mag impacs & Trasfr fuctis f tw prt twrk hc put impac at prt, with prt trmiat with i i caus i i i i r. Hay Hamma, Grma Uivrsity i air mag impacs & Trasfr fuctis f tw prt twrk Rciprcal twrk i u t th currt ircti Slvig fr a y vrtig matrix r. Hay Hamma, Grma Uivrsity i air i i i OMM (603) Lctur #0 5

GU (r. Hay Hamma) 4/0/06 mag impacs & Trasfr fuctis f tw prt twrk W sir that i i & i i Frm i i & i i i i r. Hay Hamma, Grma Uivrsity i air ii i i i i Sutractig th quatis i i i i i i i i i ii i i i i i i & sic i i i f symmtrical twrk i i i i mag mpac as fucti f th Paramtrs mag impacs & Trasfr fuctis f tw prt twrk Th trasfr fucti f th twrk i trm f Similarly frm r. Hay Hamma, Grma Uivrsity i air i i t: x y x y t: x yx y x y x y Fr a symmtrical T r twrks th cfficit is uity OMM (603) Lctur #0 6

GU (r. Hay Hamma) 4/0/06 mag impacs & Trasfr fuctis f tw prt twrk (Rati) Fr rciprcal twrks this factr ca qual t uity. Prpagati factr f th twrk r. Hay Hamma, Grma Uivrsity i air mag impacs & Trasfr fuctis f tw prt twrk Lt j t: x y x y x yx y x y x y csh csh Symmtrical T r twrks ca us t sig th filtrs / / twrk r. Hay Hamma, Grma Uivrsity i air T twrk OMM (603) Lctur #0 7

GU (r. Hay Hamma) 4/0/06 mag mpac Prpagati stat Paramtrs mag impacs & Trasfr fuctis f tw prt twrk / / i csh i i 4 T r. Hay Hamma, Grma Uivrsity i air 4 csh 4 it 4 4 csh 4 mag impacs & Trasfr fuctis f tw prt twrk xt stp is t vlp th lw-pass a high-pass filtr scti. Shrt Lw frqucy Lw Pass Rsps Shrt High Frqucy Highpass Rsps r. Hay Hamma, Grma Uivrsity i air OMM (603) Lctur #0 8