EECE 301 Signals & Systems Prof. Mark Fowler

Similar documents
EECE 260 Electrical Circuits Prof. Mark Fowler

Equations from Relativistic Transverse Doppler Effect. The Complete Correlation of the Lorentz Effect to the Doppler Effect in Relativistic Physics

Equations from The Relativistic Transverse Doppler Effect at Distances from One to Zero Wavelengths. Copyright 2006 Joseph A.

International Journal of Scientific & Engineering Research, Volume 4, Issue 9, September ISSN

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

Multi-Section Coupled Line Couplers

Last time: introduced our first computational model the DFA.

Path (space curve) Osculating plane

Topic 5: Discrete-Time Fourier Transform (DTFT)

MATHEMATICS FOR MANAGEMENT BBMP1103

ME 236 Engineering Mechanics I Test #4 Solution

Lecture 35. Diffraction and Aperture Antennas

Lecture 11 Waves in Periodic Potentials Today: Questions you should be able to address after today s lecture:

More on FT. Lecture 10 4CT.5 3CT.3-5,7,8. BME 333 Biomedical Signals and Systems - J.Schesser

How to Use. The Bears Beat the Sharks!

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:

Lecture 4. Electric Potential

Chapter 2 Reciprocal Lattice. An important concept for analyzing periodic structures

Section 3: Antiderivatives of Formulas

EEO 401 Digital Signal Processing Prof. Mark Fowler

OVERVIEW Using Similarity and Proving Triangle Theorems G.SRT.4

More Foundations. Undirected Graphs. Degree. A Theorem. Graphs, Products, & Relations

3.1 General solutions for TEM, TE and TM waves Procedure to analyze a TEM (Ez, Hz=0) line

ELEC 351 Notes Set #18

Lecture 26: Quadrature (90º) Hybrid.

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

Helping every little saver

Frequency Response. Lecture #12 Chapter 10. BME 310 Biomedical Computing - J.Schesser

MAT 1275: Introduction to Mathematical Analysis

Let s celebrate! UNIT. 1 Write the town places. 3 Read and match. school. c 1 When s your birthday? Listen, check and practise the dialogues.

1 Error Analysis of Simple Rules for Numerical Integration

C-Curves. An alternative to the use of hyperbolic decline curves S E R A F I M. Prepared by: Serafim Ltd. P. +44 (0)

Walk Like a Mathematician Learning Task:

ECE 2100 Circuit Analysis

Measurement of Residual Stress/Strain (Using Strain Gages and the Hole Drilling Method) Summary of Discussion in Section 8.9

Axe Wo. Blood Circle Just like with using knives, when we are using an axe we have to keep an area around us clear. Axe Safety Check list:

Lecture 27: The 180º Hybrid.

ME 522 PRINCIPLES OF ROBOTICS. FIRST MIDTERM EXAMINATION April 19, M. Kemal Özgören

Electric Potential Energy

[ ] [ ] DFT: Discrete Fourier Transform ( ) ( ) ( ) ( ) Congruence (Integer modulo m) N-point signal

1 Introduction to Modulo 7 Arithmetic

Daily Skill Practice

IMPOSSIBLE NAVIGATION

09/29/2009 Reading: Hambley Chapter 5 and Appendix A

Selecting Your Digital Leader

GUC (Dr. Hany Hammad)

1 PreCalculus AP Unit G Rotational Trig (MCR) Name:

A 2 ab bc ca. Surface areas of basic solids Cube of side a. Sphere of radius r. Cuboid. Torus, with a circular cross section of radius r

this is called an indeterninateformof-oior.fi?afleleitns derivatives can now differentiable and give 0 on on open interval containing I agree to.

ECE COMBINATIONAL BUILDING BLOCKS - INVEST 13 DECODERS AND ENCODERS

TURFGRASS DISEASE RESEARCH REPORT J. M. Vargas, Jr. and R. Detweiler Department of Botany and Plant Pathology Michigan State University

# 1 ' 10 ' 100. Decimal point = 4 hundred. = 6 tens (or sixty) = 5 ones (or five) = 2 tenths. = 7 hundredths.

The Theory of Small Reflections

WYSE Academic Challenge Sectional Mathematics 2006 Solution Set

INTEGRALS. Chapter 7. d dx. 7.1 Overview Let d dx F (x) = f (x). Then, we write f ( x)

ALGEBRA 2/TRIGONMETRY TOPIC REVIEW QUARTER 3 LOGS

EE 119 Homework 6 Solution

² Ý ² ª ² Þ ² Þ Ң Þ ² Þ. ² à INTROIT. huc. per. xi, sti. su- sur. sum, cum. ia : ia, ia : am, num. VR Mi. est. lis. sci. ia, cta. ia.

Protect yourself from flu

Chapter 2 Linear Waveshaping: High-pass Circuits

COMP108 Algorithmic Foundations

5.1 Properties of Inverse Trigonometric Functions.

Preview. Graph. Graph. Graph. Graph Representation. Graph Representation 12/3/2018. Graph Graph Representation Graph Search Algorithms

Propagation of Light About Rapidly Rotating Neutron Stars. Sheldon Campbell University of Alberta

Part a: Writing the nodal equations and solving for v o gives the magnitude and phase response: tan ( 0.25 )

(2) If we multiplied a row of B by λ, then the value is also multiplied by λ(here lambda could be 0). namely

Fourier Transform Fast Fourier Transform discovered by Carl Gauss ~1805 re- re invented by Cooley & Tukey in 1965

This immediately suggests an inverse-square law for a "piece" of current along the line.

So He Thought He Should Dance

User s Guide. Electronic Crossover Network. XM66 Variable Frequency. XM9 24 db/octave. XM16 48 db/octave. XM44 24/48 db/octave. XM26 24 db/octave Tube

Handout 7. Properties of Bloch States and Electron Statistics in Energy Bands

XV Quantum Electrodynamics

Lecture contents. Bloch theorem k-vector Brillouin zone Almost free-electron model Bands Effective mass Holes. NNSE 508 EM Lecture #9

3 What You Should Know About Complex Numbers

2. Background Material

Let's celebrate Europe's day

- Prefix 'audi', 'photo' and 'phobia' - What's striped and bouncy? A zebra on a trampoline!

Lecture 5: Equilibrium and Oscillations

Supplementary Course Notes Adding and Subtracting AC Voltages and Currents

Lecture 4. Conic section

I. Signals & Sinusoids

SOUTH LAMBETH ESTATE REGENERATION DESIGN FOCUS - PRECEDENT SCHEMES

TOPIC 5: INTEGRATION

Sinusoidal Forcing of a First-Order Process. / τ

EEO 401 Digital Signal Processing Prof. Mark Fowler

( ) Frequency Response Analysis. Sinusoidal Forcing of a First-Order Process. Chapter 13. ( ) sin ω () (

Unit 3: Transistor at Low Frequencies

Relationships Between Frequency, Capacitance, Inductance and Reactance.

11.2. Infinite Series

MASTER CLASS PROGRAM UNIT 4 SPECIALIST MATHEMATICS SEMESTER TWO 2014 WEEK 11 WRITTEN EXAMINATION 1 SOLUTIONS

Unit 6: Playing with Word Patterns in Musical Theater Songs

The Fourier Transform (and more )

IMU Theory: Earth and Body Frames

ECE 2100 Circuit Analysis

Errata for Second Edition, First Printing

d n 1 f dt n 1 + K+ a 0f = C cos(ωt + φ)

GENERAL FORMULAS FOR FLAT-TOPPED WAVEFORMS. J.e. Sprott. Plasma Studies. University of Wisconsin

12/3/12. Outline. Part 10. Graphs. Circuits. Euler paths/circuits. Euler s bridge problem (Bridges of Konigsberg Problem)

Chapter DEs with Discontinuous Force Functions

5/9/13. Part 10. Graphs. Outline. Circuits. Introduction Terminology Implementing Graphs

Transcription:

EECE 301 Signls & Systms Pf. Mk Fwl Discussin #1 Cmplx Numbs nd Cmplx-Vlud Functins Rding Assignmnt: Appndix A f Kmn nd Hck

Cmplx Numbs Cmplx numbs is s ts f plynmils. Dfinitin f imginy # j nd sm sulting pptis: j ( ( 1 j)( j) 1 j)( j 1 j) 1 Rcll tht th slutin f diffntil qutins invlvs finding ts f th chctistic plynmil S Rctngul fm f cmplx numb: jb l numbs R{ } b Im{ } Th uls f dditin nd multiplictin stight-fwd: Add : ( Multiply : ( jb) ( c jb)( c jd) ( jd) ( c c) j( b bd) j( d d) bc)

Pl Fm j > 0 Pl fm n ltnt wy t xpss cmplx numb Pl Fm gd f multiplictin nd divisin Nt: yu my hv lnd pl fm s w will NOT us tht h!! Th dvntg f th j is tht whn it is mnipultd using uls f xpnntils nd it bhvs pply ccding t th uls f cmplx #s: ( x )( y ) x y x / y x y Multiplying Using Pl Fm ( j )( ) 1 j j( 1 ) n 1 ( j ) n 1/ n 1/ n j / n n 1 jn Dividing Using Pl Fm ( j ) 1 ( j ) 1 1 j( 1 ) 1 1 1 j j

W nd t b bl cnvt btwn Rctngul nd Pl Fms this is md sy nd bvius by lking t th gmty (nd tignmty) f cmplx #s: Gmty f Cmplx Numbs b Im jb R b b Cnvsin Fmuls sin cs tn 1 b b

Q: Why th fm j f pl fm?? Stt with tignmty: [ cs j sin ] jb cs j( sin ) 4 6 Fm Clc II: cs 1...! 4! 6! j sin j 3 j 3! 5 j 5! 7 j 7!... cs j sin 1 j! 3 j 3! 4 4!... Als Fm Clc II: x 1 x x! 3 x 3! 4 x 4!... j 1 j! 3 j 3! 4 4!... Sinc cs jsin hs th sm xpnsin s j w cn sy tht: cs j sin j

Cmplx Expnntils vs. Sins nd Csins Eul s Equtins: (A) (B) (C) (D)

Summy f Rctngul & Pl Fms Rct Fm: jb R{ } cs Im{ } b sin Pl Fm: j tn b 1 0 b ( π, π ] Wning: Yu clcult will giv yu th wng nsw whnv yu hv < 0. In th wds, f vlus tht li in th II nd III qudnts. Yu cn lwys fix this by ith dding subtcting π. Us cmmn sns lking t th signs f nd b will tll yu wht qudnt is in mk su yu ngl gs with tht!!!

Cnjugt f Z Dntd s * jb * jb j * j Pptis f * 1. * R{ }. * ( jb)( jb) b

Unit Cicl 1 Im R Unit Cicl: A st f cmplx numbs with mgnitud f 1 ( 1) All n th unit cicl lk lik: j 1 Fu spcil pints n th unit cicl: jπ 1 Im jπ j j 1 jπ j0 R ± jnπ ± jnπ jnπ Knw ths!!! 1, n dd intg 1, n vn intg 1 f ll intgs j, n 1,5,9,... j, n 3,7,11,... 1, n 0, 4,8,... 1, n,6,10,...

A sinusid is cmpltly dfind by its th pmts: -Amplitud A (f EE s typiclly in vlts mps th physicl unit) -Fquncy ω in dins p scnd -Phs shift φ in dins T is th pid f th sinusid nd is ltd t th fquncy

Fquncy cn b xpssd in tw cmmn units: -Cyclic fquncy: f 1/T in H (1 H 1 cycl/scnd) -Rdin Fquncy: ω π/t (in dins/scnd) Fm this w cn s tht ths tw fquncy units hv simpl cnvsin fct ltinship (lik ll th unit cnvsins.g. ft nd mts): ω πf Phs shift (ftn just shtnd t phs) shws up xplicitly in th qutin but shws up in th plt s tim shift (bcus th plt is functin f tim). Q: Wht is th ltinship btwn th plt-bsvd tim shift nd th qutinspcifid phs shift? A: W cn wit th tim shift f functin by plcing t by t t (m n this lt, but yu shuld b bl t vify tht this is tu!) Thn w gt: f ( t t) Asin( ω ( t t)) Asin( ωt ωt) S w gt tht: φ ωt (unit-wis this mks sns!!!) φ

In cicuits yu usd phss (w ll cll thm sttic phss h) th pint f using thm is t mk it EASY t nly cicuits tht divn by singl sinusid. H is n xmpl t fsh yu mmy!! Find utput vltg f th fllwing cicuit: R 1Ω ( ) x( t) 5cs 1000t π 4 L mh y( t)? Us phs nd impdnc ids: Impdnc f Induct : Phs f Input : xˆ 5 Z L jπ 4 jωl Us vltg divid t find utput: yˆ j xˆ 1 j 5 jπ [ ] j0.46 0. 4 89 j Output phs: y ˆ 4.45 Output signl: y( t) 4.45cs(1000t 1.5) j1.5

Nt tht in using sttic phss th ws n nd t cy und th fquncy it gts suppssd in th sttic phs BUT if yu hv multipl diving sinusids (ch t its wn uniqu fquncy) thn yu ll nd t kp tht fquncy in th phs psnttin tht lds t: Rtting Phss Kping th fquncy pt A jω t R cs( ω t cs( ω t) j sin( ω t) { jφ jω t} A A cs( ω t φ ) input tting phs φ ) A cs( ω t φ ) A A A sttic phs pt jφ j( ω t φ ) jφ jω t jω t systm Mdifid systm utput tting phs Rtting phs

If ~ x ( t) [ ω t φ ] ( x( t) Acs( ω t φ )) Wht is : A ~ x *( t) [ ω t φ ] jφ jωt A ~ x ( t) ~ x *( t) R{ ~ x ( t) } Acs( ω t j A j φ ) Bcus tting phss tk th vlu f cmplx numb t ch Instnt f tim thy must fllw ll th uls f cmplx numbs Espcilly: EULER S EQUATIONS!!

Rtting Phss Eul s Equtins

Viwing tting phs n th cmplx pln