Lectures 9-11: Fourier Transforms

Similar documents
Consider a system of 2 simultaneous first order linear equations

The Variance-Covariance Matrix

Frequency Response. Response of an LTI System to Eigenfunction

Theoretical Seismology

Summary: Solving a Homogeneous System of Two Linear First Order Equations in Two Unknowns

Wave Superposition Principle

t=0 t>0: + vr - i dvc Continuation

EE243 Advanced Electromagnetic Theory Lec # 10: Poynting s Theorem, Time- Harmonic EM Fields

Advanced Queueing Theory. M/G/1 Queueing Systems

ELEN E4830 Digital Image Processing

Boosting and Ensemble Methods

9. Simple Rules for Monetary Policy

Supplementary Figure 1. Experiment and simulation with finite qudit. anharmonicity. (a), Experimental data taken after a 60 ns three-tone pulse.

Lecture 1: Numerical Integration The Trapezoidal and Simpson s Rule

Chapter 13 Laplace Transform Analysis

Homework: Introduction to Motion

Lecture 12: Introduction to nonlinear optics II.

Problem 1: Consider the following stationary data generation process for a random variable y t. e t ~ N(0,1) i.i.d.

Partition Functions for independent and distinguishable particles

CIVL 8/ D Boundary Value Problems - Triangular Elements (T6) 1/8

Chapter 9 Transient Response

Physics 256: Lecture 2. Physics

MECE 3320 Measurements & Instrumentation. Static and Dynamic Characteristics of Signals

innovations shocks white noise

State Observer Design

Control Systems (Lecture note #6)

Double Slits in Space and Time

Charging of capacitor through inductor and resistor

Bethe-Salpeter Equation Green s Function and the Bethe-Salpeter Equation for Effective Interaction in the Ladder Approximation

4.1 The Uniform Distribution Def n: A c.r.v. X has a continuous uniform distribution on [a, b] when its pdf is = 1 a x b

CSE 245: Computer Aided Circuit Simulation and Verification

UNIT #5 EXPONENTIAL AND LOGARITHMIC FUNCTIONS

FAULT TOLERANT SYSTEMS

OUTLINE FOR Chapter 2-2. Basic Laws

The Fourier Transform

Gauge Theories. Elementary Particle Physics Strong Interaction Fenomenology. Diego Bettoni Academic year

Boyce/DiPrima 9 th ed, Ch 2.1: Linear Equations; Method of Integrating Factors

Chap 2: Reliability and Availability Models

FI 3103 Quantum Physics

SIMEON BALL AND AART BLOKHUIS

The Mathematics of Harmonic Oscillators

Lecture 3: Phasor notation, Transfer Functions. Context

Conventional Hot-Wire Anemometer

Phys463.nb Conductivity. Another equivalent definition of the Fermi velocity is

Continous system: differential equations

Lecture 4 : Backpropagation Algorithm. Prof. Seul Jung ( Intelligent Systems and Emotional Engineering Laboratory) Chungnam National University

Ergodic Capacity of a SIMO System Over Nakagami-q Fading Channel

Final Exam : Solutions

Fourier Series: main points

Institute of Actuaries of India

Surface Impedance of Superconductors and Normal Conductors in EM Simulators 1

(heat loss divided by total enthalpy flux) is of the order of 8-16 times

A Propagating Wave Packet Group Velocity Dispersion

Grand Canonical Ensemble

Thermodynamic Properties of the Harmonic Oscillator and a Four Level System

The Hyperelastic material is examined in this section.

Physics 160 Lecture 3. R. Johnson April 6, 2015

10.5 Linear Viscoelasticity and the Laplace Transform

Midterm exam 2, April 7, 2009 (solutions)

Chapter 7: Plane Electromagnetic Waves and Wave Propagation

Lecture 14. Relic neutrinos Temperature at neutrino decoupling and today Effective degeneracy factor Neutrino mass limits Saha equation

Chapter 12 Introduction To The Laplace Transform

Lecture 37 (Schrödinger Equation) Physics Spring 2018 Douglas Fields

CHAPTER CHAPTER14. Expectations: The Basic Tools. Prepared by: Fernando Quijano and Yvonn Quijano

Elementary Differential Equations and Boundary Value Problems

167 T componnt oftforc on atom B can b drvd as: F B =, E =,K (, ) (.2) wr w av usd 2 = ( ) =2 (.3) T scond drvatv: 2 E = K (, ) = K (1, ) + 3 (.4).2.2

CHAPTER 33: PARTICLE PHYSICS

Chapter 5 The Laplace Transform. x(t) input y(t) output Dynamic System

Let s look again at the first order linear differential equation we are attempting to solve, in its standard form:

Introduction to Fourier Transform

Safety and Reliability of Embedded Systems. (Sicherheit und Zuverlässigkeit eingebetteter Systeme) Stochastic Reliability Analysis

Economics 302 (Sec. 001) Intermediate Macroeconomic Theory and Policy (Spring 2011) 3/28/2012. UW Madison

SECTION where P (cos θ, sin θ) and Q(cos θ, sin θ) are polynomials in cos θ and sin θ, provided Q is never equal to zero.

k of the incident wave) will be greater t is too small to satisfy the required kinematics boundary condition, (19)

TIME-DOMAIN EQUIVALENT EDGE CURRENT (EEC's) TECHNIQUE TO IMPROVE A TLM-PHYSICAL OPTICS HYBRID PROCEDURE

Retarded Interaction of Electromagnetic field and Symmetry Violation of Time Reversal in Non-linear Optics

Lucas Test is based on Euler s theorem which states that if n is any integer and a is coprime to n, then a φ(n) 1modn.

Searching for pairing interactions with coherent charge fluctuations spectroscopy

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

Effect of sampling on frequency domain analysis

NAME: ANSWER KEY DATE: PERIOD. DIRECTIONS: MULTIPLE CHOICE. Choose the letter of the correct answer.

Voltage v(z) ~ E(z)D. We can actually get to this wave behavior by using circuit theory, w/o going into details of the EM fields!

Dr. Junchao Xia Center of Biophysics and Computational Biology. Fall /21/2016 1/23

Mechanics Physics 151

Lecture 23. Multilayer Structures

EXERCISE - 01 CHECK YOUR GRASP

Vertical Sound Waves

2.1. Differential Equations and Solutions #3, 4, 17, 20, 24, 35

8. Queueing systems. Contents. Simple teletraffic model. Pure queueing system

On the Derivatives of Bessel and Modified Bessel Functions with Respect to the Order and the Argument

Chapters 2 Kinematics. Position, Distance, Displacement

Chapter 7 Stead St y- ate Errors

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.

Safety and Reliability of Embedded Systems. (Sicherheit und Zuverlässigkeit eingebetteter Systeme) Stochastic Reliability Analysis

Microscopic Flow Characteristics Time Headway - Distribution

Chapter 7. Now, for 2) 1. 1, if z = 1, Thus, Eq. (7.20) holds

Two-Dimensional Quantum Harmonic Oscillator

8-node quadrilateral element. Numerical integration

Solution in semi infinite diffusion couples (error function analysis)

10/7/14. Mixture Models. Comp 135 Introduction to Machine Learning and Data Mining. Maximum likelihood estimation. Mixture of Normals in 1D

Transcription:

Lcurs 9-: ourr Transforms Rfrncs Jordan & Smh Ch7, Boas Ch5 scon 4, Kryszg Ch Wb s hp://wwwjhudu/sgnals/: go o Connuous Tm ourr Transform Proprs PHY6 Inroducon o ourr Transforms W hav sn ha any prodc funcon can b rprsnd by a ourr srs and ha any puls can b rprsnd by a half rang ourr srs In boh cass h shap s formd from summd sn and/or cosn rms of spcfc harmonc frquncs and ampluds Somms w may wsh o sudy hs dsrbuon of frquncs rahr han sar a h fnal summd ourr srs S blow from jhudu Two qusons may occur o us: Is hr anyhng analogous o a ourr srs for a funcon whch s no prodc? Th frquncs ncludd n h ourr sum s an nfn s n aks valus from o nfny bu by no mans ncluds all possbl frquncs s a dscr s of frquncs n s rsrcd o ngr valus, no a connuous spcrum Can w somhow modfy h srs o conan a connuous spcrum? Snc an ngral s h lm of a sum, you may no b surprsd o larn ha n h abov cass h ourr srs sum s rplacd by h ourr ransform whch dscrbs h frquncs prsn n h orgnal funcon ourr ransforms, somms calld ourr ngrals can b usd o rprsn - non-prodc funcons, g a sngl volag puls, a flash of lgh - a connuous spcrum of frquncs, g a connuous rang of colours of lgh or muscal pch Thy ar usd xnsvly n all aras of physcs and asronomy Dfnon of ourr Transforms In our sudy of ourr srs w focussd manly on h sn and cosn forms bu wh ourr ransforms s usually mor convnn o us a complx xponnal form Th formula ar: Smlarly, f d whr f d kx f x k dk whr k Phl Lghfoo 8/9 Lcurs 9- - Pag of 8 kx f x dx Essnally h formula for k dfns h ourr ransform of fx; lar w wll prov ha subsung hs no h ohr formula rurns h orgnal funcon fx rs w wll assum h formula ar ru, larn o us hm and obsrv som mporan proprs Th funcons fx and k smlarly f and ar calld a par of ourr ransforms or ngrals Th only dffrnc n h form of h ngrals s h sgn of h xponn, and n pracc s common o call hr funcon h ourr ransform of h ohr Nos and, or x and k, ar ofn calld conjuga varabls k s h wavnumbr, k /λ compar wh /T 3 Thr ar dffrn convnons abou h facor of Th convnon w ar usng, wh / apparng symmrcally, s h mos commonly usd by physcss

PHY6 pplcaons ourr ransforms ar usd n many dvrs aras of physcs and asronomy or xampl: In h opcs cours you wll fnd ha h nnsy of h raunhofr dffracon parn from an aprur s h modulus squard of h ourr ransform of h aprur Nx yar n nuclar physcs you wll fnd ha any wak scarng s found from h ourr ransform of h scarng ponal lhough nuclar physcss call h form facor nsad of h ourr ransform In quanum mchancs a localsd parcl has a sprad of momna Ths ar gvn by h ourr ransform of h wav pack 3 Exampls Exampl : rcangular op ha funcon nd h ourr ransform of h funcon f x p < x < p p > x and x > p k f x kx dx p p kx dx k kp kp [ ] Ths funcon occurs so ofn has a nam: s calld a snc funcon p sn kp kp snc x sn x x Or somms dfnd as sn x x ndng h valu a x s a ll rcky Th ass mhod s o us h srs xpanson of sn and look a h lm as x : x 3 x{ } x x sn x sn x x x[ ] Hnc lm lm 6 x lm{ } 3! 6 x x x x x 6 W s ha h majory of h funcon ls nsd h rgon < x < Ths s vn mor ru of h funcon snc x, whch s of nrs n opcs s lar sn x Th oal ara undr h curv can b valuad: dx x Exampl : Th Gaussan nd h ourr ransform of h Gaussan funcon f x a ax / No Th Gaussan s a funcon ncounrd frqunly n Quanum Mchancs and sascs Th consan a s rlad o h wdh: fx falls o / of s nal valu a x / a x ± / a Th facor of a / nsurs ha f x dx as rqurd for a probably dsrbuon Usng h formula abov, k ax a kx dx a ax kx dx Phl Lghfoo 8/9 Lcurs 9- - Pag of 8

Ths ngral s pry rcky I can b shown ha So a ax k k a kx a a a k dx j nx jx 4n dx n Hr a n and j k PHY6 Hnc w hav found ha h ourr ransform of a Gaussan s a Gaussan! Th nvrs ransform can b prformd n a vry smlar way of cours gvng h nal Gaussan Rlvanc o Quanum mchancs k a ax L us look a h wdhs of h Gaussan / a f x and s ransform k W could ak any wdh w wand such as full wdh half maxmum, h man squard valu of x, or vn sgma so long as w wr conssn for boh Gaussans, bu o kp hngs smpl l s consdr whr ach funcon falls o / of s maxmum valu W can hrfor say h half wdh of fx s hn x / / a and for k s k / a So h full wdhs ar x / a 8 a and k a 8a W fnd h followng mporan rsul: h produc of h wdhs x k cons 8 Th produc of h wdhs s hrfor a consan, ndpndn of a, s xac valu drmnd by how h wdh s dfnd Ths s no jus ru for Gaussans I s ru for any funcon and s ourr ransform S uoral qusons! Th narrowr h funcon, h wdr h ransform, and vc vrsa Th broadr h funcon n ral spac x spac, h narrowr h ransform n k spac Or smlarly, workng wh m and frquncy, consan On can undrsand hs by hnkng abou wavpacks pur sn wav fx sn kx has unform nnsy hroughou all spac and comprss a sngl frquncy, x, k If w add oghr wo sn wavs of vry smlar k, gx sn kx sn k δkx, h sns add oghr consrucvly a h orgn bu bgn o cancl ach ohr ou nrfr dsrucvly furhr away s on adds oghr mor funcons wh a wdr rang of k s k ncrass, h wavs add consrucvly ovr an ncrasngly narrow rgon x dcrass, and nrfr dsrucvly vrywhr ls Th rsul abov s rlad o h uncrany rlaonshp n quanum mchancs Rmmbr ha momnum s rlad o k by p h k Thus p h k n dal fr parcl can b rprsnd by a wavfuncon kx ψ x, ψ, ha s has a dfn valu of k, a dfn momnum Corrspondngly hs wavfuncon xnds hrough all spac so w canno say whr h parcl s! k p, x parcl whch s localsd n spac has fn x mus b rprsnd by a wavpack wh a sprad of k, a sprad of momna W hav x k ~, hnc x p ~ ħ Ths s h uncrany rlaonshp bwn poson and momnum In h sam way, from ~, and h rlaonshp E h w hav E ~ ħ Ths s h uncrany rlaon bwn nrgy and m Phl Lghfoo 8/9 Lcurs 9- - Pag 3 of 8

PHY6 Phl Lghfoo 8/9 Lcurs 9- - Pag 4 of 8 Exampl 3: puls of radaon Consdr a puls of lgh gvn by < < ohrws f cos Th frquncy spcrum s gvn by d d d f cos d Groupng rms Bu rmmbr ha sn θ θ θ so w can wr sn sn sn sn Now l s mulply boh op and boom by sn sn Ofn >> so h scond rm s vry small and w nd only consdr h frs rm: sn Th frquncs ha ar prsn ar ssnally hos n h rang < < ± whr / So h full wdh of frquncs s / No ha f h puls s vry long h frquncy sprad s vry small ssnally h only frquncy obsrvd wll b Ths s as xpcd Bu for a shor puls hr wll b sgnfcan broadnng Ths rsul s rlvan o pulsd lasrs T-sapphr lasrs hav bn dvlopd whch gv vry shor pulss of lgh pulss lasng jus a fw fmosconds Such lgh pulss ar usd, for xampl, o prob rlaxaon phnomna n solds Howvr h frquncy of h lgh slf s only a ll grar han 5 Hz so hs mans ha w rally hav a shor cosn wav puls n m, and h frquncy s hrfor sprad Whl CW connuous wav lasrs can m lgh wh an xrmly narrow ln-wdh, pulsd lasr lgh mus, by s vry naur, hav a broadr ln-wdh nd h shorr h puls, h broadr h ln-wdh

PHY6 Exampl 4: Th on-sdd xponnal funcon Show ha h funcon f x k f x kx dx x < has ourr ransform λ x x > dx dx k λ k λ k [ ] λx kx x λ k λ k 4 Complxy, Symmry and h Cosn Transform Th formula for k nvolvs kx So n gnral, f fx s ral, k wll b complx In xampl 4, k s complx Howvr n xampls, and 3, k s ral Why? or ourr srs w found spcal rsuls for vn and odd funcons I s smlar for ourr ransforms W can wr k kx f x dx f x cos kxdx f xsn kxdx or an vn funcon, h scond ngral wll b zro h ngral of an odd funcon ovr a symmrc nrval Hnc f fx s ral and vn hn s ourr ransform s ral xampls,, and 3 Smlarly for an odd funcon h frs ngral wll b zro, so h ourr ransform s purly magnary In h gnral cas of a funcon wh no dfn symmry, h ourr ransform s complx xampl4 X X or vn funcons, also f x dx f x dx, so w can wr: k X f xcoskxdx Such ransforms k ar also vn, so h nvrs ransform can b smlarly smplfd So for an vn ral funcon w can wr f x kcoskxdx whr k f xcoskxdx k s hn calld h ourr cosn ransform of fx Th cosn ngral s somms bu no always! asr o valua Exampl 5: Rpa Exampl usng h ourr cosn ransform formula abov k f xcos kxdx p cos kx dx sn kx k p sn kp k 5 Us of ourr Transforms Gnral Commns Gvn ourr hory, w can undrsand why n opcs and many ohr branchs of physcs on sars by sayng, l us consdr a plan wav If w can solv o fnd h bhavour of a plan wav w can us ourr analyss o do anyhng by combnng plan wavs or xampl, n an lcroncs problm on mgh wan o know h rspons of a crcu o an lcrcal puls On can consdr h rspons of h crcu o a sngl frquncy and hn us ourr hory o wr h puls n rms of sngl frquncs Compuaonal Mhods vry ffcn mhod has bn dvsd for calculang h ourr ransform of a s of daa pons I s known as fas ourr Transforms or T I s usd vry wdly n many branchs of compuaonal physcs You may m hs n h fuur Phl Lghfoo 8/9 Lcurs 9- - Pag 5 of 8

PHY6 Physcs/sronomy Exampls 5 Opcs: Dffracon of Lgh rom school physcs lssons, you may b famlar wh h dffracon of lgh a small aprurs Many of you wll sudy hs n mor dal nx smsr PHY7 Consdr a small sl llumnad unformly by lgh of wavlngh λ h sl, h lgh amplud fx, and hus also h lgh nnsy fx, wll b smlar o h op ha funcon xampl abov Obsrvng h dffracon parn on a dsan scrn, h nnsy a any pon s gvn by h ourr ransform squard: k snθ whr k and θ s λ h angular poson on a dsan scrn rom xampl, h nnsy a h scrn hrfor has a snc dsrbuon w obsrv a brgh cnral frng and rgularly spacd sd frngs of dcrasng nnsy Smlarly n all cass of scarng, h nnsy of h scard lgh s gvn by h squar of h T of 7 h objc ha dos h scarng Snc lgh has a small wavlngh, λ ~3 m w only g a 6 rasonabl rang of θ valus for a small objc g d m In vryday lf, you may b abl o s a dffracon parn by lookng a a sodum srlgh hrough an umbrlla or hrough a ms of randrops ourr ransforms go boh ways, so also from lookng a a dffracon parn w can dduc h naur of h objc causng h scarng or xampl, crysal lacs can scar X-rays and from h dffracon parns h crysal srucur can b dducd 5 Nuclar Physcs: scarng of lcrons Consdr a bam of lcrons scard by proons ull analyss rqurs rlavsc quanum mchancs Bu w xpc h sam faurs as n ohr scarng: h scarng wll b largs for kd < and vry small for kd >> Th dpndnc of h scarng on k s known as h form facor Som dcads ago, proons wr hough o b lmnary parcls, so w would xpc o fnd d o b of h ordr of h sz of small nucl Howvr h daa dos no f h prdcons!! Rmmbr ha a broadr k ndcas a narrowr fx Ths daa was h frs vdnc for quarks and gluons! 53 Tlcommuncaons: bandwdh lmaons s w hav sn n xampl 3, h shorr h puls, h broadr s h frquncy dsrbuon n h ourr srs rqurd o dscrb Th lcommuncaons ndusry consanly ry o mprov daa ransfr ra along cabls Typcally h daa aks h form of a dgal sgnal and mprovd spd s achvd by shornng h lnghs of h s and s Ths xnds h frquncy dsrbuon of h ourr srs ha dscrbs If h bandwdh lm of a lphon cabl s MHz hn only frquncs blow MHz can pass, ffcvly clppng h hgh frquncy nd of h daa sgnal and dformng h shap of h logc puls squar wav a ll som pon hs wll lm daa ransfr Phl Lghfoo 8/9 Lcurs 9- - Pag 6 of 8

6 Dla uncons PHY6 Th Drac dla funcon δx s vry usful n many aras of physcs I s no an ordnary funcon, n fac proprly spakng can only lv nsd an ngral Hr w dfn, xplor s proprs, hn us o prov h ourr ngral horm Essnally h dla funcon s an nfnly narrow spk ha has un ara δx s a spk cnrd a x, δx x s a spk cnrd a x x Th produc of h dla funcon δx x wh any funcon fx s zro xcp whr x ~ x ormally, for any funcon fx f x δ x x dx f and δ x x dx x b f In fac hs ngrals can also b wrn x δ x x dx f x and a b δ x x dx a whr a < x < b, snc δx x s also dfnd o b zro vrywhr xcp a x x Thr ar svral ways n whch w pcur δx x Th smpls s as h lm as h of a rcangl of hgh h, wdh /h, and hus ara h/h h /h Exampls x x Gvn ha f x δ x x dx f, a fnd x sn x δ x x dx, b fnd x δ x a dx, c fnd h T of fx δx a a b c Phl Lghfoo 8/9 Lcurs 9- - Pag 7 of 8

7 Proof of h ourr Transform Thorm PHY6 Th formula for ourr ransforms can b drvd from h formula for ourr srs by consdrng a prodc funcon hn lng h prod nd o nfny You can fnd hs yp of drvaon n Kryszg scon 7, Jordan & Smh scon 7 no ha h auhors work n rms of f no and show h proof for sn srs / ngrals and Boas scon 54 uss h complx form bu no hr dffrn convnon rgardng facors of L Consdr h ngral I x kx dk L L kx kx L Lx Lx sn Lx L sn Lx W hav I x dk [ ] L cf xampl L x x x Lx Ths snc funcon nds o L/ as x and away from hr bcoms small sn x sn Lx W sad arlr ha dx Smlarly x dx x So w s ha akng h lm as L of Ix w hav h proprs w wan n a dla funcon L kx So w can dfn a dla funcon as δ x Lm L dk L Hnc kx δ x dk or k xx δ x x dk W wll us hs dfnon o prov h ourr ngral horm Earlr w sad kx f x k dk whr k kx f x dx Gvn a funcon fx, h scond formula dfns k Wha nds o b provd s ha subsung hs k no h frs formula dos yld h orgnal funcon fx Pu h scond ngral no h frs: kx kx kx f x k dk f x dx dk kx kx k x x f x dx dk f x dx dk f x δ x x dx f x Hnc, usng our dfnon of a dla funcon, w hav provd h horm Phl Lghfoo 8/9 Lcurs 9- - Pag 8 of 8