Time-domain Aeroelastic Analysis of Bridge using a Truncated Fourier Series of the Aerodynamic Transfer Function

Size: px
Start display at page:

Download "Time-domain Aeroelastic Analysis of Bridge using a Truncated Fourier Series of the Aerodynamic Transfer Function"

Transcription

1 Te 8 Ci-Jp-ore eriol Worksop o Wid Egieerig My, 3 Time-domi Aeroelsic Alysis of ridge usig Truced Fourier Series of e Aerodymic Trsfer Fucio Jiwook Prk, Seoul iol iversiy, ore ilje Jug, iversiy of ore Dme, SA Ho-yug im, Seoul iol iversiy, ore He Sug Lee, Seoul iol iversiy, ore

2 Coes. roducio. Cusliy Requireme 3. Truced Fourier Series Approximio 4. Applicio d Verificio - H-ype secio 5. Summry Seoul iol iversiy

3 . roducio Aerodymic Forces iduced by Moio of ridge - Self-exied forces L e Aerodymic Sysem M e Srip Teory Goverig Equio : vier-sokes Eq. egrio of e Pressure Disribuio o lyicl soluios of e erodymic forces sully ssumed s lier sysem i frequecy domi Deermied roug Wid uel es or CFD simulio For e ime-domi lysis, e erodymic sysem sould sisfy e Cusliy Requireme. Seoul iol iversiy 3

4 4 Seoul iol iversiy Lierized Aerodymic Sysem i Frequecy Domi - Adopig e Fluer Derivives proposed by Scl Mixed frequecy/ime domi Smll-mpliude siusoidl moio wi sigle frequecy were, : Reduced frequecy siclly bsed o e Aerodymic Trsfer Fucios were, F : Fourier rsform A A H H A A H H M L e e F F F F A ia A ia H ih H ih M F L F e e. Cusliy Requireme

5 Mesured Trsfer Fucio ormlized mgiude. Cusliy Requireme Lierized Aerodymic Sysem i Time-domi - sig Covoluio egrl Teorem y kig e iverse Fourier rsform L M e e d d d d -5 Aerodymic mpulse Respose Fucios - mgiry pr Rel pr -5 =/ 3 4 Seoul iol iversiy i e d for k, l, verse FT 4 Evlued RF = : Cusliy codiio / 5

6 ormlized mgiude. Cusliy Requireme Cusliy Codiio - Defiiio for 4 Evlued RF Modified RF - Memicl meig Oe-sided covoluio egrl L M e e d d / d d Reliosip bewee e rel d imgiry pr of TF R cos si d for - Pysicl meig o erodymic force is geered before e deck moves Seoul iol iversiy 6

7 Rel pr of compoe. Cusliy Requireme Previous works - RFA Riol Fucio Approximio : RFA is bsed o e soluio o e idelly i secio. : RFA s limiio o is pplicbiliy o bluff secios. - Pely Fucio Approc, Jug e l. : is pplicble o e bluff secios : Cusliy codiio is wey imposed s pely fucio roug e opimizio. -Limiio of RFA, Jug e l. Mesured rsfer fucio RFA r= RFA r= RFA r=3 4 - Aerodymic rsfer fucio for H-ype secio - RFA is drw gis e rig vericl xis RFA yields urelible resuls / Propose e efficie meod excly sisfy e cusliy codiio!! * Jug,., im, H.., d Lee, H. S.. Evluio of impulse respose fucios for covoluio iegrls of erodymic forces by opimizio wi pely fucio. J. Eg. Mec., 385, Seoul iol iversiy 7

8 . Cusliy Requireme Compriso bewee Previous Work d Proposed Meod RFA Proposed Approximio meod Ryleig-Riz ype pproximio Fiie eleme meod Ryleig-Riz ype pproximio sis fucio Riol fucio Cubic splie Sie, Cosie fucio Cusliy codiio Srogly eforceme Wey eforceme Srogly eforceme Applicbiliy Limiio of pplicio o e bluff secio Applicble o e bluff secio Applicble o e bluff secio Seoul iol iversiy 8

9 3. Truced Fourier Series Approximio Approximio usig Truced Fourier Series - Fourier series represeios of e rsfer fucios R b cos mx bsi mx, b mx : modified rsfer fucio : coefficies of e Fourier series : e umber of erms i e Fourier series : mximum reduced frequecy - eed of e lier erm b i e imgiry pr Wiou e lier erm, e discoiuiy rises mx. Te discoiuiy cuses Gibbs peomeo. A lrge umber of erms sould be icluded. mx Seoul iol iversiy 9

10 3. Truced Fourier Series Approximio Eforceme of e Cusliy Codiio - RF correspodig o e modified rsfer fucio : RF becomes series of Dirc-del fucios. R [ cos R cos b si d si mx b ] d mx b - Cusliy codiio for e modified rsfer fucio for b for,, Seoul iol iversiy

11 Seoul iol iversiy Fil Aerodymic Forces mx mx mx mx e e b b M b b L e e d d M d d L To perform e covoluio iegrls, oly ps displcemes re required. 3. Truced Fourier Series Approximio

12 3. Truced Fourier Series Approximio Deermiio of Coefficies of e Fourier Series - Te ukow coefficies re deermied by miimizig e errors bewee e mesured d modified rsfer fucios. Mi w : weigig fcor, R, R L mx mx w R R w d L : L -orm, : mesured rsfer fucios ierpoled by cubic splie L d b T : + ukows : + equios Seoul iol iversiy

13 4. Applicio d Verificio - H-ype secio Codiio of e Problem - Jug el l. demosred e limiio of RFA for is H-ype secio - Goverig equio m c k L m c k e M L e ex M ex m c k f 3.64 kg/m,.3 kg/s/m, 33.6 /m/m, k 3.5 Hz, m c f. kgm /m. kgm /s/m 6. m/m 5.5 Hz - Dimesio of e H-ype bluff secio, im d ig 7 6m/ s 3.5 kg/m - Exerl forces : To compre e sedy-se resposes wi ose obied by mesured rsfer fucio. L M ex ex /m si m/m ex, ex 8 rd/s Seoul iol iversiy 3

14 mgiy pr of compoe Rel pr of compoe 4. Applicio d Verificio - H-ype secio Compoes of e Trsfer Fucios for e Lif Force - Mesured rsfer fucio Proposed meod = Proposed meod =5 Proposed meod = =/ R Mesured rsfer fucio - Proposed meod = Proposed meod =5 Proposed meod = =/ - Te d Proposed meod yields lmos e sme resuls. - Eve, e Proposed meod yields closer soluio o e Mesured e. - For e proposed meod, oly 5 erms of Fourier series re eoug coverge. Seoul iol iversiy 4

15 mgiry pr of compoe Rel pr of compoe 4. Applicio d Verificio - H-ype secio Compoes of e Trsfer Fucios for e Lif Force Mesured rsfer fucio Proposed meod = Proposed meod =5 Proposed meod = R Mesured rsfer fucio Proposed meod = Proposed meod =5 Proposed meod = =/ =/ - Te d Proposed meod yields lmos e sme resuls. - Te differeces wi Mesured idices e degrees of violio of e cusliy codiio i e Mesured. Seoul iol iversiy 5

16 mgiry pr of compoe Rel pr of compoe 4. Applicio d Verificio - H-ype secio Compoes of e Trsfer Fucios for e Mome 4 4 R Mesured rsfer fucio - Proposed meod = Proposed meod =5 Proposed meod = =/ Mesured rsfer fucio - Proposed meod = Proposed meod =5-4 Proposed meod = =/ -Te resuls for e mome c be similrly ierpreed wi ose for e lif force Seoul iol iversiy 6

17 mgiry pr of compoe Rel pr of compoe 4. Applicio d Verificio - H-ype secio Compoes of e Trsfer Fucios for e Mome 4 Mesured rsfer fucio Proposed meod = Proposed meod =5 Proposed meod = 4 R =/ Mesured rsfer fucio - Proposed meod = Proposed meod =5 Proposed meod = =/ -Te resuls for e mome c be similrly ierpreed wi ose for e lif force Seoul iol iversiy 7

18 Priculr sol. Vericl displceme cm Priculr sol. Roiol gle - rd Vericl displceme cm Priculr sol. Roiol gle - rd 4. Applicio d Verificio - H-ype secio Resposes - sig ewmrk-be meod wi ime iervl of.96 sec - Te, proposed meod d priculr soluio ve o oiceble differece. 5 Proposed meod = 5 Proposed meod = -5 Time s 5 Priculr sol. Proposed meod = -5 5 Time s Priculr sol. Proposed meod = Time s Time s Seoul iol iversiy 8

19 4. Applicio d Verificio - H-ype secio Compriso of Compuio Time - Compuer:.4GHz sigle core - Progrm: MATLA Rb - Alysis ime: sec - Time iervl:.958 sec Proposed meod = Compuio ime 4.7 sec.6 sec Reducio of 94 % Proposed meod c be used o perform ime-domi eroelsic lysis eve for lrge-scle srucure efficiely wiou y loss of ccurcy. Seoul iol iversiy 9

20 5. Summry Cusliy Requireme Propose e Exc d Efficie Meod usig Truced Fourier Series - Cusliy codiio is srogly imposed. - RF becomes Dirc-del fucios Reducio of e compuio Applicio d Verificio roug e exmple of H-ype bluff secio Seoul iol iversiy

21 ACOWLEDGEMET Tis reserc ws suppored by e gr 9CCT- A from e Miisry of Ld, Trspor d Mriime Affirs of ore goverme roug e Core Reserc siue Seoul iol iversiy for Core Egieerig Tecology Developme of Super Log Sp ridge R&D Ceer. Tk you!

Time-domain Aeroelastic Analysis of Bridge using a Truncated Fourier Series of the Aerodynamic Transfer Function

Time-domain Aeroelastic Analysis of Bridge using a Truncated Fourier Series of the Aerodynamic Transfer Function Time-domai Aeroelasic Aalysis of ridge usig a Trucaed Fourier Series of he Aerodyamic Trasfer Fucio Jiwook PA Graduae Sude Seoul aioal iversiy Seoul, orea jwpark7@su.ac.kr H Sug LEE Professor Seoul aioal

More information

ERROR ESTIMATES FOR APPROXIMATING THE FOURIER TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION

ERROR ESTIMATES FOR APPROXIMATING THE FOURIER TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION ERROR ESTIMATES FOR APPROXIMATING THE FOURIER TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION N.S. BARNETT, S.S. DRAGOMIR, AND G. HANNA Absrc. I his pper we poi ou pproximio for he Fourier rsform for fucios

More information

Approach Method to Evaluate the Total Harmonic Distortion for a System Has Multiple Nonlinear Loads

Approach Method to Evaluate the Total Harmonic Distortion for a System Has Multiple Nonlinear Loads eriol Jourl of Egieerig Reserc SSN:39-689(olie,347-53(pri Volume No.4, ssue No., pp : 68-64 Nov. 5 Approc eod o Evlue e ol rmoic Disorio for Sysem s uliple Nolier Lods. A. omed Elecricl Power d cies Deprme,

More information

Experiment 6: Fourier Series

Experiment 6: Fourier Series Fourier Series Experime 6: Fourier Series Theory A Fourier series is ifiie sum of hrmoic fucios (sies d cosies) wih every erm i he series hvig frequecy which is iegrl muliple of some pricipl frequecy d

More information

Free Flapping Vibration of Rotating Inclined Euler Beams

Free Flapping Vibration of Rotating Inclined Euler Beams World cdemy of Sciece, Egieerig d Techology 56 009 Free Flppig Vibrio of Roig Iclied Euler Bems Chih-ig Hug, We-Yi i, d Kuo-Mo Hsio bsrc mehod bsed o he power series soluio is proposed o solve he url frequecy

More information

Special Functions. Leon M. Hall. Professor of Mathematics University of Missouri-Rolla. Copyright c 1995 by Leon M. Hall. All rights reserved.

Special Functions. Leon M. Hall. Professor of Mathematics University of Missouri-Rolla. Copyright c 1995 by Leon M. Hall. All rights reserved. Specil Fucios Leo M. Hll Professor of Mhemics Uiversiy of Missouri-Roll Copyrigh c 995 y Leo M. Hll. All righs reserved. Chper 5. Orhogol Fucios 5.. Geerig Fucios Cosider fucio f of wo vriles, ( x,), d

More information

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions

Existence Of Solutions For Nonlinear Fractional Differential Equation With Integral Boundary Conditions Reserch Ivey: Ieriol Jourl Of Egieerig Ad Sciece Vol., Issue (April 3), Pp 8- Iss(e): 78-47, Iss(p):39-6483, Www.Reserchivey.Com Exisece Of Soluios For Nolier Frciol Differeil Equio Wih Iegrl Boudry Codiios,

More information

Reinforcement Learning

Reinforcement Learning Reiforceme Corol lerig Corol polices h choose opiml cios Q lerig Covergece Chper 13 Reiforceme 1 Corol Cosider lerig o choose cios, e.g., Robo lerig o dock o bery chrger o choose cios o opimize fcory oupu

More information

F.Y. Diploma : Sem. II [CE/CR/CS] Applied Mathematics

F.Y. Diploma : Sem. II [CE/CR/CS] Applied Mathematics F.Y. Diplom : Sem. II [CE/CR/CS] Applied Mhemics Prelim Quesio Pper Soluio Q. Aemp y FIVE of he followig : [0] Q. () Defie Eve d odd fucios. [] As.: A fucio f() is sid o e eve fucio if f() f() A fucio

More information

ONE RANDOM VARIABLE F ( ) [ ] x P X x x x 3

ONE RANDOM VARIABLE F ( ) [ ] x P X x x x 3 The Cumulive Disribuio Fucio (cd) ONE RANDOM VARIABLE cd is deied s he probbiliy o he eve { x}: F ( ) [ ] x P x x - Applies o discree s well s coiuous RV. Exmple: hree osses o coi x 8 3 x 8 8 F 3 3 7 x

More information

NOTES ON BERNOULLI NUMBERS AND EULER S SUMMATION FORMULA. B r = [m = 0] r

NOTES ON BERNOULLI NUMBERS AND EULER S SUMMATION FORMULA. B r = [m = 0] r NOTES ON BERNOULLI NUMBERS AND EULER S SUMMATION FORMULA MARK WILDON. Beroulli umbers.. Defiiio. We defie he Beroulli umbers B m for m by m ( m + ( B r [m ] r r Beroulli umbers re med fer Joh Beroulli

More information

ECE 636: Systems identification

ECE 636: Systems identification ECE 636: Sysems ideificio Lecures 7 8 Predicio error mehods Se spce models Coiuous ime lier se spce spce model: x ( = Ax( + Bu( + w( y( = Cx( + υ( A:, B: m, C: Discree ime lier se spce model: x( + = A(

More information

Fourier transform. Continuous-time Fourier transform (CTFT) ω ω

Fourier transform. Continuous-time Fourier transform (CTFT) ω ω Fourier rasform Coiuous-ime Fourier rasform (CTFT P. Deoe ( he Fourier rasform of he sigal x(. Deermie he followig values, wihou compuig (. a (0 b ( d c ( si d ( d d e iverse Fourier rasform for Re { (

More information

LOCUS 1. Definite Integration CONCEPT NOTES. 01. Basic Properties. 02. More Properties. 03. Integration as Limit of a Sum

LOCUS 1. Definite Integration CONCEPT NOTES. 01. Basic Properties. 02. More Properties. 03. Integration as Limit of a Sum LOCUS Defiie egrio CONCEPT NOTES. Bsic Properies. More Properies. egrio s Limi of Sum LOCUS Defiie egrio As eplied i he chper iled egrio Bsics, he fudmel heorem of clculus ells us h o evlue he re uder

More information

Forced Oscillation of Nonlinear Impulsive Hyperbolic Partial Differential Equation with Several Delays

Forced Oscillation of Nonlinear Impulsive Hyperbolic Partial Differential Equation with Several Delays Jourl of Applied Mhemics d Physics, 5, 3, 49-55 Published Olie November 5 i SciRes hp://wwwscirporg/ourl/mp hp://dxdoiorg/436/mp5375 Forced Oscillio of Nolier Impulsive Hyperbolic Pril Differeil Equio

More information

Distortion Analysis of a LNA

Distortion Analysis of a LNA Disorio lysis of LN Su Tr Lim 0. bsrc This pper preses overview d compriso of he commo soluio i deermiig disorio i LN. Brief bckgroud iformio regrdig how disorio ffecs he performce of CMOS LN is preseed.

More information

Frequency-domain Characteristics of Discrete-time LTI Systems

Frequency-domain Characteristics of Discrete-time LTI Systems requecy-domi Chrcteristics of Discrete-time LTI Systems Prof. Siripog Potisuk LTI System descriptio Previous bsis fuctio: uit smple or DT impulse The iput sequece is represeted s lier combitio of shifted

More information

Section 8 Convolution and Deconvolution

Section 8 Convolution and Deconvolution APPLICATIONS IN SIGNAL PROCESSING Secio 8 Covoluio ad Decovoluio This docume illusraes several echiques for carryig ou covoluio ad decovoluio i Mahcad. There are several operaors available for hese fucios:

More information

ON SOME FRACTIONAL PARABOLIC EQUATIONS DRIVEN BY FRACTIONAL GAUSSIAN NOISE

ON SOME FRACTIONAL PARABOLIC EQUATIONS DRIVEN BY FRACTIONAL GAUSSIAN NOISE IJRRAS 6 3) Februry www.rppress.com/volumes/vol6issue3/ijrras_6_3_.pdf ON SOME FRACIONAL ARABOLIC EQUAIONS RIVEN BY FRACIONAL GAUSSIAN NOISE Mhmoud M. El-Bori & hiri El-Sid El-Ndi Fculy of Sciece Alexdri

More information

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead)

Week 8 Lecture 3: Problems 49, 50 Fourier analysis Courseware pp (don t look at French very confusing look in the Courseware instead) Week 8 Lecure 3: Problems 49, 5 Fourier lysis Coursewre pp 6-7 (do look Frech very cofusig look i he Coursewre ised) Fourier lysis ivolves ddig wves d heir hrmoics, so i would hve urlly followed fer he

More information

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.

David Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition. ! Revised April 21, 2010 1:27 P! 1 Fourier Series David Radall Assume ha u( x,) is real ad iegrable If he domai is periodic, wih period L, we ca express u( x,) exacly by a Fourier series expasio: ( ) =

More information

6.003: Signals and Systems Lecture 20 April 22, 2010

6.003: Signals and Systems Lecture 20 April 22, 2010 6.003: Sigals ad Sysems Lecure 0 April, 00 6.003: Sigals ad Sysems Relaios amog Fourier Represeaios Mid-erm Examiaio #3 Wedesday, April 8, 7:30-9:30pm. No reciaios o he day of he exam. Coverage: Lecures

More information

Analytical approach to transient heat conduction in cooling load calculations Duska, M; Bartak, M.; Drkal, F.; Hensen, J.L.M.

Analytical approach to transient heat conduction in cooling load calculations Duska, M; Bartak, M.; Drkal, F.; Hensen, J.L.M. lyicl pproch o rsie he coducio i coolig lod clculios Dusk, M; rk, M.; Drkl, F.; Hese,.L.M. Published i: Proceedigs of he 17h I. ir-codiioig d Veilio Coferece, Prgue Published: 1/1/6 Docume Versio cceped

More information

International Journal of Computer Sciences and Engineering. Research Paper Volume-6, Issue-1 E-ISSN:

International Journal of Computer Sciences and Engineering. Research Paper Volume-6, Issue-1 E-ISSN: Ieriol Jourl of Compuer Scieces d Egieerig Ope ccess Reserch Pper Volume-6, Issue- E-ISSN: 47-69 pplicios of he boodh Trsform d he Homoopy Perurbio Mehod o he Nolier Oscillors P.K. Ber *, S.K. Ds, P. Ber

More information

An Improved Bat Algorithm for Software Cost Estimation

An Improved Bat Algorithm for Software Cost Estimation DEEAK NANDAL e l: AN IMROVED ALGORITHM FOR SOFTWARE COST ESTIMATION A Improved B Algorihm for Sofwre Cos Esimio Deepk Ndl 1, Om rksh Sgw 2 1 dr.deepkdlgju@gmil.com, 2 sgw0863@gmil.com Deprme of Compuer

More information

SHOCK AND VIBRATION RESPONSE SPECTRA COURSE Unit 21 Base Excitation Shock: Classical Pulse

SHOCK AND VIBRATION RESPONSE SPECTRA COURSE Unit 21 Base Excitation Shock: Classical Pulse SHOCK AND VIBRAION RESPONSE SPECRA COURSE Ui 1 Base Exciaio Shock: Classical Pulse By om Irvie Email: omirvie@aol.com Iroucio Cosier a srucure subjece o a base exciaio shock pulse. Base exciaio is also

More information

Sampling Example. ( ) δ ( f 1) (1/2)cos(12πt), T 0 = 1

Sampling Example. ( ) δ ( f 1) (1/2)cos(12πt), T 0 = 1 Samplig Example Le x = cos( 4π)cos( π). The fudameal frequecy of cos 4π fudameal frequecy of cos π is Hz. The ( f ) = ( / ) δ ( f 7) + δ ( f + 7) / δ ( f ) + δ ( f + ). ( f ) = ( / 4) δ ( f 8) + δ ( f

More information

Systematic and Optimal Design of CMOS Two-Stage Opamps with Hybrid Cascode Compensation

Systematic and Optimal Design of CMOS Two-Stage Opamps with Hybrid Cascode Compensation Sysemic d Opiml Desig of MOS Two-Sge Opmps wih Hybrid scode ompesio Mohmmd Yvri, Omid Shoei, d Agel Rodriguez-Vzquez* I Desig borory, EE Deprme, Uiversiy of Tehr, Tehr 14395-515, Ir * Isiue of Microelecroics

More information

Transient Solution of the M/M/C 1 Queue with Additional C 2 Servers for Longer Queues and Balking

Transient Solution of the M/M/C 1 Queue with Additional C 2 Servers for Longer Queues and Balking Jourl of Mhemics d Sisics 4 (): 2-25, 28 ISSN 549-3644 28 Sciece ublicios Trsie Soluio of he M/M/C Queue wih Addiiol C 2 Servers for Loger Queues d Blkig R. O. Al-Seedy, A. A. El-Sherbiy,,2 S. A. EL-Shehwy

More information

Local Fractional Kernel Transform in Fractal Space and Its Applications

Local Fractional Kernel Transform in Fractal Space and Its Applications From he SelecedWorks of Xio-J Yg 22 Locl Frciol Kerel Trsform i Frcl Spce d Is Applicios Yg Xioj Aville : hps://works.epress.com/yg_ioj/3/ Advces i Compuiol Mhemics d is Applicios 86 Vol. No. 2 22 Copyrigh

More information

VARIATIONAL ITERATION METHOD (VIM) FOR SOLVING PARTIAL INTEGRO-DIFFERENTIAL EQUATIONS

VARIATIONAL ITERATION METHOD (VIM) FOR SOLVING PARTIAL INTEGRO-DIFFERENTIAL EQUATIONS Jourl of Theoreicl d Applied Iformio Techology h Jue 16. Vol.88. No. 5-16 JATIT & LLS. All righs reserved. ISSN: 199-8645 www.ji.org E-ISSN: 1817-195 VARIATIONAL ITERATION ETHOD VI FOR SOLVING PARTIAL

More information

A L A BA M A L A W R E V IE W

A L A BA M A L A W R E V IE W A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N

More information

EEE 303: Signals and Linear Systems

EEE 303: Signals and Linear Systems 33: Sigls d Lir Sysms Orhogoliy bw wo sigls L us pproim fucio f () by fucio () ovr irvl : f ( ) = c( ); h rror i pproimio is, () = f() c () h rgy of rror sigl ovr h irvl [, ] is, { }{ } = f () c () d =

More information

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018

DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS. Assoc. Prof. Dr. Burak Kelleci. Spring 2018 DEPARTMENT OF ELECTRICAL &ELECTRONICS ENGINEERING SIGNALS AND SYSTEMS Assoc. Prof. Dr. Bur Kelleci Sprig 8 OUTLINE The Z-Trsform The Regio of covergece for the Z-trsform The Iverse Z-Trsform Geometric

More information

Comparison between Fourier and Corrected Fourier Series Methods

Comparison between Fourier and Corrected Fourier Series Methods Malaysia Joural of Mahemaical Scieces 7(): 73-8 (13) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Joural homepage: hp://eispem.upm.edu.my/oural Compariso bewee Fourier ad Correced Fourier Series Mehods 1

More information

1. Six acceleration vectors are shown for the car whose velocity vector is directed forward. For each acceleration vector describe in words the

1. Six acceleration vectors are shown for the car whose velocity vector is directed forward. For each acceleration vector describe in words the Si ccelerio ecors re show for he cr whose eloci ecor is direced forwrd For ech ccelerio ecor describe i words he iseous moio of he cr A ri eers cured horizol secio of rck speed of 00 km/h d slows dow wih

More information

Evaluation and Design of Filters Using a Taylor Series Expansion

Evaluation and Design of Filters Using a Taylor Series Expansion 84 IEEE RASACIOS O VISUALIZAIO AD COMPUER GRAPHICS, VOL. 3, O., APRIL-JUE 997 Evluio d Desig of Filers Usig ylor Series Expsio orse Möller, Rghu Mchirju, Klus Mueller, d Roi Ygel Absrc We describe e mehod

More information

An Extension of Hermite Polynomials

An Extension of Hermite Polynomials I J Coemp Mh Scieces, Vol 9, 014, o 10, 455-459 HIKARI Ld, wwwm-hikricom hp://dxdoiorg/101988/ijcms0144663 A Exesio of Hermie Polyomils Ghulm Frid Globl Isiue Lhore New Grde Tow, Lhore, Pkis G M Hbibullh

More information

Chapter 5: The pn Junction

Chapter 5: The pn Junction Cher 5: The ucio Noequilibrium ecess crriers i semicoducors Crrier geerio d recombiio Mhemicl lysis of ecess crriers Ambiolr rsor The jucio Bsic srucure of he jucio Zero lied bis Reverse lied bis No-uiformly

More information

ELEG 5173L Digital Signal Processing Ch. 2 The Z-Transform

ELEG 5173L Digital Signal Processing Ch. 2 The Z-Transform Deprtmet of Electricl Egieerig Uiversity of Arkss ELEG 573L Digitl Sigl Processig Ch. The Z-Trsform Dr. Jigxi Wu wuj@urk.edu OUTLINE The Z-Trsform Properties Iverse Z-Trsform Z-Trsform of LTI system Z-TRANSFORM

More information

Boundary Value Problems of Conformable. Fractional Differential Equation with Impulses

Boundary Value Problems of Conformable. Fractional Differential Equation with Impulses Applied Meicl Scieces Vol 2 28 o 8 377-397 HIKARI Ld www-irico ps://doiorg/2988/s28823 Boudry Vlue Probles of Coforble Frciol Differeil Equio wi Ipulses Arisr Tgvree Ci Tipryoo d Apisi Ppogpu Depre of

More information

Supplement: Gauss-Jordan Reduction

Supplement: Gauss-Jordan Reduction Suppleme: Guss-Jord Reducio. Coefficie mri d ugmeed mri: The coefficie mri derived from sysem of lier equios m m m m is m m m A O d he ugmeed mri derived from he ove sysem of lier equios is [ ] m m m m

More information

The Trigonometric Representation of Complex Type Number System

The Trigonometric Representation of Complex Type Number System Ieriol Jourl of Scieific d Reserch Pulicios Volume 7 Issue Ocoer 7 587 ISSN 5-353 The Trigoomeric Represeio of Complex Type Numer Sysem ThymhyPio Jude Nvih Deprme of Mhemics Eser Uiversiy Sri Lk Asrc-

More information

Supplementary Information for Thermal Noises in an Aqueous Quadrupole Micro- and Nano-Trap

Supplementary Information for Thermal Noises in an Aqueous Quadrupole Micro- and Nano-Trap Supplemeary Iformaio for Thermal Noises i a Aqueous Quadrupole Micro- ad Nao-Trap Jae Hyu Park ad Predrag S. Krsić * Physics Divisio, Oak Ridge Naioal Laboraory, Oak Ridge, TN 3783 E-mail: krsicp@orl.gov

More information

Electromechanical System Dynamics, energy Conversion, and Electromechanical Analogies. Modeling of Dynamic Systems

Electromechanical System Dynamics, energy Conversion, and Electromechanical Analogies. Modeling of Dynamic Systems Elecroecicl Syse Dyics, eergy Coersio, d Elecroecicl Alogies Modelig of Dyic Syses Modelig of dyic syses y e doe i seerl wys: Use e sdrd equio of oio Newo s Lw for ecicl syses Use circuis eores O s lw

More information

Chapter 6 - Work and Energy

Chapter 6 - Work and Energy Caper 6 - Work ad Eergy Rosedo Pysics 1-B Eploraory Aciviy Usig your book or e iere aswer e ollowig quesios: How is work doe? Deie work, joule, eergy, poeial ad kieic eergy. How does e work doe o a objec

More information

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE

FIXED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE Mohia & Samaa, Vol. 1, No. II, December, 016, pp 34-49. ORIGINAL RESEARCH ARTICLE OPEN ACCESS FIED FUZZY POINT THEOREMS IN FUZZY METRIC SPACE 1 Mohia S. *, Samaa T. K. 1 Deparme of Mahemaics, Sudhir Memorial

More information

Solutions Manual 4.1. nonlinear. 4.2 The Fourier Series is: and the fundamental frequency is ω 2π

Solutions Manual 4.1. nonlinear. 4.2 The Fourier Series is: and the fundamental frequency is ω 2π Soluios Maual. (a) (b) (c) (d) (e) (f) (g) liear oliear liear liear oliear oliear liear. The Fourier Series is: F () 5si( ) ad he fudameal frequecy is ω f ----- H z.3 Sice V rms V ad f 6Hz, he Fourier

More information

K3 p K2 p Kp 0 p 2 p 3 p

K3 p K2 p Kp 0 p 2 p 3 p Mah 80-00 Mo Ar 0 Chaer 9 Fourier Series ad alicaios o differeial equaios (ad arial differeial equaios) 9.-9. Fourier series defiiio ad covergece. The idea of Fourier series is relaed o he liear algebra

More information

Lecture 15 First Properties of the Brownian Motion

Lecture 15 First Properties of the Brownian Motion Lecure 15: Firs Properies 1 of 8 Course: Theory of Probabiliy II Term: Sprig 2015 Isrucor: Gorda Zikovic Lecure 15 Firs Properies of he Browia Moio This lecure deals wih some of he more immediae properies

More information

Inverse Transient Quasi-Static Thermal Stresses. in a Thin Rectangular Plate

Inverse Transient Quasi-Static Thermal Stresses. in a Thin Rectangular Plate Adv Theor Al Mech Vol 3 o 5-3 Iverse Trsie Qusi-Sic Therml Sresses i Thi Recgulr Ple Prvi M Slve Bhlero Sciece College Soer Ngur Idi rvimslve@hoocom Suchir A Meshrm Derme of Mhemics PGTD RTM Ngur Uiversi

More information

Department of Mathematical and Statistical Sciences University of Alberta

Department of Mathematical and Statistical Sciences University of Alberta MATH 4 (R) Wier 008 Iermediae Calculus I Soluios o Problem Se # Due: Friday Jauary 8, 008 Deparme of Mahemaical ad Saisical Scieces Uiversiy of Albera Quesio. [Sec.., #] Fid a formula for he geeral erm

More information

Problems and Solutions for Section 3.2 (3.15 through 3.25)

Problems and Solutions for Section 3.2 (3.15 through 3.25) 3-7 Problems ad Soluios for Secio 3 35 hrough 35 35 Calculae he respose of a overdamped sigle-degree-of-freedom sysem o a arbirary o-periodic exciaio Soluio: From Equaio 3: x = # F! h "! d! For a overdamped

More information

Fractional-Order Control and Simulation of Wind Turbines with Full-Power Converters

Fractional-Order Control and Simulation of Wind Turbines with Full-Power Converters Frciol-Order Corol d Simulio of Wid Turbies wih Full-Power Coverers R. Melício d J. P. S. Clão Dep. of Elecromechicl Egieerig Uiversiy of Beir Ierior Covilh, Porugl ruimelicio@gmil.com; clo@ubi.p V. M.

More information

HOMEWORK 6 - INTEGRATION. READING: Read the following parts from the Calculus Biographies that I have given (online supplement of our textbook):

HOMEWORK 6 - INTEGRATION. READING: Read the following parts from the Calculus Biographies that I have given (online supplement of our textbook): MAT 3 CALCULUS I 5.. Dokuz Eylül Uiversiy Fculy of Sciece Deprme of Mhemics Isrucors: Egi Mermu d Cell Cem Srıoğlu HOMEWORK 6 - INTEGRATION web: hp://kisi.deu.edu.r/egi.mermu/ Tebook: Uiversiy Clculus,

More information

sin m a d F m d F m h F dy a dy a D h m h m, D a D a c1cosh c3cos 0

sin m a d F m d F m h F dy a dy a D h m h m, D a D a c1cosh c3cos 0 Q1. The free vibrtio of the plte is give by By ssumig h w w D t, si cos w W x y t B t Substitutig the deflectio ito the goverig equtio yields For the plte give, the mode shpe W hs the form h D W W W si

More information

DIFFERENCE EQUATIONS

DIFFERENCE EQUATIONS DIFFERECE EQUATIOS Lier Cos-Coeffiie Differee Eqios Differee Eqios I disree-ime ssems, esseil feres of ip d op sigls pper ol speifi iss of ime, d he m o e defied ewee disree ime seps or he m e os. These

More information

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP)

10.3 Autocorrelation Function of Ergodic RP 10.4 Power Spectral Density of Ergodic RP 10.5 Normal RP (Gaussian RP) ENGG450 Probabiliy ad Saisics for Egieers Iroducio 3 Probabiliy 4 Probabiliy disribuios 5 Probabiliy Desiies Orgaizaio ad descripio of daa 6 Samplig disribuios 7 Ifereces cocerig a mea 8 Comparig wo reames

More information

Remarks: (a) The Dirac delta is the function zero on the domain R {0}.

Remarks: (a) The Dirac delta is the function zero on the domain R {0}. Sectio Objective(s): The Dirc s Delt. Mi Properties. Applictios. The Impulse Respose Fuctio. 4.4.. The Dirc Delt. 4.4. Geerlized Sources Defiitio 4.4.. The Dirc delt geerlized fuctio is the limit δ(t)

More information

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4)

1. Solve by the method of undetermined coefficients and by the method of variation of parameters. (4) 7 Differeial equaios Review Solve by he mehod of udeermied coefficies ad by he mehod of variaio of parameers (4) y y = si Soluio; we firs solve he homogeeous equaio (4) y y = 4 The correspodig characerisic

More information

O & M Cost O & M Cost

O & M Cost O & M Cost 5/5/008 Turbie Reliabiliy, Maieace ad Faul Deecio Zhe Sog, Adrew Kusiak 39 Seamas Ceer Iowa Ciy, Iowa 54-57 adrew-kusiak@uiowa.edu Tel: 39-335-5934 Fax: 39-335-5669 hp://www.icae.uiowa.edu/~akusiak Oulie

More information

Another Approach to Solution. of Fuzzy Differential Equations

Another Approach to Solution. of Fuzzy Differential Equations Applied Memil Siees, Vol. 4, 00, o. 6, 777-790 Aoer Appro o Soluio o Fuzz Diereil Equios C. Durism Deprme o Memis ogu Egieerig College Peruduri, Erode-68 05 Tmildu, Idi d@kogu..i B. Us Deprme o Memis ogu

More information

Transverse Vibrations of Elastic Thin Beam Resting on Variable Elastic Foundations and Subjected to Traveling Distributed Forces.

Transverse Vibrations of Elastic Thin Beam Resting on Variable Elastic Foundations and Subjected to Traveling Distributed Forces. Trasverse Vibraios of Elasic Thi Beam Resig o Variable Elasic Foudaios ad Subjeced o Travelig Disribued Forces. B. Omolofe ad S.N. Oguyebi * Deparme of Mahemaical Scieces, Federal Uiversiy of Techology,

More information

Integration and Differentiation

Integration and Differentiation ome Clculus bckgroud ou should be fmilir wih, or review, for Mh 404 I will be, for he mos pr, ssumed ou hve our figerips he bsics of (mulivrible) fucios, clculus, d elemer differeil equios If here hs bee

More information

The Eigen Function of Linear Systems

The Eigen Function of Linear Systems 1/25/211 The Eige Fucio of Liear Sysems.doc 1/7 The Eige Fucio of Liear Sysems Recall ha ha we ca express (expad) a ime-limied sigal wih a weighed summaio of basis fucios: v ( ) a ψ ( ) = where v ( ) =

More information

Linear System Theory

Linear System Theory Naioal Tsig Hua Uiversiy Dearme of Power Mechaical Egieerig Mid-Term Eamiaio 3 November 11.5 Hours Liear Sysem Theory (Secio B o Secio E) [11PME 51] This aer coais eigh quesios You may aswer he quesios

More information

λiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi

λiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi Liear lgebra Lecure #9 Noes This week s lecure focuses o wha migh be called he srucural aalysis of liear rasformaios Wha are he irisic properies of a liear rasformaio? re here ay fixed direcios? The discussio

More information

ETNA Kent State University

ETNA Kent State University & ( Elecroic Trscios o Numericl Alysis Volume 29, pp 31-5, 2007 Copyrigh 2007, Ke Se iversiy ISSN 1068-9613 Ke Se iversiy e@mcseedu PRECONDITIONING BLOCK TOEPLITZ MATRICES THOMAS K HCKLE AND DIMITRIOS

More information

Notes 03 largely plagiarized by %khc

Notes 03 largely plagiarized by %khc 1 1 Discree-Time Covoluio Noes 03 largely plagiarized by %khc Le s begi our discussio of covoluio i discree-ime, sice life is somewha easier i ha domai. We sar wih a sigal x[] ha will be he ipu io our

More information

OBSERVER DESIGN FOR A BILINEAR MODEL OF A CONTINUOUS COUNTERCURRENT ION EXCHANGE PROCESS.

OBSERVER DESIGN FOR A BILINEAR MODEL OF A CONTINUOUS COUNTERCURRENT ION EXCHANGE PROCESS. 9 SUT ARICA ISTITUTE EECTRICA EGIEERS Vol.7 4 Decemer 6 BSERVER DESIG R A BIIEAR MDE A CTIUUS CUTERCURRET I EXCAGE PRCESS..M. Due* d R.T. Tzoev** * Dep. of Elecricl Egieerig Bellville Cpe Peisul Uiversiy

More information

EGR 544 Communication Theory

EGR 544 Communication Theory EGR 544 Commuicaio heory 7. Represeaio of Digially Modulaed Sigals II Z. Aliyazicioglu Elecrical ad Compuer Egieerig Deparme Cal Poly Pomoa Represeaio of Digial Modulaio wih Memory Liear Digial Modulaio

More information

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming*

Some Properties of Semi-E-Convex Function and Semi-E-Convex Programming* The Eighh Ieraioal Symposium o Operaios esearch ad Is Applicaios (ISOA 9) Zhagjiajie Chia Sepember 2 22 29 Copyrigh 29 OSC & APOC pp 33 39 Some Properies of Semi-E-Covex Fucio ad Semi-E-Covex Programmig*

More information

Extended Laguerre Polynomials

Extended Laguerre Polynomials I J Coemp Mah Scieces, Vol 7, 1, o, 189 194 Exeded Laguerre Polyomials Ada Kha Naioal College of Busiess Admiisraio ad Ecoomics Gulberg-III, Lahore, Pakisa adakhaariq@gmailcom G M Habibullah Naioal College

More information

Chapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu

Chapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu Caper : Time-Domai Represeaios of Liear Time-Ivaria Sysems Ci-Wei Liu Oulie Iroucio Te Covoluio Sum Covoluio Sum Evaluaio Proceure Te Covoluio Iegral Covoluio Iegral Evaluaio Proceure Iercoecios of LTI

More information

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering

Department of Electronics & Telecommunication Engineering C.V.Raman College of Engineering Lcur No Lcur-6-9 Ar rdig his lsso, you will lr ou Fourir sris xpsio rigoomric d xpoil Propris o Fourir Sris Rspos o lir sysm Normlizd powr i Fourir xpsio Powr spcrl dsiy Ec o rsr ucio o PSD. FOURIER SERIES

More information

Electrical Engineering Department Network Lab.

Electrical Engineering Department Network Lab. Par:- Elecrical Egieerig Deparme Nework Lab. Deermiaio of differe parameers of -por eworks ad verificaio of heir ierrelaio ships. Objecive: - To deermie Y, ad ABD parameers of sigle ad cascaded wo Por

More information

z line a) Draw the single phase equivalent circuit. b) Calculate I BC.

z line a) Draw the single phase equivalent circuit. b) Calculate I BC. ECE 2260 F 08 HW 7 prob 4 solutio EX: V gyb' b' b B V gyc' c' c C = 101 0 V = 1 + j0.2 Ω V gyb' = 101 120 V = 6 + j0. Ω V gyc' = 101 +120 V z LΔ = 9 j1.5 Ω ) Drw the sigle phse equivlet circuit. b) Clculte

More information

B. Maddah INDE 504 Simulation 09/02/17

B. Maddah INDE 504 Simulation 09/02/17 B. Maddah INDE 54 Simulaio 9/2/7 Queueig Primer Wha is a queueig sysem? A queueig sysem cosiss of servers (resources) ha provide service o cusomers (eiies). A Cusomer requesig service will sar service

More information

Compact Finite Difference Schemes for Solving a Class of Weakly- Singular Partial Integro-differential Equations

Compact Finite Difference Schemes for Solving a Class of Weakly- Singular Partial Integro-differential Equations Ma. Sci. Le. Vol. No. 53-0 (0 Maemaical Scieces Leers A Ieraioal Joural @ 0 NSP Naural Scieces Publisig Cor. Compac Fiie Differece Scemes for Solvig a Class of Weakly- Sigular Parial Iegro-differeial Equaios

More information

12 Getting Started With Fourier Analysis

12 Getting Started With Fourier Analysis Commuicaios Egieerig MSc - Prelimiary Readig Geig Sared Wih Fourier Aalysis Fourier aalysis is cocered wih he represeaio of sigals i erms of he sums of sie, cosie or complex oscillaio waveforms. We ll

More information

Suggested Solution for Pure Mathematics 2011 By Y.K. Ng (last update: 8/4/2011) Paper I. (b) (c)

Suggested Solution for Pure Mathematics 2011 By Y.K. Ng (last update: 8/4/2011) Paper I. (b) (c) per I. Le α 7 d β 7. The α d β re he roos o he equio, such h α α, β β, --- α β d αβ. For, α β For, α β α β αβ 66 The seme is rue or,. ssume Cosider, α β d α β y deiiio α α α α β or some posiive ieer.

More information

Vibratory Motion. Prof. Zheng-yi Feng NCHU SWC. National CHung Hsing University, Department of Soil and Water Conservation

Vibratory Motion. Prof. Zheng-yi Feng NCHU SWC. National CHung Hsing University, Department of Soil and Water Conservation Vibratory Motio Prof. Zheg-yi Feg NCHU SWC 1 Types of vibratory motio Periodic motio Noperiodic motio See Fig. A1, p.58 Harmoic motio Periodic motio Trasiet motio impact Trasiet motio earthquake A powerful

More information

ECE 570 Session 7 IC 752-E Computer Aided Engineering for Integrated Circuits. Transient analysis. Discuss time marching methods used in SPICE

ECE 570 Session 7 IC 752-E Computer Aided Engineering for Integrated Circuits. Transient analysis. Discuss time marching methods used in SPICE ECE 570 Sessio 7 IC 75-E Compuer Aided Egieerig for Iegraed Circuis Trasie aalysis Discuss ime marcig meods used i SPICE. Time marcig meods. Explici ad implici iegraio meods 3. Implici meods used i circui

More information

INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS)

INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS) Mthemtics Revisio Guides Itegrtig Trig, Log d Ep Fuctios Pge of MK HOME TUITION Mthemtics Revisio Guides Level: AS / A Level AQA : C Edecel: C OCR: C OCR MEI: C INTEGRATION TECHNIQUES (TRIG, LOG, EXP FUNCTIONS)

More information

Clock Skew and Signal Representation

Clock Skew and Signal Representation Clock Skew ad Sigal Represeaio Ch. 7 IBM Power 4 Chip 0/7/004 08 frequecy domai Program Iroducio ad moivaio Sequeial circuis, clock imig, Basic ools for frequecy domai aalysis Fourier series sigal represeaio

More information

ANALYSIS HW 3. f(x + y) = f(x) + f(y) for all real x, y. Demonstration: Let f be such a function. Since f is smooth, f exists.

ANALYSIS HW 3. f(x + y) = f(x) + f(y) for all real x, y. Demonstration: Let f be such a function. Since f is smooth, f exists. ANALYSIS HW 3 CLAY SHONKWILER () Fid ll smooth fuctios f : R R with the property f(x + y) = f(x) + f(y) for ll rel x, y. Demostrtio: Let f be such fuctio. Sice f is smooth, f exists. The The f f(x + h)

More information

Available online at J. Math. Comput. Sci. 4 (2014), No. 4, ISSN:

Available online at   J. Math. Comput. Sci. 4 (2014), No. 4, ISSN: Available olie a hp://sci.org J. Mah. Compu. Sci. 4 (2014), No. 4, 716-727 ISSN: 1927-5307 ON ITERATIVE TECHNIQUES FOR NUMERICAL SOLUTIONS OF LINEAR AND NONLINEAR DIFFERENTIAL EQUATIONS S.O. EDEKI *, A.A.

More information

NEIGHBOURHOODS OF A CERTAIN SUBCLASS OF STARLIKE FUNCTIONS. P. Thirupathi Reddy. E. mail:

NEIGHBOURHOODS OF A CERTAIN SUBCLASS OF STARLIKE FUNCTIONS. P. Thirupathi Reddy. E. mail: NEIGHOURHOOD OF CERTIN UCL OF TRLIKE FUNCTION P Tirupi Reddy E mil: reddyp@yooom sr: Te im o is pper is o rodue e lss ( sulss o ( sisyig e odio wi is ( ) p < 0< E We sudy eigouroods o is lss d lso prove

More information

Fourier Series and Applications

Fourier Series and Applications 9/7/9 Fourier Series d Applictios Fuctios epsio is doe to uderstd the better i powers o etc. My iportt probles ivolvig prtil dieretil equtios c be solved provided give uctio c be epressed s iiite su o

More information

Optimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis

Optimization of Rotating Machines Vibrations Limits by the Spring - Mass System Analysis Joural of aerials Sciece ad Egieerig B 5 (7-8 (5 - doi: 765/6-6/57-8 D DAVID PUBLISHING Opimizaio of Roaig achies Vibraios Limis by he Sprig - ass Sysem Aalysis BENDJAIA Belacem sila, Algéria Absrac: The

More information

6.003: Signals and Systems

6.003: Signals and Systems 6.003: Sigals ad Sysems Lecure 8 March 2, 2010 6.003: Sigals ad Sysems Mid-erm Examiaio #1 Tomorrow, Wedesday, March 3, 7:30-9:30pm. No reciaios omorrow. Coverage: Represeaios of CT ad DT Sysems Lecures

More information

Math 2414 Homework Set 7 Solutions 10 Points

Math 2414 Homework Set 7 Solutions 10 Points Mah Homework Se 7 Soluios 0 Pois #. ( ps) Firs verify ha we ca use he iegral es. The erms are clearly posiive (he epoeial is always posiive ad + is posiive if >, which i is i his case). For decreasig we

More information

6.003 Homework #5 Solutions

6.003 Homework #5 Solutions 6. Homework #5 Soluios Problems. DT covoluio Le y represe he DT sigal ha resuls whe f is covolved wih g, i.e., y[] = (f g)[] which is someimes wrie as y[] = f[] g[]. Deermie closed-form expressios for

More information

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory

Ideal Amplifier/Attenuator. Memoryless. where k is some real constant. Integrator. System with memory Liear Time-Ivaria Sysems (LTI Sysems) Oulie Basic Sysem Properies Memoryless ad sysems wih memory (saic or dyamic) Causal ad o-causal sysems (Causaliy) Liear ad o-liear sysems (Lieariy) Sable ad o-sable

More information

EE757 Numerical Techniques in Electromagnetics Lecture 9

EE757 Numerical Techniques in Electromagnetics Lecture 9 EE757 uericl Techiques i Elecroeics Lecure 9 EE757 06 Dr. Mohed Bkr Diereil Equios Vs. Ierl Equios Ierl equios ke severl ors e.. b K d b K d Mos diereil equios c be epressed s ierl equios e.. b F d d /

More information

Let s express the absorption of radiation by dipoles as a dipole correlation function.

Let s express the absorption of radiation by dipoles as a dipole correlation function. MIT Deparme of Chemisry 5.74, Sprig 004: Iroducory Quaum Mechaics II Isrucor: Prof. Adrei Tokmakoff p. 81 Time-Correlaio Fucio Descripio of Absorpio Lieshape Le s express he absorpio of radiaio by dipoles

More information

Horizontal product differentiation: Consumers have different preferences along one dimension of a good.

Horizontal product differentiation: Consumers have different preferences along one dimension of a good. Produc Differeiio Firms see o e uique log some dimesio h is vlued y cosumers. If he firm/roduc is uique i some resec, he firm c commd rice greer h cos. Horizol roduc differeiio: Cosumers hve differe refereces

More information

Chapter Simpson s 1/3 Rule of Integration. ( x)

Chapter Simpson s 1/3 Rule of Integration. ( x) Cper 7. Smpso s / Rule o Iegro Aer redg s per, you sould e le o. derve e ormul or Smpso s / rule o egro,. use Smpso s / rule o solve egrls,. develop e ormul or mulple-segme Smpso s / rule o egro,. use

More information

Advection! Discontinuous! solutions shocks! Shock Speed! ! f. !t + U!f. ! t! x. dx dt = U; t = 0

Advection! Discontinuous! solutions shocks! Shock Speed! ! f. !t + U!f. ! t! x. dx dt = U; t = 0 p://www.d.edu/~gryggva/cfd-course/ Advecio Discoiuous soluios socks Gréar Tryggvaso Sprig Discoiuous Soluios Cosider e liear Advecio Equaio + U = Te aalyic soluio is obaied by caracerisics d d = U; d d

More information

P a g e 5 1 of R e p o r t P B 4 / 0 9

P a g e 5 1 of R e p o r t P B 4 / 0 9 P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e

More information