Microwave Engineering

Size: px
Start display at page:

Download "Microwave Engineering"

Transcription

1 Micrwave Engineering Cheng-Hsing Hsu Deparmen f Elecrical Engineering Nainal Unied Universiy

2 Ouline. Transmissin ine Thery. Transmissin ines and Waveguides eneral Sluins fr TEM, TE, and TM waves ; Parallel Plae waveguide ; ecangular Waveguide ; Caxial ine ; Sripline ; Micrsrip 3. Micrwave Newrk Analysis Impedance and Equivalen Vlages and Currens ; Impedance and Admiance Marices ; The Scaering Marix ; ABCD Marix ; Signal Flw raphs ; Discninuies and Mdel Analysis 4. Impedance Maching and Tuning Maching wih umped Elemens ; Single-Sub Tuning ; Duble-Sub Tuning ; The Quarer-Wave Transfrmer ; The Thery f Small eflecins 5. Micrwave esnars Series and Parallel esnan Circuis ; Transmissin ine esnars ; ecangular Waveguide Caviies Dielecric esnars 6. Pwer Dividers and Direcinal Cuplers Basic Prperies f Dividers and Cuplers ; The T-Juncin Pwer Divider ; The Wilkinsn Pwer Divider ; Cupled ine Direcinal Cuplers ; 8 hybrid 7. Micrwave Filers Peridic Srucure ; Filer Design by he Inserin ss Mehd ; Filer Transfrmains ; Filer Implemenain ; Elecrnic Maerials and Devices Applicains ab

3 4. Impedance Maching and Tuning Maching wih umped Elemens Single-Sub Tuning Duble-Sub Tuning The Quarer-Wave Transfrmer The Thery f Small eflecins Tapered ines Elecrnic Maerials and Devices Applicains ab

4 Impedance maching is fen a par f he larger design prcess fr a micrwave cmpnen r sysem, and he maching circui is ideally lssless, avid unnecessary lss f pwer and is usually designed s ha he impedance seen lking in he maching newrk is. Then reflecins are eliminaed n he ransmissin line he lef f he maching newrk. Impedance maching r uning is impran fr he fllwing reasns: (I) Maximum pwer is delivered when he lad is mached he line (assuming he generar is mached), and pwer lss in he feed line is minimized. (II) Impedance maching sensiive receiver cmpnens (anenna, lw-nise amplifier, ec) imprves he signal--nise rai f he sysem. (III) Impedance maching in a pwer disribuin newrk (such as an anenna array feed newrk) will reduce ampliude and phase errrs. As lng as he lad impedance,, has sme nnzer real par. Facrs ha may be impran in he secin f a paricular maching newrk include he fllwing: Cmplexiy - he simples design ha saisfies he required specificains is generally he ms preferable Bandwidh Implemenain - depending n he ype f ransmissin line r waveguide being used ; uning subs are much easier implemen in waveguide Adjusabiliy adjusmen mach a variable lad impedance A lssless newrk maching an arbirary lad impedance a ransmissin line. Elecrnic Maerials and Devices Applicains ab

5 Maching wih umped Elemens ( Newrks) Simples ype f maching newrk is he -secin, which uses w reacive elemens mach an arbirary lad impedance a ransmissin line. => If he nrmalized lad impedance, z = /, is inside he + j x circle n he Smih Char, hen he circui as he fig. (a). If he nrmalized lad impedance is uside he + j x circle n he Smih Char, hen he circui as he fig. (b). The + j x circle is he resisance circle n he impedance Smih Char fr which r =. In addiin, he reacive elemens may be eiher inducrs r capacirs., depending n he lad impedance. (eigh disinc pssibiliies fr he maching circui fr varius lad impedance) -secin maching newrks. (a) Newrk fr z inside he + jx circle. (b) Newrk fr z uside he + jx circle. Elecrnic Maerials and Devices Applicains ab

6 Elecrnic Maerials and Devices Applicains ab

7 Analyic Sluins Cnsider he circui f Fig. (a), le = + j X => We saed ha his circui wuld be used when z = / is inside he + j x circle n he Smih char => implies ha > The impedance seen lking in he maching newrk fllwed by he lad impedance mus be equal, fr a mach jx jb / jx B X X ; X BX Since X B earranging and separaing in real and imaginary pars gives w equains fr he w unknwns, X and B The sluin is / X Then he series reacance can be fund as X B Slving abve equain fr X and subsiuing in abve equain gives a quadraic equain fr B. X X B X, he argumen f he secnd square r is always psiive. Tw sluins are pssible fr B and X. Bh f hese sluins are physically realizable, since bh psiive and negaive values f B and X are pssible. (psiive X implies an inducr, negaive X implies a capacir, while psiive B implies a capacir and negaive B implies an inducr) B -secin maching newrks. (a) Newrk fr z inside he + jx circle. (b) Newrk fr z uside he + jx circle. Elecrnic Maerials and Devices Applicains ab

8 Elecrnic Maerials and Devices Applicains ab

9 Cnsider he circui f Fig. (b), le = + j X => We saed ha his circui wuld be used when z = / is uside he + j x circle n he Smih char => implies ha < The admiance seen lking in he maching newrk fllwed by he lad impedance mus be equal /, fr a mach jb j X jx earranging and separaing in real and imaginary pars gives w equains fr he w unknwns, X B X X ; X X Slving abve equain fr The sluin is X B / X X B X and subsiuing in abve equain gives a quadraic equain fr B. Since, he argumen f he square rs are always psiive. In rder mach an arbirary cmplex lad a line f characerisic impedance, he real par f he inpu impedance he maching newrk mus be, while he imaginary par mus be zer. This implies ha a general maching newrk mus have a leas w degrees f freedm => in he -secin maching circui hese w degrees f freedm are prvided by he values f w reacive cmpnens. ; B / and B -secin maching newrks. (a) Newrk fr z inside he + jx circle. (b) Newrk fr z uside he + jx circle. Elecrnic Maerials and Devices Applicains ab

10 Elecrnic Maerials and Devices Applicains ab

11 EX: Design an -secin maching newrk mach a series C lad wih an impedance = j, a line, a a frequency f 5MHz. Elecrnic Maerials and Devices Applicains ab

12 Elecrnic Maerials and Devices Applicains ab

13 Single-Sub Tuning I is anher cnsider a maching echnique ha uses a single pen-circuied r shrcircuied lengh f a ransmissin line (a sub ), cnneced eiher in parallel r in series wih he ransmissin feed line a a cerain disance frm he lad. The w adjusable parameers are he disance, d, frm he lad he sub psiin, and he value f suscepance r reacance prvided by he shun r series sub. [ Fr shun : selec d s ha he admiance,, seen lking in he line a disance d frm he lad is f he frm +jb -> hen he sub suscepance is chsen as jb ] ; [ Fr series : he disance d is seleced s ha he impedance,, seen lking in he line a a disance d frm he lad, is f he frm +jx -> hen he sub reacance is chsen as jx ] The prper lengh f pen r shred T can be prvide any desired value f reacance and impedance Can mach varius impedance (real par ) Elecrnic Maerials and Devices Applicains ab

14 Elecrnic Maerials and Devices Applicains ab

15 Shun subs Elecrnic Maerials and Devices Applicains ab

16 EX. Fr a lad impedance =6-j8, design w single-sub (shr circui) shun uning newrks mach his lad a 5 line. Assuming ha he lad is mached a Hz, and he lad cnsiss f a resiser and capacir in series, pl he reflecin cefficien magniude frm Hz 3 Hz fr each sluin. <Sl> nrmalized lad impedance: z =.-j.6 -> cnsruc he apprpriae SW circle, and cnver he lad admiance, y. -> Nw nice ha SW circle inersecs he +jb circle a w pins (y and y ). Thus he disance d, frm he lad he sub, is given by eiher f hese w inersecins. eading he WT scale => d = =.; d = =.6 There is an infinie number f disances, d, n he SW circle ha inersec he +jb circle. Usually, i is desired keep he maching sub as clse as pssible he lad, imprve he bandwidh f he mach and reduce lsses caused by a pssibly large sanding wave rai n he line beween he sub and he lad. y =. + j.47 ; y =. j.47 => suscepance f j.47 and j.47 l =.95; l =.45 lad impedance => = 6and C =.995 pf Elecrnic Maerials and Devices Applicains ab

17 Sluin Example 5.. (a) Smih char fr he shun-sub uners. Elecrnic Maerials and Devices Applicains ab

18 Elecrnic Maerials and Devices Applicains ab -B B B B l B B l, fr π π fr, π d / -X X X X X / d X X X B X jb d jx j j jx j X / l d s s s s where an an : - circuied sub a shr fr an an an pen - circuied sub : fr an an hen, If fr, / chsen s ha ) is (which implies Nw ; where, is pin The admiance a his an where line frm he lad is f d, lengh, dwn a he impedance le he lad impedance be wrien as, and T derive frmulas fr

19 Series Subs Elecrnic Maerials and Devices Applicains ab

20 EX. Mach a lad impedance f =+j8 a 5 line using a single series pen-circui sub. Assuming ha he lad is mached a Hz, and he lad cnsiss f a resiser and inducr in series, pl he reflecin cefficien magniude frm Hz 3 Hz fr each sluin. <Sl> nrmalized lad impedance: z =-j.6 -> draw he SW circle. Fr he series-sub design, he char is an impedance char. -> Nw nice ha SW circle inersecs he +jx circle a w pins (z and z ). The shres disance, d, frm he lad he sub is, frm he WT scale, => d =.38.8 =.; while he secnd disance is d = (.5.8)+.7 =.463 z =. - j.33 ; z =. + j.33 => reacance f j.33 and -j.33 l =.397; l =.3 lad impedance => = and = 6.37 ph Elecrnic Maerials and Devices Applicains ab

21 Sluin Example 5.3. (a) Smih char fr he series-sub uners. Elecrnic Maerials and Devices Applicains ab

22 Elecrnic Maerials and Devices Applicains ab -X X X X l X X l, fr π π fr, π d / -B B B B B / d B B B X B jx d jb j j jb d j B / l d s s s s where an an : an pen - circuied sub fr an an : - circuied sub a shr fr an an hen, If fr, / chsen s ha ) is (which implies Nw ; where, is pin The admiance a his /,and an where line frm he lad is f, lengh, dwn a he admiance le he lad admiance be wrien as fr he series - sub uner,, and T derive frmulas fr

23 Duble-Sub Tuning The duble sub uner, which uses w uning subs in fixed psiins, can be used. Such uners are fen fabricaed in caxial line, wih adjusable subs cnneced in parallel he main caxial line. -> he duble sub uner cann mach all lad impedances. The duble sub uner circui, where he lad may be an arbirary disance frm he firs sub. Alhugh his is mre represenaive f pracical siuain, where he lad has been ransfrmed back he psiin f he firs sub, is easier deal wih and des n lse any generaliy. => he subs are shun subs, which are usually easier implemen in pracice han are series subs. (pen-circuied r shr-circuied) => d /8 r 3/ 8 Elecrnic Maerials and Devices Applicains ab

24 Smih Char Sluin. The suscepance f he firs sub, b (b ), mves he lad admiance y (y ) => These pins lie n he raed + jb circle; he amun f rain is d wavelengh ward he lad, where d is he elecrical disance beween he w sub.. Transfrming y (y ) ward he generar hrugh a lengh, d, f line leaves us a he pin y (y ) which mus be n he +jb circle. => he secnd sub hen adds a suscepance b (b ), which brings us he cener f he char, and cmplee mach. Elecrnic Maerials and Devices Applicains ab

25 EX. Design a duble sub shun uner mach a lad impedance =6-j8 a 5 line. The subs are be pen-circuied subs, and are spaced / 8 apar. Assuming ha his lad cnsiss f a series resisr and capacir, and ha he mach frequency is Hz, pl he reflecin cefficien magniude verus frequency frm Hz 3 Hz. <Sl> nrmalized lad admiance: y =.3+j.4. -> cnsruc he raed +jb cnducance circle, by mving every pin n he g = circle / 8 ward he lad => he firs sub : b =.34 ; b = -.4 => Transfrm he / 8 secin f line by raing alng a cnsan radius (SW) circle / 8 ward he generar => y = - j3.38 ; y = + j.38 The suscepance f he secnd sub shuld be b = 3.38 ; b = -.38 The lenghs f he pen-circuied subs are hen fund as l =.46, l =.48; l =.4, l =.35 lad impedance => = 6and C =.995 pf Elecrnic Maerials and Devices Applicains ab

26 Sluin Example 5.4. (a) Smih char fr he duble-sub uners. Elecrnic Maerials and Devices Applicains ab

27 The lef f he firs sub, he admiance is and B Since 4 is he suscepance f he firs sub. jb A his pin, he real par f B B B 4 B B is real, he quaniy wihin he square r which gives he range n he secnd sub suscepance B l fr pen - circuied sub : an ls fr shr - circuied sub : an Afer d has been fixed, he firs sub suscepance can be deermined Afer ransfrming hrugh a lengh d f ransmissin line, he admiance jus he righ f he secnd sub is B j -B B B B jb jb where an d,and mus equal Slving fr, which leads he equain ha can bemached fr a given sub spacing, d. B B j / : mus be nnnegaive B sin where, d where B B r B jb is he lad admiance Elecrnic Maerials and Devices Applicains ab

28 The quarer-wave ransfrmer The quarer-wave ransfrmer is a simple and useful circui fr maching a real lad impedance a ransmissin line. An addiinal feaure f he quarer-wave ransfrmer is ha i can be exended mulisecin designs in a mehdical manner, fr brader bandwidh. => If nly a narrw band impedance mach is required, a single-secin ransfrmer may suffice. One drawback f he quarer-wave ransfrmer is ha i can nly mach a real lad impedance. => A cmplex lad impedance can always be ransfrmed a real impedance by using an apprpriae lengh f ransmissin line beween he lad and he ransfrmer, r an apprpriae series r shun reacive subs. Elecrnic Maerials and Devices Applicains ab

29 The single secin quarer wave maching ransfrmer circui is shwn in Figure. The characerisic impedance f Γ Since Γ A he design frequency, f where an d an,and j j, his reduces Γ he reflecin cefficien magniude is / 4 4 / in in Γ bu a her frequencies he lengh is differen s a prefec mach is n lnger bained The inpu impedance seen lking in he maching secin is and he fracinal band widh is csθ, If we assume TEM lines, hen he maching secin is fr θnear π/ πf v p θ βl v 4 f Δf f p, he elecrical lengh f he maching secin is λ/ 4, f j apprximae expressin fr he mismach versus frequency f f πf, f m f f / θ m in 4θm π j j l / a he design frequency, f., since an 4 cs π θ sec Nw if we assume ha he frequency is near he design frequency, f, hen l λ/ 4 and θ π/.then sec sec Γm Γ m θ herefre he frequency f he lwer band edge a θ θ Elecrnic Maerials and Devices Applicains ab θ m

30 The hery f small reflecin Single-secin Transfrmer = ( - )/( + ) ; = - ; 3 = ( - )/( + ) ; T = + = /( + ) ; T = + = /( + ) ; Elecrnic Maerials and Devices Applicains ab

31 Mulisecin Transfrmer Parial reflecin cefficiens can be defined a each juncins = ( - )/( + ) ; n = ( n+! - n )/( n+ + n ) ; N =( - N )/( + N ) ; Elecrnic Maerials and Devices Applicains ab

32 Taped ines Discuss hw an arbirary real lad impedance culd be mached a line ver a desired bandwidh by using mulisecin maching ransfrmers => As he number, N, f discree secins increases, he sep changes in characerisic impedance beween he secins becme smaller.=> Thus, in he limi f an infinie number f secins, we apprach a cninuusly apered line. A apered ransmissin line maching secin and he mdel fr an incremenal lengh f apered line. (a) The apered ransmissin line maching secin. (b) Mdel fr an incremenal sep change in impedance f he apered line. Elecrnic Maerials and Devices Applicains ab

33 A maching secin wih an expnenial impedance aper. (a) Variain f impedance. (b) esuling reflecin cefficien magniude respnse. A maching secin wih a riangular aper fr d(in //dz. (a) Variain f impedance. (b) esuling reflecin cefficien magniude respnse. Elecrnic Maerials and Devices Applicains ab

34 Elecrnic Maerials and Devices Applicains ab

Impedance Matching and Tuning

Impedance Matching and Tuning Impedance Maching and Tuning Impedance Maching and Tuning Impedance maching or uning is imporan for he following reasons: Maximum power is delivered Improve he SN of he sysem educe ampliude and phase errors

More information

5.1 Angles and Their Measure

5.1 Angles and Their Measure 5. Angles and Their Measure Secin 5. Nes Page This secin will cver hw angles are drawn and als arc lengh and rains. We will use (hea) represen an angle s measuremen. In he figure belw i describes hw yu

More information

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering

Unit-I (Feedback amplifiers) Features of feedback amplifiers. Presentation by: S.Karthie, Lecturer/ECE SSN College of Engineering Uni-I Feedback ampliiers Feaures eedback ampliiers Presenain by: S.Karhie, Lecurer/ECE SSN Cllege Engineering OBJECTIVES T make he sudens undersand he eec negaive eedback n he llwing ampliier characerisics:

More information

Kinematics Review Outline

Kinematics Review Outline Kinemaics Review Ouline 1.1.0 Vecrs and Scalars 1.1 One Dimensinal Kinemaics Vecrs have magniude and direcin lacemen; velciy; accelerain sign indicaes direcin + is nrh; eas; up; he righ - is suh; wes;

More information

Visco-elastic Layers

Visco-elastic Layers Visc-elasic Layers Visc-elasic Sluins Sluins are bained by elasic viscelasic crrespndence principle by applying laplace ransfrm remve he ime variable Tw mehds f characerising viscelasic maerials: Mechanical

More information

The Buck Resonant Converter

The Buck Resonant Converter EE646 Pwer Elecrnics Chaper 6 ecure Dr. Sam Abdel-Rahman The Buck Resnan Cnverer Replacg he swich by he resnan-ype swich, ba a quasi-resnan PWM buck cnverer can be shwn ha here are fur mdes f pera under

More information

PHY305F Electronics Laboratory I. Section 2. AC Circuit Basics: Passive and Linear Components and Circuits. Basic Concepts

PHY305F Electronics Laboratory I. Section 2. AC Circuit Basics: Passive and Linear Components and Circuits. Basic Concepts PHY305F Elecrnics abrary I Secin ircui Basics: Passie and inear mpnens and ircuis Basic nceps lernaing curren () circui analysis deals wih (sinusidally) ime-arying curren and lage signals whse ime aerage

More information

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302)

ELEG 205 Fall Lecture #10. Mark Mirotznik, Ph.D. Professor The University of Delaware Tel: (302) EEG 05 Fall 07 ecure #0 Mark Mirznik, Ph.D. Prfessr The Universiy f Delaware Tel: (3083-4 Email: mirzni@ece.udel.edu haper 7: apacirs and Inducrs The apacir Symbl Wha hey really lk like The apacir Wha

More information

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components

The Components of Vector B. The Components of Vector B. Vector Components. Component Method of Vector Addition. Vector Components Upcming eens in PY05 Due ASAP: PY05 prees n WebCT. Submiing i ges yu pin ward yur 5-pin Lecure grade. Please ake i seriusly, bu wha cuns is wheher r n yu submi i, n wheher yu ge hings righ r wrng. Due

More information

10.7 Temperature-dependent Viscoelastic Materials

10.7 Temperature-dependent Viscoelastic Materials Secin.7.7 Temperaure-dependen Viscelasic Maerials Many maerials, fr example plymeric maerials, have a respnse which is srngly emperaure-dependen. Temperaure effecs can be incrpraed in he hery discussed

More information

Physics 111. Exam #1. September 28, 2018

Physics 111. Exam #1. September 28, 2018 Physics xam # Sepember 8, 08 ame Please read and fllw hese insrucins carefully: Read all prblems carefully befre aemping slve hem. Yur wrk mus be legible, and he rganizain clear. Yu mus shw all wrk, including

More information

21.9 Magnetic Materials

21.9 Magnetic Materials 21.9 Magneic Maerials The inrinsic spin and rbial min f elecrns gives rise he magneic prperies f maerials è elecrn spin and rbis ac as iny curren lps. In ferrmagneic maerials grups f 10 16-10 19 neighbring

More information

AP Physics 1 MC Practice Kinematics 1D

AP Physics 1 MC Practice Kinematics 1D AP Physics 1 MC Pracice Kinemaics 1D Quesins 1 3 relae w bjecs ha sar a x = 0 a = 0 and mve in ne dimensin independenly f ne anher. Graphs, f he velciy f each bjec versus ime are shwn belw Objec A Objec

More information

( ) For more files visit

( ) For more files visit SETION A (75 marks). This quesin cnsiss f TWENTYFIVE subquesins (..5) f ONE mark each. Fr each f hese subquesins, fur pssible alernaives (A,B, and D) are given, u f which ONLY ONE is crrec. Indicae he

More information

Brace-Gatarek-Musiela model

Brace-Gatarek-Musiela model Chaper 34 Brace-Gaarek-Musiela mdel 34. Review f HJM under risk-neural IP where f ( T Frward rae a ime fr brrwing a ime T df ( T ( T ( T d + ( T dw ( ( T The ineres rae is r( f (. The bnd prices saisfy

More information

Physics Courseware Physics I Constant Acceleration

Physics Courseware Physics I Constant Acceleration Physics Curseware Physics I Cnsan Accelerain Equains fr cnsan accelerain in dimensin x + a + a + ax + x Prblem.- In he 00-m race an ahlee acceleraes unifrmly frm res his p speed f 0m/s in he firs x5m as

More information

Motion Along a Straight Line

Motion Along a Straight Line PH 1-3A Fall 010 Min Alng a Sraigh Line Lecure Chaper (Halliday/Resnick/Walker, Fundamenals f Physics 8 h ediin) Min alng a sraigh line Sudies he min f bdies Deals wih frce as he cause f changes in min

More information

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder.

Coherent PSK. The functional model of passband data transmission system is. Signal transmission encoder. x Signal. decoder. Cheren PSK he funcinal mdel f passand daa ransmissin sysem is m i Signal ransmissin encder si s i Signal Mdular Channel Deecr ransmissin decder mˆ Carrier signal m i is a sequence f syml emied frm a message

More information

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271.

PRINCE SULTAN UNIVERSITY Department of Mathematical Sciences Final Examination Second Semester (072) STAT 271. PRINCE SULTAN UNIVERSITY Deparmen f Mahemaical Sciences Final Examinain Secnd Semeser 007 008 (07) STAT 7 Suden Name Suden Number Secin Number Teacher Name Aendance Number Time allwed is ½ hurs. Wrie dwn

More information

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS*

ON THE COMPONENT DISTRIBUTION COEFFICIENTS AND SOME REGULARITIES OF THE CRYSTALLIZATION OF SOLID SOLUTION ALLOYS IN MULTICOMPONENT SYSTEMS* METL 006.-5.5.006, Hradec nad Mravicí ON THE OMPONENT DISTRIUTION OEFFIIENTS ND SOME REGULRITIES OF THE RYSTLLIZTION OF SOLID SOLUTION LLOYS IN MULTIOMPONENT SYSTEMS* Eugenij V.Sidrv a, M.V.Pikunv b, Jarmír.Drápala

More information

CHAPTER 5. Exercises. the coefficient of t so we have ω = 200π

CHAPTER 5. Exercises. the coefficient of t so we have ω = 200π HPTER 5 Exerises E5. (a) We are given v ( ) 5 s(π 3 ). The angular frequeny is he effiien f s we have ω π radian/s. Then f ω / π Hz T / f ms m / 5 / 6. Furhermre, v() aains a psiive peak when he argumen

More information

Revelation of Soft-Switching Operation for Isolated DC to Single-phase AC Converter with Power Decoupling

Revelation of Soft-Switching Operation for Isolated DC to Single-phase AC Converter with Power Decoupling Revelain f Sf-Swiching Operain fr Islaed DC Single-phase AC Cnverer wih wer Decupling Nagisa Takaka, Jun-ichi Ih Dep. f Elecrical Engineering Nagaka Universiy f Technlgy Nagaka, Niigaa, Japan nakaka@sn.nagakau.ac.jp,

More information

Optimization of Four-Button BPM Configuration for Small-Gap Beam Chambers

Optimization of Four-Button BPM Configuration for Small-Gap Beam Chambers Opimizain f Fur-Bun BPM Cnfigurain fr Small-Gap Beam Chamers S. H. Kim Advanced Phn Surce Argnne Nainal Larary 9700 Suh Cass Avenue Argnne, Illinis 60439 USA Asrac. The cnfigurain f fur-un eam psiin mnirs

More information

DC-DC Switch-Mode Converters

DC-DC Switch-Mode Converters - Swich-Mde nverers - cnverers are used : egulaed swich-mde pwer supplies, nrmally wih HF elecrical isla Mr drives, nrmally wihu an isla ransfrmer We will lk a he w basic dc-dc cnverer plgies: Sep-dwn

More information

3 ) = 10(1-3t)e -3t A

3 ) = 10(1-3t)e -3t A haper 6, Sluin. d i ( e 6 e ) 0( - )e - A p i 0(-)e - e - 0( - )e -6 W haper 6, Sluin. w w (40)(80 (40)(0) ) ( ) w w w 0 0 80 60 kw haper 6, Sluin. i d 80 60 40x0 480 ma haper 6, Sluin 4. i (0) 6sin 4-0.7

More information

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur

Module 4. Analysis of Statically Indeterminate Structures by the Direct Stiffness Method. Version 2 CE IIT, Kharagpur Mdle Analysis f Saically Indeerminae Srcres by he Direc Siffness Mehd Versin CE IIT, Kharagr Lessn The Direc Siffness Mehd: Temerare Changes and Fabricain Errrs in Trss Analysis Versin CE IIT, Kharagr

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 15 10/30/2013. Ito integral for simple processes MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.7J Fall 13 Lecure 15 1/3/13 I inegral fr simple prcesses Cnen. 1. Simple prcesses. I ismery. Firs 3 seps in cnsrucing I inegral fr general prcesses 1 I inegral

More information

Lecture Outline. Introduction Transmission Line Equations Transmission Line Wave Equations 8/10/2018. EE 4347 Applied Electromagnetics.

Lecture Outline. Introduction Transmission Line Equations Transmission Line Wave Equations 8/10/2018. EE 4347 Applied Electromagnetics. 8/10/018 Course Insrucor Dr. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: rcrumpf@uep.edu EE 4347 Applied Elecromagneics Topic 4a Transmission Line Equaions Transmission These Line noes

More information

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from

CHAPTER 7 CHRONOPOTENTIOMETRY. In this technique the current flowing in the cell is instantaneously stepped from CHAPTE 7 CHONOPOTENTIOMETY In his echnique he curren flwing in he cell is insananeusly sepped frm zer sme finie value. The sluin is n sirred and a large ecess f suppring elecrlye is presen in he sluin;

More information

INFLUENCE OF WIND VELOCITY TO SUPPLY WATER TEMPERATURE IN HOUSE HEATING INSTALLATION AND HOT-WATER DISTRICT HEATING SYSTEM

INFLUENCE OF WIND VELOCITY TO SUPPLY WATER TEMPERATURE IN HOUSE HEATING INSTALLATION AND HOT-WATER DISTRICT HEATING SYSTEM Dr. Branislav Zivkvic, B. Eng. Faculy f Mechanical Engineering, Belgrade Universiy Predrag Zeknja, B. Eng. Belgrade Municipal DH Cmpany Angelina Kacar, B. Eng. Faculy f Agriculure, Belgrade Universiy INFLUENCE

More information

a. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with

a. (1) Assume T = 20 ºC = 293 K. Apply Equation 2.22 to find the resistivity of the brass in the disk with Aignmen #5 EE7 / Fall 0 / Aignmen Sluin.7 hermal cnducin Cnider bra ally wih an X amic fracin f Zn. Since Zn addiin increae he number f cnducin elecrn, we have cale he final ally reiiviy calculaed frm

More information

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018

Answers: ( HKMO Heat Events) Created by: Mr. Francis Hung Last updated: 21 September 2018 nswers: (009-0 HKMO Hea Evens) reaed by: Mr. Francis Hung Las updaed: Sepember 08 09-0 Individual 6 7 7 0 Spare 8 9 0 08 09-0 8 0 0.8 Spare Grup 6 0000 7 09 8 00 9 0 0 Individual Evens I In hw many pssible

More information

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring

An Introduction to Wavelet Analysis. with Applications to Vegetation Monitoring An Inrducin Wavele Analysis wih Applicains Vegeain Mniring Dn Percival Applied Physics Labrary, Universiy f Washingn Seale, Washingn, USA verheads fr alk available a hp://saff.washingn.edu/dbp/alks.hml

More information

Impact Switch Study Modeling & Implications

Impact Switch Study Modeling & Implications L-3 Fuzing & Ordnance Sysems Impac Swich Sudy Mdeling & Implicains Dr. Dave Frankman May 13, 010 NDIA 54 h Annual Fuze Cnference This presenain cnsiss f L-3 Crprain general capabiliies infrmain ha des

More information

51. Elektrijada, Kopaonik

51. Elektrijada, Kopaonik may 11. 51. Elekrijada Kpanik Tes in Physics 1. A mbile is frmed by suppring fur meal buerflies f equal mass m frm a sring f lengh L. The pins f suppr are evenly spaced a disance l apar as shwn in Figure

More information

Examples of Complex Sound Fields:

Examples of Complex Sound Fields: UIUC Physics 406 Acusical Physics f Music Eamples f Cmple Sund Fields: Eample # 0: Generic 3-D Mnchrmaic Traveling Wave: Befre we launch in discussing several specific eamples f cmple sund fields/sund

More information

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical.

Lecture 4 ( ) Some points of vertical motion: Here we assumed t 0 =0 and the y axis to be vertical. Sme pins f erical min: Here we assumed and he y axis be erical. ( ) y g g y y y y g dwnwards 9.8 m/s g Lecure 4 Accelerain The aerage accelerain is defined by he change f elciy wih ime: a ; In analgy,

More information

The 37th International Physics Olympiad Singapore. Experimental Competition. Wednesday, 12 July, Sample Solution

The 37th International Physics Olympiad Singapore. Experimental Competition. Wednesday, 12 July, Sample Solution The 37h Inernainal Physics Olypiad Singapre Experienal Cpeiin Wednesday, July, 006 Saple Sluin Par a A skech f he experienal seup (n required) Receiver Raing able Gnieer Fixed ar Bea splier Gnieer Mvable

More information

Nelson Primary School Written Calculation Policy

Nelson Primary School Written Calculation Policy Addiin Fundain Y1 Y2 Children will engage in a wide variey f sngs, rhymes, games and aciviies. They will begin relae addiin cmbining w grups f bjecs. They will find ne mre han a given number. Cninue develp

More information

Productivity changes of units: A directional measure of cost Malmquist index

Productivity changes of units: A directional measure of cost Malmquist index Available nline a hp://jnrm.srbiau.ac.ir Vl.1, N.2, Summer 2015 Jurnal f New Researches in Mahemaics Science and Research Branch (IAU Prduciviy changes f unis: A direcinal measure f cs Malmquis index G.

More information

Lecture 3: Resistive forces, and Energy

Lecture 3: Resistive forces, and Energy Lecure 3: Resisive frces, and Energy Las ie we fund he velciy f a prjecile ving wih air resisance: g g vx ( ) = vx, e vy ( ) = + v + e One re inegrain gives us he psiin as a funcin f ie: dx dy g g = vx,

More information

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures

THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES. Part 3: The Calculation of C* for Natural Gas Mixtures A REPORT ON THE DETERMINATION OF CRITICAL FLOW FACTORS FOR NATURAL GAS MIXTURES Par 3: The Calculain f C* fr Naural Gas Mixures FOR NMSPU Deparmen f Trade and Indusry 151 Buckingham Palace Rad Lndn SW1W

More information

Lecture II Simple One-Dimensional Vibrating Systems

Lecture II Simple One-Dimensional Vibrating Systems UIUC Physics 406 Acusical Physics f Music Lecure II Simple One-Dimensinal Vibraing Sysems One mehd f prducing a sund relies n a physical bjec (e.g. varius ypes f musical insrumens sringed and wind insrumens

More information

Chapter 4 AC Network Analysis

Chapter 4 AC Network Analysis haper 4 A Nework Analysis Jaesung Jang apaciance Inducance and Inducion Time-Varying Signals Sinusoidal Signals Reference: David K. heng, Field and Wave Elecromagneics. Energy Sorage ircui Elemens Energy

More information

Efficient and Fast Simulation of RF Circuits and Systems via Spectral Method

Efficient and Fast Simulation of RF Circuits and Systems via Spectral Method Efficien and Fas Simulain f RF Circuis and Sysems via Specral Mehd 1. Prjec Summary The prpsed research will resul in a new specral algrihm, preliminary simular based n he new algrihm will be subsanially

More information

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is UNIT IMPULSE RESPONSE, UNIT STEP RESPONSE, STABILITY. Uni impulse funcion (Dirac dela funcion, dela funcion) rigorously defined is no sricly a funcion, bu disribuion (or measure), precise reamen requires

More information

An application of nonlinear optimization method to. sensitivity analysis of numerical model *

An application of nonlinear optimization method to. sensitivity analysis of numerical model * An applicain f nnlinear pimizain mehd sensiiviy analysis f numerical mdel XU Hui 1, MU Mu 1 and LUO Dehai 2 (1. LASG, Insiue f Amspheric Physics, Chinese Academy f Sciences, Beijing 129, China; 2. Deparmen

More information

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3

d 1 = c 1 b 2 - b 1 c 2 d 2 = c 1 b 3 - b 1 c 3 and d = c b - b c c d = c b - b c c This process is coninued unil he nh row has been compleed. The complee array of coefficiens is riangular. Noe ha in developing he array an enire row may be divided or

More information

Dr. Kasra Etemadi February 20, 2007

Dr. Kasra Etemadi February 20, 2007 Dr. Kasra Eeadi February, 7 Seady-Sae Sinusidal Analysis Sinusidal Surces: Elecric pwer disribued fr residences and businesses Radi cunicain All signal f pracical ineres are cpsed f sinusidal cpnens Furier

More information

CHAPTER 18: Electric Currents. Answers to Questions

CHAPTER 18: Electric Currents. Answers to Questions CHTE : Elecric Currens nswers Quesins. mpere-hurs measures charge. The ampere is a charge per uni ime, an he hur is a ime, s he pruc is charge. mpere-hur f charge is 6 Culmbs f charge.. n he circui (n

More information

Introduction to Smith Charts

Introduction to Smith Charts Intrductin t Smith Charts Dr. Russell P. Jedlicka Klipsch Schl f Electrical and Cmputer Engineering New Mexic State University as Cruces, NM 88003 September 2002 EE521 ecture 3 08/22/02 Smith Chart Summary

More information

PASSIVE PFC FOR FLYBACK CONVERTORS

PASSIVE PFC FOR FLYBACK CONVERTORS PASSIE PFC FOR FLYBACK COERORS Parviz Par and Keyue M Sedley Dep f Elecrical and Cpuer Engineering Universiy f Califrnia, Irvine Irvine, Califrnia 9697 Absrac A new passive Pwer Facr Crrecr (PFC) based

More information

Problem Set #1. i z. the complex propagation constant. For the characteristic impedance:

Problem Set #1. i z. the complex propagation constant. For the characteristic impedance: Problem Se # Problem : a) Using phasor noaion, calculae he volage and curren waves on a ransmission line by solving he wave equaion Assume ha R, L,, G are all non-zero and independen of frequency From

More information

CHAPTER 5. Solutions for Exercises

CHAPTER 5. Solutions for Exercises HAPTE 5 Slutins fr Exercises E5. (a We are given v ( t 50 cs(00π t 30. The angular frequency is the cefficient f t s we have ω 00π radian/s. Then f ω / π 00 Hz T / f 0 ms m / 50 / 06. Furthermre, v(t attains

More information

Method of Orthogonal Potentials Developed for the Analysis of TEM Mode Electromagnetic Resonators

Method of Orthogonal Potentials Developed for the Analysis of TEM Mode Electromagnetic Resonators 14-016-01-01_00 R.F. Ne #15 NSCL June 1, 005 Jhn incen Mehd f Orhgnal Penials Develed fr he Analysis f TEM Mde Elecrmagneic Resnars INTRODUCTION... DEELOPMENT... 3 E, H FIELD, ω... 4 SUMMARY EQUATIONS...

More information

Announcements. Formulas Review. Exam format

Announcements. Formulas Review. Exam format Annuncemens 1. N hmewrk due mrrw! a. Wuld be an ecellen eening sud fr and/r ake he eam. Eam 1 sars da! a. Aailable in Tesing Cener frm Tues, Sep. 16 10:15 am, up Mnda, Sep, clsing ime i. If u pick up ur

More information

GAMS Handout 2. Utah State University. Ethan Yang

GAMS Handout 2. Utah State University. Ethan Yang Uah ae Universiy DigialCmmns@UU All ECAIC Maerials ECAIC Repsiry 2017 GAM Handu 2 Ehan Yang yey217@lehigh.edu Fllw his and addiinal wrs a: hps://digialcmmns.usu.edu/ecsaic_all Par f he Civil Engineering

More information

DISTANCE PROTECTION OF HVDC TRANSMISSION LINE WITH NOVEL FAULT LOCATION TECHNIQUE

DISTANCE PROTECTION OF HVDC TRANSMISSION LINE WITH NOVEL FAULT LOCATION TECHNIQUE IJRET: Inernainal Jurnal f Research in Engineering and Technlgy eissn: 9-6 pissn: -78 DISTANCE PROTECTION OF HVDC TRANSMISSION LINE WITH NOVEL FAULT LOCATION TECHNIQUE Ruchia Nale, P. Suresh Babu Suden,

More information

Chapter 3. DC to DC CONVERTER (CHOPPER)

Chapter 3. DC to DC CONVERTER (CHOPPER) Chaper 3 C C COEE General Buck cnverer Bs cnverer (CHOPPE Buck-Bs cnverer Swiche-e pwer supply Brige cnverer es n elecragneic cpaibiliy (EMC an sluins. Pwer Elecrnics an rives (ersin : r. C-C Cnverer (Chpper

More information

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period.

Ramsey model. Rationale. Basic setup. A g A exogenous as in Solow. n L each period. Ramsey mdel Rainale Prblem wih he Slw mdel: ad-hc assumpin f cnsan saving rae Will cnclusins f Slw mdel be alered if saving is endgenusly deermined by uiliy maximizain? Yes, bu we will learn a l abu cnsumpin/saving

More information

SMKA NAIM LILBANAT KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI. Kertas soalan ini mengandungi 7 halaman bercetak.

SMKA NAIM LILBANAT KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI. Kertas soalan ini mengandungi 7 halaman bercetak. Name : Frm :. SMKA NAIM LILBANAT 55 KOTA BHARU KELANTAN. SEKOLAH BERPRESTASI TINGGI PEPERIKSAAN PERCUBAAN SPM / ADDITIONAL MATHEMATICS Keras ½ Jam ½ Jam Unuk Kegunaan Pemeriksa Arahan:. This quesin paper

More information

6.003: Signals and Systems

6.003: Signals and Systems 6.3: Signals and Sysems Lecure 7 April 8, 6.3: Signals and Sysems C Fourier ransform C Fourier ransform Represening signals by heir frequency conen. X(j)= x()e j d ( analysis equaion) x()= π X(j)e j d

More information

CHAPTER 14 CHEMICAL KINETICS

CHAPTER 14 CHEMICAL KINETICS CHAPTER 4 CHEMICAL KINETICS PRACTICE EXAMPLES A B (E) The rae f cnsumpin fr a reacan is expressed as he negaive f he change in mlariy divided by he ime inerval. The rae f reacin is expressed as he rae

More information

6 th International Conference on Trends in Agricultural Engineering 7-9 September 2016, Prague, Czech Republic

6 th International Conference on Trends in Agricultural Engineering 7-9 September 2016, Prague, Czech Republic THEORETICAL INVESTIGATIONS OF MINERAL FERTILISER DISTRIBTION BY MEANS OF AN INCLINED CENTRIFGAL TOOL V. Bulgakv 1, O. Adamchuk, S. Ivanvs 3 1 Nainal niversiy Lie and Envirnmenal Sciences kraine Nainal

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signals & Sysems Prof. Mar Fowler Noe Se #1 C-T Signals: Circuis wih Periodic Sources 1/1 Solving Circuis wih Periodic Sources FS maes i easy o find he response of an RLC circui o a periodic source!

More information

ECE 5318/6352 Antenna Engineering. Spring 2006 Dr. Stuart Long. Chapter 6. Part 7 Schelkunoff s Polynomial

ECE 5318/6352 Antenna Engineering. Spring 2006 Dr. Stuart Long. Chapter 6. Part 7 Schelkunoff s Polynomial ECE 538/635 Antenna Engineering Spring 006 Dr. Stuart Lng Chapter 6 Part 7 Schelkunff s Plynmial 7 Schelkunff s Plynmial Representatin (fr discrete arrays) AF( ψ ) N n 0 A n e jnψ N number f elements in

More information

Basic Circuit Elements Professor J R Lucas November 2001

Basic Circuit Elements Professor J R Lucas November 2001 Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions

More information

Section 12 Time Series Regression with Non- Stationary Variables

Section 12 Time Series Regression with Non- Stationary Variables Secin Time Series Regressin wih Nn- Sainary Variables The TSMR assumpins include, criically, he assumpin ha he variables in a regressin are sainary. Bu many (ms?) ime-series variables are nnsainary. We

More information

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers

University of Cyprus Biomedical Imaging and Applied Optics. Appendix. DC Circuits Capacitors and Inductors AC Circuits Operational Amplifiers Universiy of Cyprus Biomedical Imaging and Applied Opics Appendix DC Circuis Capaciors and Inducors AC Circuis Operaional Amplifiers Circui Elemens An elecrical circui consiss of circui elemens such as

More information

Strengthening of web opening in non-compact steel girders

Strengthening of web opening in non-compact steel girders IOSR Jurnal f Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-1684,p-ISSN: 2320-334X, Vlume 12, Issue 5 Ver. II (Sep. - Oc. 2015), PP 34-47 www.isrjurnals.rg Srenghening f web pening in nn-cmpac

More information

K The slowest step in a mechanism has this

K The slowest step in a mechanism has this CM 6 Generl Chemisry II Nme SLUTINS Exm, Spring 009 Dr. Seel. (0 pins) Selec he nswer frm he clumn n he righ h bes mches ech descripin frm he clumn n he lef. Ech nswer cn be used, ms, nly nce. E G This

More information

SINUSOIDAL WAVEFORMS

SINUSOIDAL WAVEFORMS SINUSOIDAL WAVEFORMS The sinusoidal waveform is he only waveform whose shape is no affeced by he response characerisics of R, L, and C elemens. Enzo Paerno CIRCUIT ELEMENTS R [ Ω ] Resisance: Ω: Ohms Georg

More information

Subject: Turbojet engines (continued); Design parameters; Effect of mass flow on thrust.

Subject: Turbojet engines (continued); Design parameters; Effect of mass flow on thrust. 16.50 Leure 19 Subje: Turbje engines (ninued; Design parameers; Effe f mass flw n hrus. In his haper we examine he quesin f hw hse he key parameers f he engine bain sme speified perfrmane a he design ndiins,

More information

Physics for Scientists & Engineers 2

Physics for Scientists & Engineers 2 Direc Curren Physics for Scieniss & Engineers 2 Spring Semeser 2005 Lecure 16 This week we will sudy charges in moion Elecric charge moving from one region o anoher is called elecric curren Curren is all

More information

IE1206 Embedded Electronics

IE1206 Embedded Electronics E06 Embedded Elecronics Le Le3 Le4 Le Ex Ex P-block Documenaion, Seriecom Pulse sensors,, R, P, serial and parallel K LAB Pulse sensors, Menu program Sar of programing ask Kirchhoffs laws Node analysis

More information

For example, the comb filter generated from. ( ) has a transfer function. e ) has L notches at ω = (2k+1)π/L and L peaks at ω = 2π k/l,

For example, the comb filter generated from. ( ) has a transfer function. e ) has L notches at ω = (2k+1)π/L and L peaks at ω = 2π k/l, Comb Filers The simple filers discussed so far are characeried eiher by a single passband and/or a single sopband There are applicaions where filers wih muliple passbands and sopbands are required The

More information

Numerical solution of some types of fractional optimal control problems

Numerical solution of some types of fractional optimal control problems Numerical Analysis and Scienific mpuing Preprin Seria Numerical sluin f sme ypes f fracinal pimal cnrl prblems N.H. Sweilam T.M. Al-Ajmi R.H.W. Hppe Preprin #23 Deparmen f Mahemaics Universiy f Husn Nvember

More information

Differentiation Applications 1: Related Rates

Differentiation Applications 1: Related Rates Differentiatin Applicatins 1: Related Rates 151 Differentiatin Applicatins 1: Related Rates Mdel 1: Sliding Ladder 10 ladder y 10 ladder 10 ladder A 10 ft ladder is leaning against a wall when the bttm

More information

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2

Hall effect. Formulae :- 1) Hall coefficient RH = cm / Coulumb. 2) Magnetic induction BY 2 Page of 6 all effec Aim :- ) To deermine he all coefficien (R ) ) To measure he unknown magneic field (B ) and o compare i wih ha measured by he Gaussmeer (B ). Apparaus :- ) Gauss meer wih probe ) Elecromagne

More information

Phys1112: DC and RC circuits

Phys1112: DC and RC circuits Name: Group Members: Dae: TA s Name: Phys1112: DC and RC circuis Objecives: 1. To undersand curren and volage characerisics of a DC RC discharging circui. 2. To undersand he effec of he RC ime consan.

More information

Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter).

Three charges, all with a charge of 10 C are situated as shown (each grid line is separated by 1 meter). Three charges, all with a charge f 0 are situated as shwn (each grid line is separated by meter). ) What is the net wrk needed t assemble this charge distributin? a) +0.5 J b) +0.8 J c) 0 J d) -0.8 J e)

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180

Chapters 6 & 7: Trigonometric Functions of Angles and Real Numbers. Divide both Sides by 180 Algebra Chapers & : Trigonomeric Funcions of Angles and Real Numbers Chapers & : Trigonomeric Funcions of Angles and Real Numbers - Angle Measures Radians: - a uni (rad o measure he size of an angle. rad

More information

RC, RL and RLC circuits

RC, RL and RLC circuits Name Dae Time o Complee h m Parner Course/ Secion / Grade RC, RL and RLC circuis Inroducion In his experimen we will invesigae he behavior of circuis conaining combinaions of resisors, capaciors, and inducors.

More information

EE 101 Electrical Engineering. vrect

EE 101 Electrical Engineering. vrect EE Elecrical Engineering ac heory 3. Alernaing urren heory he advanage of he alernaing waveform for elecric power is ha i can be sepped up or sepped down in poenial easily for ransmission and uilisaion.

More information

Fractional Order Disturbance Observer based Robust Control

Fractional Order Disturbance Observer based Robust Control 201 Inernainal Cnference n Indusrial Insrumenain and Cnrl (ICIC) Cllege f Engineering Pune, India. May 28-30, 201 Fracinal Order Disurbance Observer based Rbus Cnrl Bhagyashri Tamhane 1, Amrua Mujumdar

More information

(2) Even if such a value of k was possible, the neutrons multiply

(2) Even if such a value of k was possible, the neutrons multiply CHANGE OF REACTOR Nuclear Thery - Curse 227 POWER WTH REACTVTY CHANGE n this lessn, we will cnsider hw neutrn density, neutrn flux and reactr pwer change when the multiplicatin factr, k, r the reactivity,

More information

if N =2 J, obtain analysis (decomposition) of sample variance:

if N =2 J, obtain analysis (decomposition) of sample variance: Wavele Mehds fr Time Series Analysis Eamples: Time Series X Versus Time Inde Par VII: Wavele Variance and Cvariance X (a) (b) eamples f ime series mivae discussin decmpsiin f sample variance using waveles

More information

HW6: MRI Imaging Pulse Sequences (7 Problems for 100 pts)

HW6: MRI Imaging Pulse Sequences (7 Problems for 100 pts) HW6: MRI Imaging Pulse Sequences (7 Problems for 100 ps) GOAL The overall goal of HW6 is o beer undersand pulse sequences for MRI image reconsrucion. OBJECTIVES 1) Design a spin echo pulse sequence o image

More information

Lead/Lag Compensator Frequency Domain Properties and Design Methods

Lead/Lag Compensator Frequency Domain Properties and Design Methods Lectures 6 and 7 Lead/Lag Cmpensatr Frequency Dmain Prperties and Design Methds Definitin Cnsider the cmpensatr (ie cntrller Fr, it is called a lag cmpensatr s K Fr s, it is called a lead cmpensatr Ntatin

More information

6.003: Signals and Systems Lecture 20 November 17, 2011

6.003: Signals and Systems Lecture 20 November 17, 2011 6.3: Signals and Sysems Lecure November 7, 6.3: Signals and Sysems Applicaions of Fourier ransforms Filering Noion of a filer. LI sysems canno creae new frequencies. can only scale magniudes and shif phases

More information

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in

Circuit Variables. AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters per second to miles per second: 1 ft 12 in Circui Variables 1 Assessmen Problems AP 1.1 Use a produc of raios o conver wo-hirds he speed of ligh from meers per second o miles per second: ( ) 2 3 1 8 m 3 1 s 1 cm 1 m 1 in 2.54 cm 1 f 12 in 1 mile

More information

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax .7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical

More information

Analysis of Microstrip Coupling Gap to Estimate Polymer Permittivity

Analysis of Microstrip Coupling Gap to Estimate Polymer Permittivity Analysis of Microsrip Couplin Gap o Esimae Polymer Permiiviy Chanchal Yadav Deparmen of Physics & Elecronics Rajdhani Collee, Universiy of Delhi Delhi, India Absrac A ap in he microsrip line can be modeled

More information

Lab 11 LRC Circuits, Damped Forced Harmonic Motion

Lab 11 LRC Circuits, Damped Forced Harmonic Motion Physics 6 ab ab 11 ircuits, Damped Frced Harmnic Mtin What Yu Need T Knw: The Physics OK this is basically a recap f what yu ve dne s far with circuits and circuits. Nw we get t put everything tgether

More information

11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work

11. HAFAT İş-Enerji Power of a force: Power in the ability of a force to do work MÜHENDİSLİK MEKNİĞİ. HFT İş-Eneji Pwe f a fce: Pwe in he abiliy f a fce d wk F: The fce applied n paicle Q P = F v = Fv cs( θ ) F Q v θ Pah f Q v: The velciy f Q ÖRNEK: İŞ-ENERJİ ω µ k v Calculae he pwe

More information

6.003 Homework #8 Solutions

6.003 Homework #8 Solutions 6.003 Homework #8 Soluions Problems. Fourier Series Deermine he Fourier series coefficiens a k for x () shown below. x ()= x ( + 0) 0 a 0 = 0 a k = e /0 sin(/0) for k 0 a k = π x()e k d = 0 0 π e 0 k d

More information

Chapter 1 Electric Circuit Variables

Chapter 1 Electric Circuit Variables Chaper 1 Elecric Circui Variables Exercises Exercise 1.2-1 Find he charge ha has enered an elemen by ime when i = 8 2 4 A, 0. Assume q() = 0 for < 0. 8 3 2 Answer: q () = 2 C 3 () 2 i = 8 4 A 2 8 3 2 8

More information

Small Combustion Chamber. Combustion chamber area ratio

Small Combustion Chamber. Combustion chamber area ratio Lsses & Real Effecs in Nzzles Flw divergence Nnunifrmiy p lss due hea addiin Viscus effecs bundary layers-drag bundary layer-shck ineracins Hea lsses Nzzle ersin (hra) Transiens Muliphase flw Real gas

More information

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC

EE 435. Lecture 31. Absolute and Relative Accuracy DAC Design. The String DAC EE 435 Lecure 3 Absolue and Relaive Accuracy DAC Design The Sring DAC . Review from las lecure. DFT Simulaion from Malab Quanizaion Noise DACs and ADCs generally quanize boh ampliude and ime If convering

More information