Package Inductance and RLC Circuit Analysis. New Today. Bondwires. Package Parasitics. Model for Invertor with Inductance. Inductance (Inductantie)

Size: px
Start display at page:

Download "Package Inductance and RLC Circuit Analysis. New Today. Bondwires. Package Parasitics. Model for Invertor with Inductance. Inductance (Inductantie)"

Transcription

1 Package Inucance an ircui Analyi New Toay FATO Jawel, ik a beken al fenomeen Tenmine oner mahemaici En in wikung aangelege kringen Mijn naam, al u he ween wil i i Ik zi in allerlei berekeningen En aan he eine hef ik mij weer op U vraag nie, enk ik, om verhanelingen Maar wen a ik mezelf nu een onpop Welnu ik ben e worel ui Ik funcioneer, ofchoon ik nie bea Denk aar maar een langurig over na (Ui: Dr. P en Marjolein Kool, Wi en nauurlyriek me chemich upplemen, Ameram: Nijgh en van Dimar, h. 5 Inucive effec, for wiching (ranien behavior Applicaion of omplex Number elaion beween complex exponenial an harmonic (inuoial funcion Damping facor, ampe naural frequency, unampe naural frequency Ocillaory behavior (oplingering oncep of overampe, criically ampe, unerampe an unampe repone /7/4 7 inucance /7/4 7 inucance Package Paraiic Bull Microproceor hip Nee raniion from ubmicron onchip worl o PB (prine ircui Boar worl elaively large package paraiic Paraiic = unwane bu nonavoiable elecrical effec Inucance of package mu ofen be accoune for Onchip inerconnec inucance alo becoming imporan Bonwire: connecion from ilicon chip o package pin Bonwire /7/4 7 inucance 3 /7/4 7 inucance 4 Moel for Inveror wih Inucance Inucance (Inucanie 5 V power Many inereing properie an we eermine pee an oher properie of uch yem? i v v = v in in p n groun v ou Aion of o an migh reul in ocillaing behavior! Nee complex number o eal wih i. i v v i = an exhibi ual role of i an v aue many inereing an ueful properie of elecrical circui an circui analyi We will apply hi righ now! /7/4 7 inucance 5 /7/4 7 inucance 6

2 D Equivalen ircui D value of capacior curren: vc v = c c = i = D moel for i open circui Dual! D value of inucor volage: = = v = D moel for i hor circui /7/4 7 inucance 7 = V A V Fir Orer ircui i v : τ = : τ = / F: waveform IV: iniial value FV: final value. Ue KV for circui wih > : V i =. earrange: = i V 3. ompare o cae: v c = vc V 4. emember general formula: F = (IV FV e (/τ FV 5. Wrie own reul (by inpecion: V ( V i ( i ( e = /7/4 7 inucance 8 acae Inveror wih Inucance 5V power p Package an power upply Simplify ircui Driving gae Inerconnec p in oa gae power 5V n power groun Package an power upply groun in in Driving gae Inerconnec p n in oa gae in 5V V groun n i in v c in Prooypical erie circui Principal ubjec of hi chaper /7/4 7 inucance /7/4 7 inucance ircui Differenial Equaion V v c v c = i Sae variable: v, i Noe: KV for inucor volage i ual from K for capacior curren v i v v c i =i v KV aroun loop V v v v = V i v = /7/4 7 inucance ircui Differenial Equaion K & KV v c = i V V i v = ewrie vc = i V = v i v = V i i v c /7/4 7 inucance

3 v = V i Two couple fir orer D.E. Nex: fin v c an i Saify D.E. Saify iniial conion v c (, i ( Proceure: Aume general oluion Deermine eay ae oluion Fin naural frequencie (, Deermine coefficien of ran. par General Proceure General meho ienical o an cae /7/4 7 inucance 3 v Aume General Soluion ( = v ( V = V e V e V ( = i ( I = I e I e I i V in Deermine Seay Sae Soluion i v c V = v c ( = I = i ( = V in /7/4 7 inucance Fin Naural Frequencie v = V i e = x = = haraceriic Equaion of erie circui Sign of Dicriminan = Noe: c a = ; b = ; c = = ± a b c = b ± = D criminan Four ae epenng on ign of criminan D > like an overampe D = = criically ampe 3 D < an unerampe 4 = e( i = unampe b 4 ac a Will be explaine horly Nex: Suy cae,, 3 an 4 /7/4 7 inucance 5 /7/4 7 inucance 6 Damping Overampe criically ampe unerampe unampe Wha oe i mean? Many yem vibrae/ocillae/cycle (more or le repeiive behavior mechanical yem, elecrical, economic, Damping i he mechanim ha rie o uppre ocillaion an force he yem ino able eayae chokemper of a car emper of Eramu brige Brige can ocillae! Tacoma Narrow Brige Tacoma Narrow Brige, November 7, 4 /7/4 7 inucance 7 /7/4 7 inucance 8 3

4 //4 7 inucance Tacoma Narrow Brige ae : Overampe Serie epone Solve for v = V i e = x = = haraceriic Equaion of erie circui = = ± Now conier cae of > > D> = 5.8. Two real naural frequencie No exra fficulie compare o or cae Sricly ecaying ranien oluion /7/4 7 inucance /7/4 7 inucance ae : riically Dampe epone Now conier cae of = ± D= = > = = = : amping facor Houon, we have a problem 5.8. Becaue = = we woul have v ( = Ve Ve V = ( V V e V Then, V an V are no inepenen becaue hey refer o ame exponenial erm. Acually, V V can be replace by V. emember: for a econorer yem, we acually nee wo inepenen exponenial oluion an wo conan o aju for wo iniial conion. Similarly for i /7/4 7 inucance Secon Inepenen Soluion o D.E. e = e e = e e Mofie oluion: v c = V e V e V c Prouc rule v u u v = u v Derivaive (almo proporional o funcion i = I e I e I D = naural frequency Mofie oluion compare o or cae Overhoo in ranien oluion = e e More formal erivaion in D.E. coure /7/4 7 inucance riically Dampe Waveform v c = V e V e V c 8 7 V 5 6 V 5 V c ae 3: Unerampe epone Now conier cae of < > < Houon, we have anoher problem We nee quareroo of negaive number = ± Soluion: complex number See TIO omplexe ekenwijze FATO Jawel, ik a beken al fenomeen Tenmine oner mahemaici En in wikung aangelege kringen Mijn naam, al u he ween wil i i Ik zi in allerlei berekeningen En aan he eine hef ik mij weer op U vraag nie, enk ik, om verhanelingen Maar wen a ik mezelf nu een onpop Welnu ik ben e worel ui Ik funcioneer, ofchoon ik nie bea Denk aar maar een langurig over na D< (Ui: Dr. P en Marjolein Kool, Wi en nauurlyriek me chemich upplemen, Ameram: Nijgh en van Dimar, /7/4 7 inucance 3 /7/4 7 inucance 4 4

5 Imaginary Number We nee quareroo of negaive number We offer number of which he quare i onvenionally enoe a i: i = In EE, i i reerve for curren, ue j inea (j = Hence: x = j x = j x = j x Now, we have real number, e.g.,,.343, An imaginary number, e.g. 3j Their combinaion i calle a complex number omplex Number omplex number i um of real an imaginary number, e.g. 3j Aion keep real an imaginary par eparae: (3j (3j = j(33 = 6j Muliplicaion ue j = : (3j x (3j = 3j 3j j = 86j All normal rule for aion, ubracion, muliplicaion, viion, bu real an imaginary par are kep eparae, excep for j, which become /7/4 7 inucance 5 /7/4 7 inucance 6 b = Im(z omplex Plane an Polar Form imaginary axi bj z=abj e jϕ = coϕ jinϕ z = a bj real axi a = e(z r = z ϕ = arg(z z = r(coϕ jinϕ = r e jϕ Muliplicaion ofen eaier uing polar coornae: z z = z z arg(z z = arg(z arg(z (mo π Euler ieniy will be imporan = ± Unerampe epone Now conier cae of < > < ω e( = = ω = ± ± Damping facor ω Unampe naural frequency Woulbe naural frequency when = D< /7/4 7 inucance 7 /7/4 7 inucance 8 = omplex Naural Frequencie ± ω < = ± j ω = ± ( ( ω = ± j ω ω ω Im( = ω Dampe naural frequency = ± j ω > Main reul: wo complex naural frequencie = jω = jω = omplex Arihmeic for Unerampe epone an wo complex naural frequencie Alo nee complex coefficien in linear combinaion of boh inepenen oluion for v c an i eul: Familiar general oluion, bu wih complex arihmeic Bu we can have complex volage an curren, can we? v ( = Φ e Φ e V i ( = Γ e Γ e I i, Φi, Γi are complex /7/4 7 inucance /7/4 7 inucance 3 5

6 v ( = Φ e Φ e V i ( = Γ e Γ e I jω jω = Γ e Γ e I = e ( Γ( coω j inω Γ ( coω j inω I = e (( Γ Γ coω j( Γ Γ inω I Similar for v Apply Euler Ieniy Dilemma can be olve by exploiing Euler Ieniy e jϕ = coϕ jinϕ = jω = jω /7/4 7 inucance 3 eal or omplex? i = e ( (( Γ Γ coω j( Γ Γ inω I ook complicae complex Bu phyical ignal are imply real Soluion: Γ an Γ can no be choen inepenenly Im(Γ Γ = Im( j (Γ Γ = Γ an Γ mu be complex conjugae: e(γ = e(γ an Im(Γ = Im(Γ Γ = Γ ike an e: Γ = a jb an Γ = a jb Then: Γ Γ = a an j(γ Γ = b Finally, le: I = a an I = b learly eal! i ( = e ( Icoω I inω I Similar for v (See book /7/4 7 inucance 3 Γ an Γ are omplex onjugae If we wouln know ha Γ an Γ are complex conjugae, we can cover i a follow: Γ = a jb Γ = c j Unerampe epone Damping facor Dampe naural frequency i ( = e ( Icoω I inω I v ( = e ( Vcoω V inω V Γ Γ = a c j( b Im( Γ Γ = = b Γ Γ = a c j( b e( Γ Γ = a c = a = c Γ = a jb = Γ Exponenially ampe Sinuoial Waveform Seay Sae V i an I i again follow from iniial conion an erivaive a (our meho (or ubiuion of above general oluion in original DE (book /7/4 7 inucance 33 /7/4 7 inucance 34 Unerampe Waveform v ( = e ( Vcoω V inω V /7/4 7 inucance 35 ω V V V c ae 4: Unampe Serie epone When = =, ω =ω = ± = ± jω i ( = Icoω I inω I Ocillaing behavior, wihou amping, ocillaion coninue forever Perpeuum Mobile? = ± ω v ( = e ( V coω V inω V =, ω =ω v ( = Vcoω V inω V /7/4 7 inucance 36 6

7 eview of Naural Frequencie Digial Syem Swiching Spee The naural frequencie can be hown in complex plane Im Im Im Im e (x e e e ompare wiching pee wih an wihou upply line inucance Overampe riically Dampe Unerampe Unampe 5. ompleely worke example Bu alo ee oher example in book Fully worke example 5.7 /7/4 7 inucance 37 /7/4 7 inucance 38 Digial Syem Swiching Spee ompare an ae ou = Ω in = pf = nh V = 5V ou = Ω in = pf = nh V = 5V Deermine higholow waveform here Aume iniially high for long ime Wihou Wih Ω v? nh pf Ω v? pf ompare an cae /7/4 7 inucance 3 /7/4 7 inucance 4 Wihou Ω τ = Ω x pf =. ns v( = 5 pf v( = v = FV (IV FVe /τ = 5e /7/4 7 inucance Sraegy: Solving Secon Orer circui. Wrie own fferenial equaion (eermine ae var. Wrie own characeriic equaion an olve for 3. Aume general oluion, epenng on i, a in cheme below (A, B an can be curren or volage or Overampe: wo fferen, real riically ampe: = = 4. Solve for eay ae oluion, an conan (ue I.. an ime erivaive a 5. heck oluion! Ae Be Ae Be Unerampe: an = e( ω = Im ( complex conjugae e ( Aco ( ω Bco ( ω (unampe when = /7/4 7 inucance 4 7

8 Deermine (omplex Naural Frequencie Wrie Aume Soluion nh Ω v? i pf v = V i = 5 ± 8.66 j Uni: / hange econ ino nano econ (for convenience = 5 ± j Uni: /n = ± = ± = 5 ± 8.66 j Unerampe! = 5 Damping facor ω = 8.66 Dampe Naural Frequency ( = e ( V co( ω V in( ω V ( = e ( Ico( ω I in( ω I v i /7/4 7 inucance 43 /7/4 7 inucance 44 Seay Sae an Iniial Value Deermine onan nh Ω v? i pf ( = e ( V co( ω V in( ω V ( = e ( Ico( ω I in( ω I v i Fir: eayae value V =v ( = I =i ( = v ( = i ( = v ( = 5 i ( = Nex: Deermine conan (V, V, I, I From iniial conion From erivaive a (book ue ubiuion in D.E. /7/4 7 inucance 45 /7/4 7 inucance Ue Iniial onion (an SeaySae Value v ( = e ( V co( ω V in( ω V v ( = 5 = e ( V co( V in( V ( V V = V = V = 5 i ( = e ( Ico( ω I in( ω I i ( = = e ( Ico( I in( I ( I I = I = I = v ( = e ( 5co( ω V in( ω i ( e = I in ( ω.. 3. Prouc ule: Example: hain ule: Example: Analyi Tool eminer u e y y u = x u x x v u v = u v Analyi in = e in in e = e co e in u( x = ω x in( ωx = in( u ( ωx u x = co( u ω = ω co( ωx ombine: e in( ω = ωe co( ω e in( ω eview! Deermine e co ( ω /7/4 7 inucance 47 /7/4 7 inucance 48 8

9 Ue TimeDerivaive a for Aume Soluion v ( = e ( 5co( ω V in( ω v ( e = ( 5co( ω V in( ω e ( 5ω in( ω Vω co( ω Noe: Ue: co( = in( = e = Ue TimeDerivaive a for D.E. v v = ( = v ( i( = V i Known! = 5 = Hence: v ( = 5 Vω = ( = v = /7/4 7 inucance 4 /7/4 7 inucance 5 ombine TimeDerivaive Info a Inverer Pair Waveform v ( = 5 Vω = ( = v = V ω = 5 V =.8 earlier: ω = 8.66 = 5 Final reul ( in n: 5 v ( = e ( 5co( in( i =. 577e in( Final reul ( in n: 5 v ( = e ( 5co( in( i =. 577e in( Ue he preceng nh Ω v? pf v when = proceure for i. /7/4 7 inucance 5 /7/4 7 inucance 5 Summary: Solving Secon Orer circui. Wrie own fferenial equaion (eermine ae var. Wrie own characeriic equaion an olve for 3. Aume general oluion, epenng on i, a in cheme below (A, B an can be curren or volage or Overampe: wo fferen, real Ae Be riically ampe: = = 4. Solve for eay ae oluion, an conan (ue I.. an ime erivaive a 5. heck oluion! Ae Be Unerampe: an = e( ω = Im ( complex conjugae e ( Aco ( ω Bco ( ω (unampe when = /7/4 7 inucance 53

Package Inductance and RLC Circuit Analysis

Package Inductance and RLC Circuit Analysis Package Inucance an ircui Analyi FATO Jawel, ik a beken al fenomeen Tenmine oner mahemaici En in wikunig aangelege kringen Mijn naam, al u he ween wil i i Ik zi in allerlei berekeningen En aan he eine

More information

Chapter 8 Objectives

Chapter 8 Objectives haper 8 Engr8 ircui Analyi Dr uri Nelon haper 8 Objecive Be able o eermine he naural an he ep repone of parallel circui; Be able o eermine he naural an he ep repone of erie circui. Engr8 haper 8, Nilon

More information

CHAPTER 7: SECOND-ORDER CIRCUITS

CHAPTER 7: SECOND-ORDER CIRCUITS EEE5: CI RCUI T THEORY CHAPTER 7: SECOND-ORDER CIRCUITS 7. Inroducion Thi chaper conider circui wih wo orage elemen. Known a econd-order circui becaue heir repone are decribed by differenial equaion ha

More information

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship

To become more mathematically correct, Circuit equations are Algebraic Differential equations. from KVL, KCL from the constitutive relationship Laplace Tranform (Lin & DeCarlo: Ch 3) ENSC30 Elecric Circui II The Laplace ranform i an inegral ranformaion. I ranform: f ( ) F( ) ime variable complex variable From Euler > Lagrange > Laplace. Hence,

More information

Design of Controller for Robot Position Control

Design of Controller for Robot Position Control eign of Conroller for Robo oiion Conrol Two imporan goal of conrol: 1. Reference inpu racking: The oupu mu follow he reference inpu rajecory a quickly a poible. Se-poin racking: Tracking when he reference

More information

UT Austin, ECE Department VLSI Design 5. CMOS Gate Characteristics

UT Austin, ECE Department VLSI Design 5. CMOS Gate Characteristics La moule: CMOS Tranior heory Thi moule: DC epone Logic Level an Noie Margin Tranien epone Delay Eimaion Tranior ehavior 1) If he wih of a ranior increae, he curren will ) If he lengh of a ranior increae,

More information

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems

Sample Final Exam (finals03) Covering Chapters 1-9 of Fundamentals of Signals & Systems Sample Final Exam Covering Chaper 9 (final04) Sample Final Exam (final03) Covering Chaper 9 of Fundamenal of Signal & Syem Problem (0 mar) Conider he caual opamp circui iniially a re depiced below. I LI

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 31 Signal & Syem Prof. Mark Fowler Noe Se #27 C-T Syem: Laplace Tranform Power Tool for yem analyi Reading Aignmen: Secion 6.1 6.3 of Kamen and Heck 1/18 Coure Flow Diagram The arrow here how concepual

More information

6.8 Laplace Transform: General Formulas

6.8 Laplace Transform: General Formulas 48 HAP. 6 Laplace Tranform 6.8 Laplace Tranform: General Formula Formula Name, ommen Sec. F() l{ f ()} e f () d f () l {F()} Definiion of Tranform Invere Tranform 6. l{af () bg()} al{f ()} bl{g()} Lineariy

More information

Chapter 9 - The Laplace Transform

Chapter 9 - The Laplace Transform Chaper 9 - The Laplace Tranform Selece Soluion. Skech he pole-zero plo an region of convergence (if i exi) for hee ignal. ω [] () 8 (a) x e u = 8 ROC σ ( ) 3 (b) x e co π u ω [] ( ) () (c) x e u e u ROC

More information

EE202 Circuit Theory II

EE202 Circuit Theory II EE202 Circui Theory II 2017-2018, Spring Dr. Yılmaz KALKAN I. Inroducion & eview of Fir Order Circui (Chaper 7 of Nilon - 3 Hr. Inroducion, C and L Circui, Naural and Sep epone of Serie and Parallel L/C

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms Chaper 6. Laplace Tranform Kreyzig by YHLee;45; 6- An ODE i reduced o an algebraic problem by operaional calculu. The equaion i olved by algebraic manipulaion. The reul i ranformed back for he oluion of

More information

Single Phase Line Frequency Uncontrolled Rectifiers

Single Phase Line Frequency Uncontrolled Rectifiers Single Phae Line Frequency Unconrolle Recifier Kevin Gaughan 24-Nov-03 Single Phae Unconrolle Recifier 1 Topic Baic operaion an Waveform (nucive Loa) Power Facor Calculaion Supply curren Harmonic an Th

More information

18.03SC Unit 3 Practice Exam and Solutions

18.03SC Unit 3 Practice Exam and Solutions Sudy Guide on Sep, Dela, Convoluion, Laplace You can hink of he ep funcion u() a any nice mooh funcion which i for < a and for > a, where a i a poiive number which i much maller han any ime cale we care

More information

Chapter 6. Laplace Transforms

Chapter 6. Laplace Transforms 6- Chaper 6. Laplace Tranform 6.4 Shor Impule. Dirac Dela Funcion. Parial Fracion 6.5 Convoluion. Inegral Equaion 6.6 Differeniaion and Inegraion of Tranform 6.7 Syem of ODE 6.4 Shor Impule. Dirac Dela

More information

Chapter 7 Response of First-order RL and RC Circuits

Chapter 7 Response of First-order RL and RC Circuits Chaper 7 Response of Firs-order RL and RC Circuis 7.- The Naural Response of RL and RC Circuis 7.3 The Sep Response of RL and RC Circuis 7.4 A General Soluion for Sep and Naural Responses 7.5 Sequenial

More information

Lecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits

Lecture 13 RC/RL Circuits, Time Dependent Op Amp Circuits Lecure 13 RC/RL Circuis, Time Dependen Op Amp Circuis RL Circuis The seps involved in solving simple circuis conaining dc sources, resisances, and one energy-sorage elemen (inducance or capaciance) are:

More information

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2)

Laplace Transform. Inverse Laplace Transform. e st f(t)dt. (2) Laplace Tranform Maoud Malek The Laplace ranform i an inegral ranform named in honor of mahemaician and aronomer Pierre-Simon Laplace, who ued he ranform in hi work on probabiliy heory. I i a powerful

More information

s-domain Circuit Analysis

s-domain Circuit Analysis Domain ircui Analyi Operae direcly in he domain wih capacior, inducor and reior Key feaure lineariy i preerved c decribed by ODE and heir I Order equal number of plu number of Elemenbyelemen and ource

More information

8. Basic RL and RC Circuits

8. Basic RL and RC Circuits 8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 1 Circui Analysis Lesson 35 Chaper 8: Second Order Circuis Daniel M. Liynski, Ph.D. ECE 1 Circui Analysis Lesson 3-34 Chaper 7: Firs Order Circuis (Naural response RC & RL circuis, Singulariy funcions,

More information

Chapter Three Systems of Linear Differential Equations

Chapter Three Systems of Linear Differential Equations Chaper Three Sysems of Linear Differenial Equaions In his chaper we are going o consier sysems of firs orer orinary ifferenial equaions. These are sysems of he form x a x a x a n x n x a x a x a n x n

More information

ES 250 Practice Final Exam

ES 250 Practice Final Exam ES 50 Pracice Final Exam. Given ha v 8 V, a Deermine he values of v o : 0 Ω, v o. V 0 Firs, v o 8. V 0 + 0 Nex, 8 40 40 0 40 0 400 400 ib i 0 40 + 40 + 40 40 40 + + ( ) 480 + 5 + 40 + 8 400 400( 0) 000

More information

( ) = Q 0. ( ) R = R dq. ( t) = I t

( ) = Q 0. ( ) R = R dq. ( t) = I t ircuis onceps The addiion of a simple capacior o a circui of resisors allows wo relaed phenomena o occur The observaion ha he ime-dependence of a complex waveform is alered by he circui is referred o as

More information

8.022 (E&M) Lecture 16

8.022 (E&M) Lecture 16 8. (E&M) ecure 16 Topics: Inducors in circuis circuis circuis circuis as ime Our second lecure on elecromagneic inducance 3 ways of creaing emf using Faraday s law: hange area of circui S() hange angle

More information

EEEB113 CIRCUIT ANALYSIS I

EEEB113 CIRCUIT ANALYSIS I 9/14/29 1 EEEB113 CICUIT ANALYSIS I Chaper 7 Firs-Order Circuis Maerials from Fundamenals of Elecric Circuis 4e, Alexander Sadiku, McGraw-Hill Companies, Inc. 2 Firs-Order Circuis -Chaper 7 7.2 The Source-Free

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

EE100 Lab 3 Experiment Guide: RC Circuits

EE100 Lab 3 Experiment Guide: RC Circuits I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical

More information

CONTROL SYSTEMS. Chapter 3 Mathematical Modelling of Physical Systems-Laplace Transforms. Prof.Dr. Fatih Mehmet Botsalı

CONTROL SYSTEMS. Chapter 3 Mathematical Modelling of Physical Systems-Laplace Transforms. Prof.Dr. Fatih Mehmet Botsalı CONTROL SYSTEMS Chaper Mahemaical Modelling of Phyical Syem-Laplace Tranform Prof.Dr. Faih Mehme Boalı Definiion Tranform -- a mahemaical converion from one way of hinking o anoher o make a problem eaier

More information

Chapter 7: Inverse-Response Systems

Chapter 7: Inverse-Response Systems Chaper 7: Invere-Repone Syem Normal Syem Invere-Repone Syem Baic Sar ou in he wrong direcion End up in he original eady-ae gain value Two or more yem wih differen magniude and cale in parallel Main yem

More information

INDEX. Transient analysis 1 Initial Conditions 1

INDEX. Transient analysis 1 Initial Conditions 1 INDEX Secion Page Transien analysis 1 Iniial Condiions 1 Please inform me of your opinion of he relaive emphasis of he review maerial by simply making commens on his page and sending i o me a: Frank Mera

More information

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4. PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence

More information

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response

Voltage/current relationship Stored Energy. RL / RC circuits Steady State / Transient response Natural / Step response Review Capaciors/Inducors Volage/curren relaionship Sored Energy s Order Circuis RL / RC circuis Seady Sae / Transien response Naural / Sep response EE4 Summer 5: Lecure 5 Insrucor: Ocavian Florescu Lecure

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

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5

Mon Apr 2: Laplace transform and initial value problems like we studied in Chapter 5 Mah 225-4 Week 2 April 2-6 coninue.-.3; alo cover par of.4-.5, EP 7.6 Mon Apr 2:.-.3 Laplace ranform and iniial value problem like we udied in Chaper 5 Announcemen: Warm-up Exercie: Recall, The Laplace

More information

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients Secion 3.5 Nonhomogeneous Equaions; Mehod of Undeermined Coefficiens Key Terms/Ideas: Linear Differenial operaor Nonlinear operaor Second order homogeneous DE Second order nonhomogeneous DE Soluion o homogeneous

More information

13.1 Circuit Elements in the s Domain Circuit Analysis in the s Domain The Transfer Function and Natural Response 13.

13.1 Circuit Elements in the s Domain Circuit Analysis in the s Domain The Transfer Function and Natural Response 13. Chaper 3 The Laplace Tranform in Circui Analyi 3. Circui Elemen in he Domain 3.-3 Circui Analyi in he Domain 3.4-5 The Tranfer Funcion and Naural Repone 3.6 The Tranfer Funcion and he Convoluion Inegral

More information

CONTROL SYSTEMS. Chapter 10 : State Space Response

CONTROL SYSTEMS. Chapter 10 : State Space Response CONTROL SYSTEMS Chaper : Sae Space Repone GATE Objecive & Numerical Type Soluion Queion 5 [GATE EE 99 IIT-Bombay : Mark] Conider a econd order yem whoe ae pace repreenaion i of he form A Bu. If () (),

More information

Study of simple inductive-capacitive series circuits using MATLAB software package

Study of simple inductive-capacitive series circuits using MATLAB software package ecen Advance in ircui, Syem and Auomaic onrol Sudy of imple inducive-capaciive erie circui uing MAAB ofware package NIUESU IU, PĂSUESU DAGOŞ Faculy of Mechanical and Elecrical Engineering Univeriy of Peroani

More information

u(t) Figure 1. Open loop control system

u(t) Figure 1. Open loop control system Open loop conrol v cloed loop feedbac conrol The nex wo figure preen he rucure of open loop and feedbac conrol yem Figure how an open loop conrol yem whoe funcion i o caue he oupu y o follow he reference

More information

First Order RC and RL Transient Circuits

First Order RC and RL Transient Circuits Firs Order R and RL Transien ircuis Objecives To inroduce he ransiens phenomena. To analyze sep and naural responses of firs order R circuis. To analyze sep and naural responses of firs order RL circuis.

More information

6 December 2013 H. T. Hoang - www4.hcmut.edu.vn/~hthoang/ 1

6 December 2013 H. T. Hoang - www4.hcmut.edu.vn/~hthoang/ 1 Lecure Noe Fundamenal of Conrol Syem Inrucor: Aoc. Prof. Dr. Huynh Thai Hoang Deparmen of Auomaic Conrol Faculy of Elecrical & Elecronic Engineering Ho Chi Minh Ciy Univeriy of Technology Email: hhoang@hcmu.edu.vn

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

More information

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit

Electrical Circuits. 1. Circuit Laws. Tools Used in Lab 13 Series Circuits Damped Vibrations: Energy Van der Pol Circuit V() R L C 513 Elecrical Circuis Tools Used in Lab 13 Series Circuis Damped Vibraions: Energy Van der Pol Circui A series circui wih an inducor, resisor, and capacior can be represened by Lq + Rq + 1, a

More information

CHAPTER 12 DIRECT CURRENT CIRCUITS

CHAPTER 12 DIRECT CURRENT CIRCUITS CHAPTER 12 DIRECT CURRENT CIUITS DIRECT CURRENT CIUITS 257 12.1 RESISTORS IN SERIES AND IN PARALLEL When wo resisors are conneced ogeher as shown in Figure 12.1 we said ha hey are conneced in series. As

More information

CHAPTER 6: FIRST-ORDER CIRCUITS

CHAPTER 6: FIRST-ORDER CIRCUITS EEE5: CI CUI T THEOY CHAPTE 6: FIST-ODE CICUITS 6. Inroducion This chaper considers L and C circuis. Applying he Kirshoff s law o C and L circuis produces differenial equaions. The differenial equaions

More information

EE202 Circuit Theory II , Spring. Dr. Yılmaz KALKAN & Dr. Atilla DÖNÜK

EE202 Circuit Theory II , Spring. Dr. Yılmaz KALKAN & Dr. Atilla DÖNÜK EE202 Circui Theory II 2018 2019, Spring Dr. Yılmaz KALKAN & Dr. Ailla DÖNÜK 1. Basic Conceps (Chaper 1 of Nilsson - 3 Hrs.) Inroducion, Curren and Volage, Power and Energy 2. Basic Laws (Chaper 2&3 of

More information

Physics 1402: Lecture 22 Today s Agenda

Physics 1402: Lecture 22 Today s Agenda Physics 142: ecure 22 Today s Agenda Announcemens: R - RV - R circuis Homework 6: due nex Wednesday Inducion / A curren Inducion Self-Inducance, R ircuis X X X X X X X X X long solenoid Energy and energy

More information

Direct Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1

Direct Current Circuits. February 19, 2014 Physics for Scientists & Engineers 2, Chapter 26 1 Direc Curren Circuis February 19, 2014 Physics for Scieniss & Engineers 2, Chaper 26 1 Ammeers and Volmeers! A device used o measure curren is called an ammeer! A device used o measure poenial difference

More information

Switching Characteristics of Power Devices

Switching Characteristics of Power Devices Swiching Characeriic of Power Device Device uilizaion can be grealy improved by underanding he device wiching charcaeriic. he main performance wiching characeriic of power device: he ave operaing area

More information

Exponential Sawtooth

Exponential Sawtooth ECPE 36 HOMEWORK 3: PROPERTIES OF THE FOURIER TRANSFORM SOLUTION. Exponenial Sawooh: The eaie way o do hi problem i o look a he Fourier ranform of a ingle exponenial funcion, () = exp( )u(). From he able

More information

CHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition.

CHAPTER. Forced Equations and Systems { } ( ) ( ) 8.1 The Laplace Transform and Its Inverse. Transforms from the Definition. CHAPTER 8 Forced Equaion and Syem 8 The aplace Tranform and I Invere Tranform from he Definiion 5 5 = b b {} 5 = 5e d = lim5 e = ( ) b {} = e d = lim e + e d b = (inegraion by par) = = = = b b ( ) ( )

More information

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C :

dv 7. Voltage-current relationship can be obtained by integrating both sides of i = C : EECE202 NETWORK ANALYSIS I Dr. Charles J. Kim Class Noe 22: Capaciors, Inducors, and Op Amp Circuis A. Capaciors. A capacior is a passive elemen designed o sored energy in is elecric field. 2. A capacior

More information

6.01: Introduction to EECS I Lecture 8 March 29, 2011

6.01: Introduction to EECS I Lecture 8 March 29, 2011 6.01: Inroducion o EES I Lecure 8 March 29, 2011 6.01: Inroducion o EES I Op-Amps Las Time: The ircui Absracion ircuis represen sysems as connecions of elemens hrough which currens (hrough variables) flow

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out.

Chapter 2 The Derivative Applied Calculus 107. We ll need a rule for finding the derivative of a product so we don t have to multiply everything out. Chaper The Derivaive Applie Calculus 107 Secion 4: Prouc an Quoien Rules The basic rules will le us ackle simple funcions. Bu wha happens if we nee he erivaive of a combinaion of hese funcions? Eample

More information

t )? How would you have tried to solve this problem in Chapter 3?

t )? How would you have tried to solve this problem in Chapter 3? Exercie 9) Ue Laplace ranform o wrie down he oluion o 2 x x = F in x = x x = v. wha phenomena do oluion o hi DE illurae (even hough we're forcing wih in co )? How would you have ried o olve hi problem

More information

ECE 2100 Circuit Analysis

ECE 2100 Circuit Analysis ECE 1 Circui Analysis Lesson 37 Chaper 8: Second Order Circuis Discuss Exam Daniel M. Liynski, Ph.D. Exam CH 1-4: On Exam 1; Basis for work CH 5: Operaional Amplifiers CH 6: Capaciors and Inducor CH 7-8:

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 The Complee Response of RL and RC Circuis Seoul Naional Universiy Deparmen of Elecrical and Compuer Engineering Wha is Firs Order Circuis? Circuis ha conain only one inducor or only one capacior

More information

Chapter 8: Response of Linear Systems to Random Inputs

Chapter 8: Response of Linear Systems to Random Inputs Caper 8: epone of Linear yem o anom Inpu 8- Inroucion 8- nalyi in e ime Domain 8- Mean an Variance Value of yem Oupu 8-4 uocorrelaion Funcion of yem Oupu 8-5 Crocorrelaion beeen Inpu an Oupu 8-6 ample

More information

6.302 Feedback Systems Recitation : Phase-locked Loops Prof. Joel L. Dawson

6.302 Feedback Systems Recitation : Phase-locked Loops Prof. Joel L. Dawson 6.32 Feedback Syem Phae-locked loop are a foundaional building block for analog circui deign, paricularly for communicaion circui. They provide a good example yem for hi cla becaue hey are an excellen

More information

1 CHAPTER 14 LAPLACE TRANSFORMS

1 CHAPTER 14 LAPLACE TRANSFORMS CHAPTER 4 LAPLACE TRANSFORMS 4 nroducion f x) i a funcion of x, where x lie in he range o, hen he funcion p), defined by p) px e x) dx, 4 i called he Laplace ranform of x) However, in hi chaper, where

More information

AC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers

AC Circuits AC Circuit with only R AC circuit with only L AC circuit with only C AC circuit with LRC phasors Resonance Transformers A ircuis A ircui wih only A circui wih only A circui wih only A circui wih phasors esonance Transformers Phys 435: hap 31, Pg 1 A ircuis New Topic Phys : hap. 6, Pg Physics Moivaion as ime we discovered

More information

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3. Mah Rahman Exam Review Soluions () Consider he IVP: ( 4)y 3y + 4y = ; y(3) = 0, y (3) =. (a) Please deermine he longes inerval for which he IVP is guaraneed o have a unique soluion. Soluion: The disconinuiies

More information

EECE 301 Signals & Systems Prof. Mark Fowler

EECE 301 Signals & Systems Prof. Mark Fowler EECE 30 Signal & Syem Prof. ark Fowler oe Se #34 C-T Tranfer Funcion and Frequency Repone /4 Finding he Tranfer Funcion from Differenial Eq. Recall: we found a DT yem Tranfer Funcion Hz y aking he ZT of

More information

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max

, the. L and the L. x x. max. i n. It is easy to show that these two norms satisfy the following relation: x x n x = (17.3) max ecure 8 7. Sabiliy Analyi For an n dimenional vecor R n, he and he vecor norm are defined a: = T = i n i (7.) I i eay o how ha hee wo norm aify he following relaion: n (7.) If a vecor i ime-dependen, hen

More information

Discussion Session 2 Constant Acceleration/Relative Motion Week 03

Discussion Session 2 Constant Acceleration/Relative Motion Week 03 PHYS 100 Dicuion Seion Conan Acceleraion/Relaive Moion Week 03 The Plan Today you will work wih your group explore he idea of reference frame (i.e. relaive moion) and moion wih conan acceleraion. You ll

More information

Chapter 28 - Circuits

Chapter 28 - Circuits Physics 4B Lecure Noes Chaper 28 - Circuis Problem Se #7 - due: Ch 28 -, 9, 4, 7, 23, 38, 47, 53, 57, 66, 70, 75 Lecure Ouline. Kirchoff's ules 2. esisors in Series 3. esisors in Parallel 4. More Complex

More information

Some Basic Information about M-S-D Systems

Some Basic Information about M-S-D Systems Some Basic Informaion abou M-S-D Sysems 1 Inroducion We wan o give some summary of he facs concerning unforced (homogeneous) and forced (non-homogeneous) models for linear oscillaors governed by second-order,

More information

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder#

R.#W.#Erickson# Department#of#Electrical,#Computer,#and#Energy#Engineering# University#of#Colorado,#Boulder# .#W.#Erickson# Deparmen#of#Elecrical,#Compuer,#and#Energy#Engineering# Universiy#of#Colorado,#Boulder# Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance,

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

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

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

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

More information

More on ODEs by Laplace Transforms October 30, 2017

More on ODEs by Laplace Transforms October 30, 2017 More on OE b Laplace Tranfor Ocober, 7 More on Ordinar ifferenial Equaion wih Laplace Tranfor Larr areo Mechanical Engineering 5 Seinar in Engineering nali Ocober, 7 Ouline Review la cla efiniion of Laplace

More information

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5

Homework-8(1) P8.3-1, 3, 8, 10, 17, 21, 24, 28,29 P8.4-1, 2, 5 Homework-8() P8.3-, 3, 8, 0, 7, 2, 24, 28,29 P8.4-, 2, 5 Secion 8.3: The Response of a Firs Order Circui o a Consan Inpu P 8.3- The circui shown in Figure P 8.3- is a seady sae before he swich closes a

More information

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff

Laplace transfom: t-translation rule , Haynes Miller and Jeremy Orloff Laplace ransfom: -ranslaion rule 8.03, Haynes Miller and Jeremy Orloff Inroducory example Consider he sysem ẋ + 3x = f(, where f is he inpu and x he response. We know is uni impulse response is 0 for

More information

A Theoretical Model of a Voltage Controlled Oscillator

A Theoretical Model of a Voltage Controlled Oscillator A Theoreical Model of a Volage Conrolled Ocillaor Yenming Chen Advior: Dr. Rober Scholz Communicaion Science Iniue Univeriy of Souhern California UWB Workhop, April 11-1, 6 Inroducion Moivaion The volage

More information

LAPLACE TRANSFORM AND TRANSFER FUNCTION

LAPLACE TRANSFORM AND TRANSFER FUNCTION CHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION Professor Dae Ryook Yang Spring 2018 Dep. of Chemical and Biological Engineering 5-1 Road Map of he Lecure V Laplace Transform and Transfer funcions

More information

Homework 2 Solutions

Homework 2 Solutions Mah 308 Differenial Equaions Fall 2002 & 2. See he las page. Hoework 2 Soluions 3a). Newon s secon law of oion says ha a = F, an we know a =, so we have = F. One par of he force is graviy, g. However,

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

2.9 Modeling: Electric Circuits

2.9 Modeling: Electric Circuits SE. 2.9 Modeling: Elecric ircuis 93 2.9 Modeling: Elecric ircuis Designing good models is a ask he compuer canno do. Hence seing up models has become an imporan ask in modern applied mahemaics. The bes

More information

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution:

(b) (a) (d) (c) (e) Figure 10-N1. (f) Solution: Example: The inpu o each of he circuis shown in Figure 10-N1 is he volage source volage. The oupu of each circui is he curren i( ). Deermine he oupu of each of he circuis. (a) (b) (c) (d) (e) Figure 10-N1

More information

6.2 Transforms of Derivatives and Integrals.

6.2 Transforms of Derivatives and Integrals. SEC. 6.2 Transforms of Derivaives and Inegrals. ODEs 2 3 33 39 23. Change of scale. If l( f ()) F(s) and c is any 33 45 APPLICATION OF s-shifting posiive consan, show ha l( f (c)) F(s>c)>c (Hin: In Probs.

More information

The Fundamental Theorems of Calculus

The Fundamental Theorems of Calculus FunamenalTheorems.nb 1 The Funamenal Theorems of Calculus You have now been inrouce o he wo main branches of calculus: ifferenial calculus (which we inrouce wih he angen line problem) an inegral calculus

More information

5.1 - Logarithms and Their Properties

5.1 - Logarithms and Their Properties Chaper 5 Logarihmic Funcions 5.1 - Logarihms and Their Properies Suppose ha a populaion grows according o he formula P 10, where P is he colony size a ime, in hours. When will he populaion be 2500? We

More information

Physical Limitations of Logic Gates Week 10a

Physical Limitations of Logic Gates Week 10a Physical Limiaions of Logic Gaes Week 10a In a compuer we ll have circuis of logic gaes o perform specific funcions Compuer Daapah: Boolean algebraic funcions using binary variables Symbolic represenaion

More information

Signal and System (Chapter 3. Continuous-Time Systems)

Signal and System (Chapter 3. Continuous-Time Systems) Signal and Sysem (Chaper 3. Coninuous-Time Sysems) Prof. Kwang-Chun Ho kwangho@hansung.ac.kr Tel: 0-760-453 Fax:0-760-4435 1 Dep. Elecronics and Informaion Eng. 1 Nodes, Branches, Loops A nework wih b

More information

Let. x y. denote a bivariate time series with zero mean.

Let. x y. denote a bivariate time series with zero mean. Linear Filer Le x y : T denoe a bivariae ime erie wih zero mean. Suppoe ha he ime erie {y : T} i conruced a follow: y a x The ime erie {y : T} i aid o be conruced from {x : T} by mean of a Linear Filer.

More information

( ) ( ) ( ) () () Signals And Systems Exam#1. 1. Given x(t) and y(t) below: x(t) y(t) (A) Give the expression of x(t) in terms of step functions.

( ) ( ) ( ) () () Signals And Systems Exam#1. 1. Given x(t) and y(t) below: x(t) y(t) (A) Give the expression of x(t) in terms of step functions. Signals And Sysems Exam#. Given x() and y() below: x() y() 4 4 (A) Give he expression of x() in erms of sep funcions. (%) x () = q() q( ) + q( 4) (B) Plo x(.5). (%) x() g() = x( ) h() = g(. 5) = x(. 5)

More information

Section 5: Chain Rule

Section 5: Chain Rule Chaper The Derivaive Applie Calculus 11 Secion 5: Chain Rule There is one more ype of complicae funcion ha we will wan o know how o iffereniae: composiion. The Chain Rule will le us fin he erivaive of

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

Section 3.8, Mechanical and Electrical Vibrations

Section 3.8, Mechanical and Electrical Vibrations Secion 3.8, Mechanical and Elecrical Vibraions Mechanical Unis in he U.S. Cusomary and Meric Sysems Disance Mass Time Force g (Earh) Uni U.S. Cusomary MKS Sysem CGS Sysem fee f slugs seconds sec pounds

More information

Y 0.4Y 0.45Y Y to a proper ARMA specification.

Y 0.4Y 0.45Y Y to a proper ARMA specification. HG Jan 04 ECON 50 Exercises II - 0 Feb 04 (wih answers Exercise. Read secion 8 in lecure noes 3 (LN3 on he common facor problem in ARMA-processes. Consider he following process Y 0.4Y 0.45Y 0.5 ( where

More information

LAB 5: Computer Simulation of RLC Circuit Response using PSpice

LAB 5: Computer Simulation of RLC Circuit Response using PSpice --3LabManualLab5.doc LAB 5: ompuer imulaion of RL ircui Response using Ppice PURPOE To use a compuer simulaion program (Ppice) o invesigae he response of an RL series circui o: (a) a sinusoidal exciaion.

More information

Randomized Perfect Bipartite Matching

Randomized Perfect Bipartite Matching Inenive Algorihm Lecure 24 Randomized Perfec Biparie Maching Lecurer: Daniel A. Spielman April 9, 208 24. Inroducion We explain a randomized algorihm by Ahih Goel, Michael Kapralov and Sanjeev Khanna for

More information

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal? EE 35 Noes Gürdal Arslan CLASS (Secions.-.2) Wha is a signal? In his class, a signal is some funcion of ime and i represens how some physical quaniy changes over some window of ime. Examples: velociy of

More information

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing.

Wall. x(t) f(t) x(t = 0) = x 0, t=0. which describes the motion of the mass in absence of any external forcing. MECHANICS APPLICATIONS OF SECOND-ORDER ODES 7 Mechanics applicaions of second-order ODEs Second-order linear ODEs wih consan coefficiens arise in many physical applicaions. One physical sysems whose behaviour

More information

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p.

Introduction to AC Power, RMS RMS. ECE 2210 AC Power p1. Use RMS in power calculations. AC Power P =? DC Power P =. V I = R =. I 2 R. V p. ECE MS I DC Power P I = Inroducion o AC Power, MS I AC Power P =? A Solp //9, // // correced p4 '4 v( ) = p cos( ω ) v( ) p( ) Couldn' we define an "effecive" volage ha would allow us o use he same relaionships

More information

Non Linear Op Amp Circuits.

Non Linear Op Amp Circuits. Non Linear Op Amp ircuis. omparaors wih 0 and non zero reference volage. omparaors wih hyseresis. The Schmid Trigger. Window comparaors. The inegraor. Waveform conversion. Sine o ecangular. ecangular o

More information