Chapter 6 Electrical Systems and Electromechanical Systems
|
|
- Merryl Hubbard
- 6 years ago
- Views:
Transcription
1 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Chapter 6 Electrcal Systems and Electromechancal Systems 6. INTODUCTION A. Bazoune The majorty of engneerng systems now have at least one electrcal subsystem. Ths may be a power supply, sensor, motor, controller, or an acoustc devce such as a speaker. So an understandng of electrcal systems s essental to understandng the behavor of many systems. 6. ELECTICAL ELEMENTS Current and Voltage Current and voltage are the prmary varables used to descrbe a crcut s behavor. Current s the flow of electrons. It s the tme rate of change of electrons passng through a defned area, such as the cross-secton of a wre. Because electrons are negatvely charged, the postve drecton of current flow s opposte to that of electron flow. The mathematcal descrpton of the relatonshp between the number of electrons ( called charge q ) and current s dq dt = or q( t) = d t The unt of charge s the coulomb (C) and the unt of current s ampere (A), whch s one coulomb per second. Energy s requred to move a charge between two ponts n a crcut. The work per unt charge requred to do ths s called voltage. The unt of voltage s volt (V), whch s defned to be joule per coulomb. The voltage dfference between two ponts n a crcut s a measure of the energy requred to move charge from one pont to the other. Actve and Passve Elements. actve or passve. Crcut elements may be classfed as Passve Element: an element that contans no energy sources (.e. the element needs power from another source to operate); these nclude resstors, capactors and nductors Actve Element: an element that acts as an energy source; these nclude batteres, generators, solar cells, and op-amps. /0
2 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Current Source and Voltage Source A voltage source s a devce that causes a specfed voltage to exst between two ponts n a crcut. The voltage may be tme varyng or tme nvarant (for a suffcently long tme). Fgure 6-(a) s a schematc dagram of a voltage source. Fgure 6-(b) shows a voltage source that has a constant value for an ndefnte tme. Often the voltage s denoted by E or V. A battery s an example of ths type of voltage. A current source causes a specfed current to flow through a wre contanng ths source. Fgure 6-(c) s a schematc dagram of a current source e ( t ) E ( t ) Fgure 6. (a) Voltage source; (b) constant voltage source; (c) current source esstance elements. The resstance of a lnear resstor s gven by where = e s the voltage across the resstor and s the current through the resstor. The unt of resstance s the ohm ( Ω ), where volt ohm= ampere esstances do not store electrc energy n any form, but nstead dsspate t as heat. eal resstors may not be lnear and may also exhbt some capactance and nductance effects. PACTICAL EXAMPLES: Pctures of varous types of real-world resstors are found below. e e Wrewound esstors Wrewound esstors n Parallel /0
3 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Wrewound esstors n Seres and n Parallel Capactance Elements. Two conductors separated by a nonconductng medum form a capactor, so two metallc plates separated by a very thn delectrc materal form a capactor. The capactance C s a measure of the quantty of charge that can be stored for a gven voltage across the plates. The capactance C of a capactor can thus be gven by q C = e where q s the quantty of charge stored and e c s the voltage across the capactor. The unt of capactance s the farad ( F ), where ampere-second coulomb farad = = volt volt Notce that, snce = dq dt and ec or Therefore, = q C, we have de = C c d t c dec = dt C ec = dt + e C Although a pure capactor stores energy and can release all of t, real capactors exhbt varous losses. These energy losses are ndcated by a power factor, whch s the rato of energy lost per cycle of ac voltage to the energy stored per cycle. Thus, a small-valued power factor s desrable. PACTICAL EXAMPLES: Pctures of varous types of real-world capactors are found below. t 0 c ( 0) C e c 3/0
4 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Inductance Elements. If a crcut les n a tme varyng magnetc feld, an electromotve force s nduced n the crcut. The nductve effects can be classfed as self nductance and mutual nductance. Self nductance, or smply nductance, L s the proportonalty constant between the nduced voltage e L volts and the rate of change of current (or change n current per second) d dt amperes per second; that s, L = d e L dt The unt of nductance s the henry (H). An electrcal crcut has an nductance of henry when a rate of change of ampere per second wll nduce an emf of volt: volt weber henry = = ampere second ampere L e L The voltage e L across the nductor L s gven by d el = L d t Where L s the current through the nductor. The current ( ) t e t t ( ) = d + ( 0) L L L L 0 L L t can thus be gven by Because most nductors are cols of wre, they have consderable resstance. The energy loss due to the presence of resstance s ndcated by the qualty factor Q, whch denotes the rato of stored dsspated energy. A hgh value of Q generally means the nductor contans small resstance. Mutual Inductance refers to the nfluence between nductors that results from nteracton of ther felds. PACTICAL EXAMPLES: Pctured below are several real-world examples of nductors. 4/0
5 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems TABLE 6-. Summary of elements nvolved n lnear electrcal systems Element Voltage-current Current-voltage Voltage-charge Impedance, Z(s)=V(s)/I(s) Capactor t v( t) = ( τ ) dτ c 0 dv( t) ( t) = C v ( t) = q( t) dt c Cs esstor v ( t) = ( t) ( t) = v( t) dq( t) v( t) = dt Inductor t d( t) v( t) = L ( t) = dt v( τ ) dτ L 0 d q( t) v( t) = L Ls dt The followng set of symbols and unts are used: v(t) = V (Volts), (t) = A (Amps), q(t) = Q (Coulombs), C = F (Farads), = Ω (Ohms), L = H (Henres). 6.3 FUNDAMENTALS OF ELECTICAL CICUITS Ohm s Law. Ohm s law states that the current n crcut s proportonal to the total electromotve force (emf) actng n the crcut and nversely proportonal to the total resstance of the crcut. That s e = were s the current (amperes), e s the emf (volts), and s the resstance (ohms). Seres Crcut. The combned resstance of seres-connected resstors s the sum of the separate resstances. Fgure 6- shows a smple seres crcut. The voltage between ponts A and B s where e = e + e + e3 e =, e =, e = 3 3 5/0
6 ME 43 Systems Dynamcs & Control Thus, e = + + Chapter 6: Electrcal Systems and Electromechancal Systems 3 The combned resstance s gven by = In general, n = = 3 A e e e e 3 B Fgure 6- Seres Crcut Parallel Crcut. For the parallel crcut shown n fgure 6-3, 3 e 3 Snce = + + 3, t follows that] Fgure 6-3 Parallel Crcut e e e =, =, = 3 3 e e e e = + + = 3 where s the combned resstance. Hence, or = /0
7 ME 43 Systems Dynamcs & Control In general 3 = = n = = Chapter 6: Electrcal Systems and Electromechancal Systems 3 3 Krchhoff s Current Law (KCL) (Node Law). A node n an electrcal crcut s a pont where three or more wres are joned together. Krchhoff s Current Law (KCL) states that or The algebrac sum of all currents enterng and leavng a node s zero. The algebrac sum of all currents enterng a node s equal to the sum of all currents leavng the same node Fgure 6-4 Node. As appled to Fgure 6-4, krchhoff s current law states that or = = Enterng currents Leavng currents Krchhoff s Voltage Law (KVL) (Loop Law). Law (KVL) states that at any gven nstant of tme Krchhoff s Voltage or The algebrac sum of the voltages around any loop n an electrcal crcut s zero. The sum of the voltage drops s equal to the sum of the voltage rses around a loop. 7/0
8 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Fgure 6-5 Dagrams showng voltage rses and voltage drops n crcuts. (Note: Each crcular arrows shows the drecton one follows n analyzng the respectve crcut) A rse n voltage [whch occurs n gong through a source of electromotve force from the negatve termnal to the postve termnal, as shown n Fgure 6-5 (a), or n gong through a resstance n opposton to the current flow, as shown n Fgure 6-5 (b)] should be preceded by a plus sgn. A drop n voltage [whch occurs n gong through a source of electromotve force from the postve to the negatve termnal, as shown n Fgure 6-5 (c), or n gong through a resstance n the drecton of the current flow, as shown n Fgure 6-5 (d)] should be preceded by a mnus sgn. Fgure 6-6 shows a crcut that conssts of a battery and an external resstance. E B r A Fgure 6-6 C Electrcal Crcut. Here E s the electromotve force, r s the nternal resstance of the battery, s the external resstance and s the current. Followng the loop n the clockwse drecton( A B C D ), we have e + e + e = 0 or From whch t follows that AB BC CA E r = E = + r 0 8/0
9 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 6.4 MATHEMATICAL MODELING OF ELECTICAL SYSTEMS 9/0
10 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 0/0
11 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems /0
12 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems /0
13 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Transfer Functons of Cascade Elements. Consder the system shown n Fgure 6.8. Assume e s the nput and e o s the output. The capactances C and E s E s. C are not charged ntally. Let us fnd transfer functon o ( ) ( ) e C C eo Fgure 6-8 Electrcal system The equatons of ths system are: Loop + ( ) dt = e (6-7) C 3/0
14 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems Loop ( ) dt + + dt = 0 (6-8) C C Outer Loop dt = e o (6-9) C Takng LT of the above equatons, assumng zero I. C s, we obtan I ( s) + I ( s) I ( s) = E ( s) Cs (6-0) I ( s) I ( s) I ( s) I ( s) 0 Cs + + = (6-) Cs I ( s) = Eo ( s) (6-) Cs From Equaton (6-0) I ( s) + I ( s) I ( s) = E ( s) C s C s I ( s) Substtute I ( s ) nto Equaton (6-) E E s I s C s ( ) + ( ) ( ) + ( ) = = C s + C s + C s C se s I s ( s) = ( ) ( ) E s C C s + C + C + C s + o = s C C ( C + C + C ) + s + C C C C whch represents a transfer functon of a second order system. The characterstc polynomal (denomnator) of the above transfer functon can be compared to that of a second order system s + ζω s + ω. Therefore, one can wrte n n ωn = and ζω = C C or ( ) ω ( C C ) ( C + C + C ) n C C ( ) C + C + C C + C + C ζ = = C C n Complex Impedance. In dervng transfer functons for electrcal crcuts, we frequently fnd t convenent to wrte the Laplace-transformed equatons drectly, wthout wrtng the dfferental equatons. Table 6- gves the complex mpedance of the bascs passve elements such as resstance, an nductance L, and a capactance C. Fgure 6-9 shows the complex mpedances Z and Z n a seres crcut whle Fgure 6-9 shows the transfer functon 4/0
15 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems between the output and nput voltage. emember that the mpedance s vald only f the ntal condtons nvolved are all zeros. The general relatonshp s E( s) = Z( s) I s corresponds to Ohm s law for purely resstve crcuts. (Notce that, lke resstances, mpedances can be combned n seres and n parallel) ( ) Fgure 6-9 Z Z e e e E( s) Z = Z + Z = I ( s) Electrcal crcut Dervng Transfer Functons of Electrcal Crcuts Usng Complex Impedances. The TF of an electrcal crcut can be obtaned as a rato of complex mpedances. For the crcut shown n Fgure 6-0, assume that the voltages e and e o are the nput and output of the crcut, respectvely. Then the TF of ths crcut can be obtaned as Z ( s) I ( s) ( ) ( ) E ( ) Z ο s Z( s) = = E ( s) Z ( s) I s + Z ( s) I s Z ( s) + Z ( s) e (nput) Z e o (output) For the crcut shown n Fgure 6-, Fgure 6-0 Electrcal crcut Z = Ls +, Z = Cs Eο ( s) Hence, the transfer functon, s E ( s) ( ) ( ) Eο s Z s = = Cs = E ( ) s Z( s) + Z( s) LCs + Cs + Ls + + Cs Z L e (nput) Z C e o (output) Fgure 6- Electrcal crcut 5/0
16 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 6.5 ANALOGOUS SYSTEMS Systems that can be represented by the same mathematcal model, but that are physcally dfferent, are called analogous systems. Thus analogous systems are descrbed by the same dfferental or ntegrodfferental equatons or transfer functons. The concept of analogous s useful n practce, for the followng reasons:. The soluton of the equaton descrbng one physcal system can be drectly appled to analogous systems n any other feld.. Snce one type of system may be easer to handle expermentally than another, nstead of buldng and studyng a mechancal system (or a hydraulc system, pneumatc system, or the lke), we can buld and study ts electrcal analog, for electrcal or electronc system, n general, much easer to deal wth expermentally. Mechancal-Electrcal Analoges Mechancal systems can be studed through ther electrcal analogs, whch may be more easly constructed than models of the correspondng mechancal systems. There are two electrcal analoges for mechancal systems: The Force-Voltage Analogy and The Force Current Analogy. Force Voltage Analogy and the electrcal system of Fgure 6-4(b). Consder the mechancal system of Fgure 6-4(a) e L C Fgure 6-4 Analogous mechancal and electrcal systems. The equaton for the mechancal system s d x dx m + b + kx = p (6-4) dt dt where x s the dsplacement of mass m, measured from equlbrum poston. The equaton for the electrcal system s d L + + dt = e dt C In terms of electrcal charge q, ths last equaton becomes 6/0
17 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems d q dq dt dt C L + + q = e (6-5) Comparng equatons (6-4) and (6-5), we see that the dfferental equatons for the two systems are of dentcal form. Thus, these two systems are analogous systems. The terms that occupy correspondng postons n the dfferental equatons are called analogous quanttes, a lst of whch appear n Table 6- TABLE 6- Mechancal Systems Force p (Torque T ) Mass m (Moment of nerta J ) Vscous-frcton coeffcent b Sprng constant k Dsplacement x (angular dsplacement θ ) Velocty ẋ (angular velocty θ ) Force Voltage Analogy Electrcal Systems Voltage e Inductance L esstance ecprocal of capactance, C Charge q Current Force Current Analogy the textbook Page The student s advsed to read ths secton from 6.6 MATHEMATICAL MODELING OF ELCTOMECHANICAL SYSTEMS To control the moton or speed of dc servomotors, we control the feld current or armature current or we use a servodrver as motor-drver combnaton. There are many dfferent types of servodrvers. Most are desgned to control the speed of dc servomotors, whch mproves the effcency of operatng servomotors. Here we shall dscuss only armature control of a dc servomotor and obtan ts mathematcal model n the form of a transfer functon. 7/0
18 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 8/0
19 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 9/0
20 ME 43 Systems Dynamcs & Control Chapter 6: Electrcal Systems and Electromechancal Systems 0/0
Electrical Circuits 2.1 INTRODUCTION CHAPTER
CHAPTE Electrcal Crcuts. INTODUCTION In ths chapter, we brefly revew the three types of basc passve electrcal elements: resstor, nductor and capactor. esstance Elements: Ohm s Law: The voltage drop across
More informationPHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.
!! www.clutchprep.com CONCEPT: ELECTROMAGNETIC INDUCTION A col of wre wth a VOLTAGE across each end wll have a current n t - Wre doesn t HAVE to have voltage source, voltage can be INDUCED V Common ways
More informationPHYSICS - CLUTCH 1E CH 28: INDUCTION AND INDUCTANCE.
!! www.clutchprep.com CONCEPT: ELECTROMAGNETIC INDUCTION A col of wre wth a VOLTAGE across each end wll have a current n t - Wre doesn t HAVE to have voltage source, voltage can be INDUCED V Common ways
More informationSections begin this week. Cancelled Sections: Th Labs begin this week. Attend your only second lab slot this week.
Announcements Sectons begn ths week Cancelled Sectons: Th 122. Labs begn ths week. Attend your only second lab slot ths week. Cancelled labs: ThF 25. Please check your Lab secton. Homework #1 onlne Due
More informationPhysics 4B. A positive value is obtained, so the current is counterclockwise around the circuit.
Physcs 4B Solutons to Chapter 7 HW Chapter 7: Questons:, 8, 0 Problems:,,, 45, 48,,, 7, 9 Queston 7- (a) no (b) yes (c) all te Queston 7-8 0 μc Queston 7-0, c;, a;, d; 4, b Problem 7- (a) Let be the current
More informationPhysics 1202: Lecture 11 Today s Agenda
Physcs 122: Lecture 11 Today s Agenda Announcements: Team problems start ths Thursday Team 1: Hend Ouda, Mke Glnsk, Stephane Auger Team 2: Analese Bruder, Krsten Dean, Alson Smth Offce hours: Monday 2:3-3:3
More informationEnergy Storage Elements: Capacitors and Inductors
CHAPTER 6 Energy Storage Elements: Capactors and Inductors To ths pont n our study of electronc crcuts, tme has not been mportant. The analyss and desgns we hae performed so far hae been statc, and all
More informationDC Circuits. Crossing the emf in this direction +ΔV
DC Crcuts Delverng a steady flow of electrc charge to a crcut requres an emf devce such as a battery, solar cell or electrc generator for example. mf stands for electromotve force, but an emf devce transforms
More informationPhysics 2102 Spring 2007 Lecture 10 Current and Resistance
esstance Is Futle! Physcs 0 Sprng 007 Jonathan Dowlng Physcs 0 Sprng 007 Lecture 0 Current and esstance Georg Smon Ohm (789-854) What are we gong to learn? A road map lectrc charge lectrc force on other
More informationLecture #4 Capacitors and Inductors Energy Stored in C and L Equivalent Circuits Thevenin Norton
EES ntro. electroncs for S Sprng 003 Lecture : 0/03/03 A.R. Neureuther Verson Date 0/0/03 EES ntroducton to Electroncs for omputer Scence Andrew R. Neureuther Lecture # apactors and nductors Energy Stored
More informationIntroduction to circuit analysis. Classification of Materials
Introducton to crcut analyss OUTLINE Electrcal quanttes Charge Current Voltage Power The deal basc crcut element Sgn conventons Current versus voltage (I-V) graph Readng: 1.2, 1.3,1.6 Lecture 2, Slde 1
More informationMAE140 - Linear Circuits - Winter 16 Final, March 16, 2016
ME140 - Lnear rcuts - Wnter 16 Fnal, March 16, 2016 Instructons () The exam s open book. You may use your class notes and textbook. You may use a hand calculator wth no communcaton capabltes. () You have
More informationINDUCTANCE. RC Cicuits vs LR Circuits
INDUTANE R cuts vs LR rcuts R rcut hargng (battery s connected): (1/ )q + (R)dq/ dt LR rcut = (R) + (L)d/ dt q = e -t/ R ) = / R(1 - e -(R/ L)t ) q ncreases from 0 to = dq/ dt decreases from / R to 0 Dschargng
More informationEMF induced in a coil by moving a bar magnet. Induced EMF: Faraday s Law. Induction and Oscillations. Electromagnetic Induction.
Inducton and Oscllatons Ch. 3: Faraday s Law Ch. 3: AC Crcuts Induced EMF: Faraday s Law Tme-dependent B creates nduced E In partcular: A changng magnetc flux creates an emf n a crcut: Ammeter or voltmeter.
More informationModeling of Dynamic Systems
Modelng of Dynamc Systems Ref: Control System Engneerng Norman Nse : Chapters & 3 Chapter objectves : Revew the Laplace transform Learn how to fnd a mathematcal model, called a transfer functon Learn how
More informationE40M Device Models, Resistors, Voltage and Current Sources, Diodes, Solar Cells. M. Horowitz, J. Plummer, R. Howe 1
E40M Devce Models, Resstors, Voltage and Current Sources, Dodes, Solar Cells M. Horowtz, J. Plummer, R. Howe 1 Understandng the Solar Charger Lab Project #1 We need to understand how: 1. Current, voltage
More informationPhysics 114 Exam 2 Spring Name:
Physcs 114 Exam Sprng 013 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red wth the amount beng
More informationAdvanced Circuits Topics - Part 1 by Dr. Colton (Fall 2017)
Advanced rcuts Topcs - Part by Dr. olton (Fall 07) Part : Some thngs you should already know from Physcs 0 and 45 These are all thngs that you should have learned n Physcs 0 and/or 45. Ths secton s organzed
More informationMAE140 - Linear Circuits - Winter 16 Midterm, February 5
Instructons ME140 - Lnear Crcuts - Wnter 16 Mdterm, February 5 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator
More informationTransfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system
Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng
More informationElectricity and Magnetism Lecture 07 - Physics 121 Current, Resistance, DC Circuits: Y&F Chapter 25 Sect. 1-5 Kirchhoff s Laws: Y&F Chapter 26 Sect.
Electrcty and Magnetsm Lecture 07 - Physcs Current, esstance, DC Crcuts: Y&F Chapter 5 Sect. -5 Krchhoff s Laws: Y&F Chapter 6 Sect. Crcuts and Currents Electrc Current Current Densty J Drft Speed esstance,
More informationFE REVIEW OPERATIONAL AMPLIFIERS (OP-AMPS)( ) 8/25/2010
FE REVEW OPERATONAL AMPLFERS (OP-AMPS)( ) 1 The Op-amp 2 An op-amp has two nputs and one output. Note the op-amp below. The termnal labeled l wth the (-) sgn s the nvertng nput and the nput labeled wth
More informationPHY2049 Exam 2 solutions Fall 2016 Solution:
PHY2049 Exam 2 solutons Fall 2016 General strategy: Fnd two resstors, one par at a tme, that are connected ether n SERIES or n PARALLEL; replace these two resstors wth one of an equvalent resstance. Now
More informationBoise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab
Bose State Unersty Department of Electrcal and omputer Engneerng EE 1L rcut Analyss and Desgn Lab Experment #8: The Integratng and Dfferentatng Op-Amp rcuts 1 Objectes The objectes of ths laboratory experment
More informationPhysics Electricity and Magnetism Lecture 12 - Inductance, RL Circuits. Y&F Chapter 30, Sect 1-4
Physcs - lectrcty and Magnetsm ecture - Inductance, Crcuts Y&F Chapter 30, Sect - 4 Inductors and Inductance Self-Inductance Crcuts Current Growth Crcuts Current Decay nergy Stored n a Magnetc Feld nergy
More informationCircuit Variables. Unit: volt (V = J/C)
Crcut Varables Scentfc nestgaton of statc electrcty was done n late 700 s and Coulomb s credted wth most of the dscoeres. He found that electrc charges hae two attrbutes: amount and polarty. There are
More informationPhysics 114 Exam 2 Fall 2014 Solutions. Name:
Physcs 114 Exam Fall 014 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red. Unless otherwse ndcated,
More informationi I (I + i) 3/27/2006 Circuits ( F.Robilliard) 1
4V I 2V (I + ) 0 0 --- 3V 1 2 4Ω 6Ω 3Ω 3/27/2006 Crcuts ( F.obllard) 1 Introducton: Electrcal crcuts are ubqutous n the modern world, and t s dffcult to oerstate ther mportance. They range from smple drect
More informationFundamental loop-current method using virtual voltage sources technique for special cases
Fundamental loop-current method usng vrtual voltage sources technque for specal cases George E. Chatzaraks, 1 Marna D. Tortorel 1 and Anastasos D. Tzolas 1 Electrcal and Electroncs Engneerng Departments,
More informationDesigning Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 3A
EECS 16B Desgnng Informaton Devces and Systems II Sprng 018 J. Roychowdhury and M. Maharbz Dscusson 3A 1 Phasors We consder snusodal voltages and currents of a specfc form: where, Voltage vt) = V 0 cosωt
More informationCoupling Element and Coupled circuits. Coupled inductor Ideal transformer Controlled sources
Couplng Element and Coupled crcuts Coupled nductor Ideal transformer Controlled sources Couplng Element and Coupled crcuts Coupled elements hae more that one branch and branch oltages or branch currents
More informationMAE140 - Linear Circuits - Fall 13 Midterm, October 31
Instructons ME140 - Lnear Crcuts - Fall 13 Mdterm, October 31 () Ths exam s open book. You may use whatever wrtten materals you choose, ncludng your class notes and textbook. You may use a hand calculator
More informationmatter consists, measured in coulombs (C) 1 C of charge requires electrons Law of conservation of charge: charge cannot be created or
Basc Concepts Oerew SI Prefxes Defntons: Current, Voltage, Power, & Energy Passe sgn conenton Crcut elements Ideal s Portland State Unersty ECE 221 Basc Concepts Ver. 1.24 1 Crcut Analyss: Introducton
More informationDepartment of Electrical and Computer Engineering FEEDBACK AMPLIFIERS
Department o Electrcal and Computer Engneerng UNIT I EII FEEDBCK MPLIFIES porton the output sgnal s ed back to the nput o the ampler s called Feedback mpler. Feedback Concept: block dagram o an ampler
More informationPhysics 4B. Question and 3 tie (clockwise), then 2 and 5 tie (zero), then 4 and 6 tie (counterclockwise) B i. ( T / s) = 1.74 V.
Physcs 4 Solutons to Chapter 3 HW Chapter 3: Questons:, 4, 1 Problems:, 15, 19, 7, 33, 41, 45, 54, 65 Queston 3-1 and 3 te (clockwse), then and 5 te (zero), then 4 and 6 te (counterclockwse) Queston 3-4
More informationLinearity. If kx is applied to the element, the output must be ky. kx ky. 2. additivity property. x 1 y 1, x 2 y 2
Lnearty An element s sad to be lnear f t satsfes homogenety (scalng) property and addte (superposton) property. 1. homogenety property Let x be the nput and y be the output of an element. x y If kx s appled
More informationWeek3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity
Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle
More informationTUTORIAL PROBLEMS. E.1 KCL, KVL, Power and Energy. Q.1 Determine the current i in the following circuit. All units in VAΩ,,
196 E TUTORIAL PROBLEMS E.1 KCL, KVL, Power and Energy Q.1 Determne the current n the followng crcut. 3 5 3 8 9 6 5 Appendx E Tutoral Problems 197 Q. Determne the current and the oltage n the followng
More informationIntroduction to Vapor/Liquid Equilibrium, part 2. Raoult s Law:
CE304, Sprng 2004 Lecture 4 Introducton to Vapor/Lqud Equlbrum, part 2 Raoult s Law: The smplest model that allows us do VLE calculatons s obtaned when we assume that the vapor phase s an deal gas, and
More informationBoise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab
Bose State Unersty Department of Electrcal and omputer Engneerng EE 1L rcut Analyss and Desgn Lab Experment #8: The Integratng and Dfferentatng Op-Amp rcuts 1 Objectes The objectes of ths laboratory experment
More informationStudy Guide For Exam Two
Study Gude For Exam Two Physcs 2210 Albretsen Updated: 08/02/2018 All Other Prevous Study Gudes Modules 01-06 Module 07 Work Work done by a constant force F over a dstance s : Work done by varyng force
More informationFormulation of Circuit Equations
ECE 570 Sesson 2 IC 752E Computer Aded Engneerng for Integrated Crcuts Formulaton of Crcut Equatons Bascs of crcut modelng 1. Notaton 2. Crcut elements 3. Krchoff laws 4. ableau formulaton 5. Modfed nodal
More informationEE 2006 Electric Circuit Analysis Spring January 23, 2015 Lecture 02
EE 2006 Electrc Crcut Analyss Sprng 2015 January 23, 2015 Lecture 02 1 Lab 1 Dgtal Multmeter Lab nstructons Aalable onlne Prnt out and read before Lab MWAH 391, 4:00 7:00 pm, next Monday or Wednesday (January
More informationComplex Numbers, Signals, and Circuits
Complex Numbers, Sgnals, and Crcuts 3 August, 009 Complex Numbers: a Revew Suppose we have a complex number z = x jy. To convert to polar form, we need to know the magntude of z and the phase of z. z =
More informationI. INTRODUCTION. 1.1 Circuit Theory Fundamentals
I. INTRODUCTION 1.1 Crcut Theory Fundamentals Crcut theory s an approxmaton to Maxwell s electromagnetc equatons n order to smplfy analyss of complcated crcuts. A crcut s made of seeral elements (boxes
More information6.01: Introduction to EECS 1 Week 6 October 15, 2009
6.0: ntroducton to EECS Week 6 October 5, 2009 6.0: ntroducton to EECS Crcuts The Crcut Abstracton Crcuts represent systems as connectons of component through whch currents (through arables) flow and across
More informationPhysics 5153 Classical Mechanics. Principle of Virtual Work-1
P. Guterrez 1 Introducton Physcs 5153 Classcal Mechancs Prncple of Vrtual Work The frst varatonal prncple we encounter n mechancs s the prncple of vrtual work. It establshes the equlbrum condton of a mechancal
More informationSpin-rotation coupling of the angularly accelerated rigid body
Spn-rotaton couplng of the angularly accelerated rgd body Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 E-mal: louaelzen@gmal.com November 1, 2017 All Rghts Reserved. Abstract Ths paper s
More informationPhysics 181. Particle Systems
Physcs 181 Partcle Systems Overvew In these notes we dscuss the varables approprate to the descrpton of systems of partcles, ther defntons, ther relatons, and ther conservatons laws. We consder a system
More informationFirst Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.
Secton 1. Dynamcs (Newton s Laws of Moton) Two approaches: 1) Gven all the forces actng on a body, predct the subsequent (changes n) moton. 2) Gven the (changes n) moton of a body, nfer what forces act
More informationPhysics 53. Rotational Motion 3. Sir, I have found you an argument, but I am not obliged to find you an understanding.
Physcs 53 Rotatonal Moton 3 Sr, I have found you an argument, but I am not oblged to fnd you an understandng. Samuel Johnson Angular momentum Wth respect to rotatonal moton of a body, moment of nerta plays
More informationPhysics 114 Exam 3 Spring Name:
Physcs 114 Exam 3 Sprng 015 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem 4. Answer each of the followng questons. Ponts for each queston are ndcated n red. Unless otherwse
More informationAnnouncements. Lecture #2
Announcements Lectures wll be n 4 LeConte begnnng Frday 8/29 Addtonal dscusson TA Denns Chang (Sectons 101, 105) Offce hours: Mo 2-3 PM; Th 5-6 PM Lab sectons begn Tuesday 9/2 Read Experment #1 onlne Download
More informationChapter 6. Operational Amplifier. inputs can be defined as the average of the sum of the two signals.
6 Operatonal mpler Chapter 6 Operatonal mpler CC Symbol: nput nput Output EE () Non-nvertng termnal, () nvertng termnal nput mpedance : Few mega (ery hgh), Output mpedance : Less than (ery low) Derental
More informationDO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED.
EE 539 Homeworks Sprng 08 Updated: Tuesday, Aprl 7, 08 DO NOT DO HOMEWORK UNTIL IT IS ASSIGNED. THE ASSIGNMENTS MAY CHANGE UNTIL ANNOUNCED. For full credt, show all work. Some problems requre hand calculatons.
More informationEE 2006 Electric Circuit Analysis Fall September 04, 2014 Lecture 02
EE 2006 Electrc Crcut Analyss Fall 2014 September 04, 2014 Lecture 02 1 For Your Informaton Course Webpage http://www.d.umn.edu/~jngba/electrc_crcut_analyss_(ee_2006).html You can fnd on the webpage: Lecture:
More informationI. INTRODUCTION. There are two other circuit elements that we will use and are special cases of the above elements. They are:
I. INTRODUCTION 1.1 Crcut Theory Fundamentals In ths course we study crcuts wth non-lnear elements or deces (dodes and transstors). We wll use crcut theory tools to analyze these crcuts. Snce some of tools
More informationSpring 2002 Lecture #13
44-50 Sprng 00 ecture # Dr. Jaehoon Yu. Rotatonal Energy. Computaton of oments of nerta. Parallel-as Theorem 4. Torque & Angular Acceleraton 5. Work, Power, & Energy of Rotatonal otons Remember the md-term
More informationDr. Fritz Wilhelm, Physics 230 E:\Excel files\230 lecture\ch26 capacitance.docx 1 of 13 Last saved: 12/27/2008; 8:40 PM. Homework: See website.
Dr. Frtz Wlhelm, Physcs 3 E:\Excel fles\3 lecture\ch6 capactance.docx of 3 Last saved: /7/8; 8:4 PM Homework: See webste. Table of ontents: h.6. Defnton of apactance, 6. alculatng apactance, 6.a Parallel
More informationME2142/ME2142E Feedback Control Systems. Modelling of Physical Systems The Transfer Function
Mdellng Physcal Systems The Transer Functn Derental Equatns U Plant Y In the plant shwn, the nput u aects the respnse the utput y. In general, the dynamcs ths respnse can be descrbed by a derental equatn
More informationStructure and Drive Paul A. Jensen Copyright July 20, 2003
Structure and Drve Paul A. Jensen Copyrght July 20, 2003 A system s made up of several operatons wth flow passng between them. The structure of the system descrbes the flow paths from nputs to outputs.
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationProf. Paolo Colantonio a.a
Pro. Paolo olantono a.a. 3 4 Let s consder a two ports network o Two ports Network o L For passve network (.e. wthout nternal sources or actve devces), a general representaton can be made by a sutable
More informationUnit 1. Current and Voltage U 1 VOLTAGE AND CURRENT. Circuit Basics KVL, KCL, Ohm's Law LED Outputs Buttons/Switch Inputs. Current / Voltage Analogy
..2 nt Crcut Bascs KVL, KCL, Ohm's Law LED Outputs Buttons/Swtch Inputs VOLTAGE AND CRRENT..4 Current and Voltage Current / Voltage Analogy Charge s measured n unts of Coulombs Current Amount of charge
More informationThe Feynman path integral
The Feynman path ntegral Aprl 3, 205 Hesenberg and Schrödnger pctures The Schrödnger wave functon places the tme dependence of a physcal system n the state, ψ, t, where the state s a vector n Hlbert space
More informationPhysics 2A Chapters 6 - Work & Energy Fall 2017
Physcs A Chapters 6 - Work & Energy Fall 017 These notes are eght pages. A quck summary: The work-energy theorem s a combnaton o Chap and Chap 4 equatons. Work s dened as the product o the orce actng on
More information( ) = ( ) + ( 0) ) ( )
EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.
More informationStudy on Active Micro-vibration Isolation System with Linear Motor Actuator. Gong-yu PAN, Wen-yan GU and Dong LI
2017 2nd Internatonal Conference on Electrcal and Electroncs: echnques and Applcatons (EEA 2017) ISBN: 978-1-60595-416-5 Study on Actve Mcro-vbraton Isolaton System wth Lnear Motor Actuator Gong-yu PAN,
More informationTitle Chapters HW Due date. Lab Due date 8 Sept Mon 2 Kirchoff s Laws NO LAB. 9 Sept Tue NO LAB 10 Sept Wed 3 Power
Schedule Date Day Class No. Ttle Chapters HW Due date Lab Due date 8 Sept Mon Krchoff s Laws..3 NO LAB Exam 9 Sept Tue NO LAB 10 Sept Wed 3 Power.4.5 11 Sept Thu NO LAB 1 Sept Fr Rectaton HW 1 13 Sept
More informationFrequency dependence of the permittivity
Frequency dependence of the permttvty February 7, 016 In materals, the delectrc constant and permeablty are actually frequency dependent. Ths does not affect our results for sngle frequency modes, but
More informationTHE VIBRATIONS OF MOLECULES II THE CARBON DIOXIDE MOLECULE Student Instructions
THE VIBRATIONS OF MOLECULES II THE CARBON DIOXIDE MOLECULE Student Instructons by George Hardgrove Chemstry Department St. Olaf College Northfeld, MN 55057 hardgrov@lars.acc.stolaf.edu Copyrght George
More informationA particle in a state of uniform motion remain in that state of motion unless acted upon by external force.
The fundamental prncples of classcal mechancs were lad down by Galleo and Newton n the 16th and 17th centures. In 1686, Newton wrote the Prncpa where he gave us three laws of moton, one law of gravty,
More informationTHE CURRENT BALANCE Physics 258/259
DSH 1988, 005 THE CURRENT BALANCE Physcs 58/59 The tme average force between two parallel conductors carryng an alternatng current s measured by balancng ths force aganst the gravtatonal force on a set
More information8.6 The Complex Number System
8.6 The Complex Number System Earler n the chapter, we mentoned that we cannot have a negatve under a square root, snce the square of any postve or negatve number s always postve. In ths secton we want
More informationElectrical Engineering Department Network Lab.
Electrcal Engneerng Department Network Lab. Objecte: - Experment on -port Network: Negate Impedance Conerter To fnd the frequency response of a smple Negate Impedance Conerter Theory: Negate Impedance
More informationNote 10. Modeling and Simulation of Dynamic Systems
Lecture Notes of ME 475: Introducton to Mechatroncs Note 0 Modelng and Smulaton of Dynamc Systems Department of Mechancal Engneerng, Unversty Of Saskatchewan, 57 Campus Drve, Saskatoon, SK S7N 5A9, Canada
More informationPHYS 705: Classical Mechanics. Newtonian Mechanics
1 PHYS 705: Classcal Mechancs Newtonan Mechancs Quck Revew of Newtonan Mechancs Basc Descrpton: -An dealzed pont partcle or a system of pont partcles n an nertal reference frame [Rgd bodes (ch. 5 later)]
More informationWeek 9 Chapter 10 Section 1-5
Week 9 Chapter 10 Secton 1-5 Rotaton Rgd Object A rgd object s one that s nondeformable The relatve locatons of all partcles makng up the object reman constant All real objects are deformable to some extent,
More informationPhysics 111: Mechanics Lecture 11
Physcs 111: Mechancs Lecture 11 Bn Chen NJIT Physcs Department Textbook Chapter 10: Dynamcs of Rotatonal Moton q 10.1 Torque q 10. Torque and Angular Acceleraton for a Rgd Body q 10.3 Rgd-Body Rotaton
More informationCircuits II EE221. Instructor: Kevin D. Donohue. Instantaneous, Average, RMS, and Apparent Power, and, Maximum Power Transfer, and Power Factors
Crcuts II EE1 Unt 3 Instructor: Ken D. Donohue Instantaneous, Aerage, RMS, and Apparent Power, and, Maxmum Power pp ransfer, and Power Factors Power Defntons/Unts: Work s n unts of newton-meters or joules
More informationSelected Student Solutions for Chapter 2
/3/003 Assessment Prolems Selected Student Solutons for Chapter. Frst note that we know the current through all elements n the crcut except the 6 kw resstor (the current n the three elements to the left
More informationElectrical double layer: revisit based on boundary conditions
Electrcal double layer: revst based on boundary condtons Jong U. Km Department of Electrcal and Computer Engneerng, Texas A&M Unversty College Staton, TX 77843-318, USA Abstract The electrcal double layer
More informationEE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING
EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING TaChang Chen Unersty of Washngton, Bothell Sprng 2010 EE215 1 WEEK 8 FIRST ORDER CIRCUIT RESPONSE May 21 st, 2010 EE215 2 1 QUESTIONS TO ANSWER Frst order crcuts
More informationThe equation of motion of a dynamical system is given by a set of differential equations. That is (1)
Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence
More informationDEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA. 1. Matrices in Mathematica
demo8.nb 1 DEMO #8 - GAUSSIAN ELIMINATION USING MATHEMATICA Obectves: - defne matrces n Mathematca - format the output of matrces - appl lnear algebra to solve a real problem - Use Mathematca to perform
More informationELECTRONICS. EE 42/100 Lecture 4: Resistive Networks and Nodal Analysis. Rev B 1/25/2012 (9:49PM) Prof. Ali M. Niknejad
A. M. Nknejad Unversty of Calforna, Berkeley EE 100 / 42 Lecture 4 p. 1/14 EE 42/100 Lecture 4: Resstve Networks and Nodal Analyss ELECTRONICS Rev B 1/25/2012 (9:49PM) Prof. Al M. Nknejad Unversty of Calforna,
More informationUNIT I BASIC CIRCUIT CONCEPTS
UNIT I BASIC CIRCUIT CONCEPTS Crcut elements Krchhoff s Law V-I Relatonshp of R,L and C Independent and Dependent sources Smple Resstve crcuts Networks reducton Voltage dvson current source transformaton.
More informationInductor = (coil of wire)
A student n 1120 emaled me to ask how much extra he should expect to pay on hs electrc bll when he strngs up a standard 1-strand box of ccle holday lghts outsde hs house. (total, cumulatve cost)? Try to
More informationCOMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD
COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD Ákos Jósef Lengyel, István Ecsed Assstant Lecturer, Professor of Mechancs, Insttute of Appled Mechancs, Unversty of Mskolc, Mskolc-Egyetemváros,
More informationForce = F Piston area = A
CHAPTER III Ths chapter s an mportant transton between the propertes o pure substances and the most mportant chapter whch s: the rst law o thermodynamcs In ths chapter, we wll ntroduce the notons o heat,
More informationIndeterminate pin-jointed frames (trusses)
Indetermnate pn-jonted frames (trusses) Calculaton of member forces usng force method I. Statcal determnacy. The degree of freedom of any truss can be derved as: w= k d a =, where k s the number of all
More informationENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15
NGN 40 ynamcs and Vbratons Homework # 7 ue: Frday, Aprl 15 1. Consder a concal hostng drum used n the mnng ndustry to host a mass up/down. A cable of dameter d has the mass connected at one end and s wound/unwound
More informationB and H sensors for 3-D magnetic property testing
B and H sensors for 3-D magnetc property testng Zh We Ln, Jan Guo Zhu, You Guang Guo, Jn Jang Zhong, and Ha We Lu Faculty of Engneerng, Unversty of Technology, Sydney, PO Bo 123, Broadway, SW 2007, Australa
More informationUNIVERSITY OF UTAH ELECTRICAL & COMPUTER ENGINEERING DEPARTMENT. 10k. 3mH. 10k. Only one current in the branch:
UNIERSITY OF UTH ELECTRICL & COMPUTER ENGINEERING DEPRTMENT ECE 70 HOMEWORK #6 Soluton Summer 009. fter beng closed a long tme, the swtch opens at t = 0. Fnd (t) for t > 0. t = 0 0kΩ 0kΩ 3mH Step : (Redraw
More information8.022 (E&M) Lecture 8
8.0 (E&M) Lecture 8 Topcs: Electromotve force Crcuts and Krchhoff s rules 1 Average: 59, MS: 16 Quz 1: thoughts Last year average: 64 test slghtly harder than average Problem 1 had some subtletes math
More informationThe classical spin-rotation coupling
LOUAI H. ELZEIN 2018 All Rghts Reserved The classcal spn-rotaton couplng Loua Hassan Elzen Basher Khartoum, Sudan. Postal code:11123 louaelzen@gmal.com Abstract Ths paper s prepared to show that a rgd
More information), it produces a response (output function g (x)
Lnear Systems Revew Notes adapted from notes by Mchael Braun Typcally n electrcal engneerng, one s concerned wth functons of tme, such as a voltage waveform System descrpton s therefore defned n the domans
More informationDynamic Stability Evaluation for an Electromagnetic Contactor
Dynamc Stablty Evaluaton for an Electromagnetc Contactor Cheh-Tsung Ch *1 Chh-Yu Hung * Department of Electrcal Engneerng Chenkuo Technology Unversty No. 1, Cheh Shou N. Rd., Changhua Cty 5, Tawan, R.O.C
More informationCHAPTER 14 GENERAL PERTURBATION THEORY
CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves
More informationFEEDBACK AMPLIFIERS. v i or v s v 0
FEEDBCK MPLIFIERS Feedback n mplers FEEDBCK IS THE PROCESS OF FEEDING FRCTION OF OUTPUT ENERGY (VOLTGE OR CURRENT) BCK TO THE INPUT CIRCUIT. THE CIRCUIT EMPLOYED FOR THIS PURPOSE IS CLLED FEEDBCK NETWORK.
More information