VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING

Size: px
Start display at page:

Download "VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING"

Transcription

1 VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING DEPARTMENT: PROCESS CONTROL AND COMPUTER SYSTEMS BACCALAUREUS TECHNOLOGIAE: ENGINEERING ELECTRICAL SUBJECT : CIRCUIT ANALYSIS IV EICAM4A ASSESSMENT : UNIT FIRST ASSESSMENT DATE : 3 AUGUST 207 DURATION : 4H00 5H30 EXAMINER : R FITCHAT MODERATOR : L COETSEE REQUIREMENTS: Pocket calculator may be ued INSTRUCTIONS:. Neat work requred 2. Number your anwer clearly and correctly Full mark = 50 Total = 50 QUESTION PAPER CONSISTS OF: typed page DO NOT TURN THE PAGE BEFORE PERMISSION IS GRANTED

2 Crcut Analy IV EICAM4A Unt Frt Aement 3 Augut 207 Page Queton For the crcut n Fgure, the wtch S cloed at tme t = 0. Calculate (t) for all tme t. (0) Queton 2 For the crcut hown n Fgure 2, fnd an expreon for (t) for all tme t, f the ource current, (t), gen by: (t) for t 0 for t 0 (2) V (t) amp 0 t F H S t=0 Fgure Fgure 2 Queton 3 Refer to the crcut n Fgure 3 and determne the zero tate tep repone of the oltage (t), acro the capactor. (2) = u(t) 3 H F Fgure 3 Queton 4 For the crcut hown n Fgure 4, the wtch S wa open for a long tme, and t then cloed at tme t = 0. Determne the current (t) n the ½ H nductor and the oltage (t) acro the ¼ F capactor, for all tme t. (6) 2 V S H 2 t=0 F 4 Fgure 4 ---ooo000ooo--- Total: 50 Appendx Trgonometrc dentte: Network model Acot + Bnt = A2 B 2 co (t tan - (B/A)) co = n( + /2) = B 2 A2 n (t + tan - (A/B)) n = co( /2) Euler rule: e j = co + jn co = ½ (e j + e j ) n = ½ j (e j e j L ) Laplace tranform: L[f(t)] = F() = (0) 0 f(t)e - tdt L(0) f(t) F() f(t) F() df(t)/dt F() f(0) te -at u(t) /(+a) 2 t 0 f(t)dt F()/ nt u(t) /(2 + 2 ) (t) cot u(t) /( ) u(t) / e -at nt u(t) /[(+a) ] e -at u(t) /(+a) e -at cot u(t) (+a)/[(+a) ] tu(t) / 2 2Ae -at co(t+)u(t) A A a j a j C (0) C(0) C L

3 Faculty: Department: Dploma: Subject: Internal code: VAAL UNIVERSITY OF TECHNOLOGY Engneerng Coer Sheet for Memorandum (Unt Frt Aement 3 Augut 207) Proce Control and Computer Sytem Baccalaureu Technologae: Engneerng: Electrcal Crcut Analy IV EICAM4A Nne dgt code: Hour: Examner: Moderator: ½ R Ftchat L Coetee Total Mark: 50 Full mark: 50 Sgnature of Examner: Sgnature of Moderator: Date: Date:

4 Stroombaananale IV EICAM4A Eenhed Eerte Ealuae 3 Augutu 206 Memorandum Blady. t < 0: (t) = V [2] t 0: = d/dt + d/dt + 2 = [5] = Ae 2t + ½ [] (0) = A = ½ [] [0] (t) = ½(e 2t + ) [] t < 0 t 0 V 2. t < 0: (t) = ½ A [] t 0: Node N: = +... () t < 0 t 0 N Loop L: d/dt = 0 = + d/dt... (2) L (2) n (): = + + d/dt d/dt d/dt + 2 = [6] [2] (t) = ( /2) + Ae 2t [2] but (0) = ½ A = [] (t) = ½ + e 2t amp, for t 0 [2] 3. t < 0: (t) = 0 [½], (t) = 0 [½] zero tate t 0: 3 d/dt = 0 en = + d/dt 3 d/dt 3( + d/dt) d/dt( + d/dt) = 0 3 3d/dt d/dt d 2 /dt 2 = 0 d 2 /dt 2 + 4d/dt + 4 = [6] = 2 en n = 2 krtek gedemp (t) = Ate -2t + Be -2t + ¼ [2] (0) = 0 B + ¼ = 0 B = ¼ d/dt = Ae -2t 2Ate -2t 2Be -2t d(0)/dt = A 2B V 3 d(0)dt = (0) (0) = 0 A 2B = 0 A 2( /4) = 0 A = /2 [2] (t) = ½te -2t ¼e -2t + ¼ [3] [6] ½ 0 4. t < 0: (t) = V [] en (t) = A [] t 0: Loop contanng ½H and ¼F (loop L): L + = 0 ½d/dt + = 0 = ½d/dt... () 2 V Node N: = C + R = ¼d/dt + / = ¼d/dt +... (2) () n (2): {or (2) n ()} = ¼d/dt( ½d/dt) + ( ½d/dt) { = ½d/dt(¼d/dt+} (/8)d 2 /dt 2 + ½d/dt + = 0 {(/8)d 2 /dt 2 +½d/dt+=0} d 2 /dt 2 + 4d/dt + 8 = 0 [6] {d 2 /dt 2 +4d/dt+8=0 [6] } = 2 and n = 8 underdamped wth d = 2 r/ (t) = Ae -2t co2t+be -2t n2t [2] {(t)=ae -2t co2t+be -2t n2t [2] } t (0) = A = {(0)= A=} d/dt = 2Ae 2t co2t 2Ae 2t n2t 2Be 2t n2t + 2Be 2t co2t d(0)/dt = 2A + 2B {d/dt= 2Ae 2t co2t 2Ae 2t n2t 2Be 2t n2t+2be 2t co2td(0)/dt= 2A+2B} but (0) = ½d(0)/dt (from ()) = ½d(0)/dt d(0)/dt = 2 {but (0)=¼d(0)/dt+(0) (from (2)) =¼d(0)/dt+ d(0)/dt=0} 2() + 2B = 2 B = 0 (t) = e 2t co2t for t 0 [4] { 2() + 2B = 0 B = (t) = e 2t co2t + e 2t n2t [4] } and d/dt = 2e 2t co2t 2e 2t n2t {and d/dt = 2e 2t co2t 2e 2t n2t 2e 2t n2t+2e 2t co2t = 4e 2t n2t} (t) = ½d/dt = ½( 2e 2t co2t 2e 2t n2t) = e 2t co2t + e 2t n2t [2] {(t)=¼d/dt+=¼[ 4e 2t n2t] + e 2t co2t + e 2t n2t = e 2t co2t [2] } F V L F 2 4 N d/dt t < 0 t 0 L C R

5 VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING DEPARTMENT: PROCESS CONTROL AND COMPUTER SYSTEMS BACCALAUREUS TECHNOLOGIAE: ENGINEERING ELECTRICAL SUBJECT : CIRCUIT ANALYSIS IV EICAM4A ASSESSMENT : UNIT 2 FIRST ASSESSMENT DATE : 28 SEPTEMBER 207 DURATION : 0H00 H30 EXAMINER : R FITCHAT MODERATOR : L COETSEE REQUIREMENTS: Pocket calculator may be ued INSTRUCTIONS:. Neat work requred 2. Number your anwer clearly and correctly Full mark = 50 Total = 50 QUESTION PAPER CONSISTS OF: typed page DO NOT TURN THE PAGE BEFORE PERMISSION IS GRANTED

6 Crcut Analy IV EICAM4A Unt 2 Frt Aement 28 September 207 Page Queton Refer to the crcut n Fgure. a) Fnd the teady tate current repone (t) n the tme doman, olng the dfferental equaton for, f the upply oltage, gen by the real nuod (t) = co2t olt. Ge your anwer n the form, Aco(t + ). (0) b) Fnd the teady tate current repone (t) n the tme doman, olng the dfferental equaton for, f the upply oltage the complex nuod = e j2t olt. Ge your anwer n the form Ae j(t + ). (6) c) Ue frequency doman analy to determne the phaor current I, f the upply oltage the phaor V = 0 olt. Recontruct the tme form of (t), Aco(t + ), agan from the phaor current I. (6) Queton 2 Refer to the crcut n Fgure 2. a) Determne the reonance frequency of the crcut from the perpecte that the mpedance een by the ource, mut become real. (0) b) Calculate the mpedance of the crcut at reonance. (2) Queton 3 Refer to the crcut n Fgure 3. The upply oltage to the crcut gen by (t) = co2t u(t) olt. The ntal current through the nductor (0) = 0 amp and the ntal oltage acro the capactor (0) = 0 olt. Draw an equalent Laplace network model for the crcut and ue th model to fnd an expreon for (t). (6) co2t e j2t 0 ---ooo000ooo--- Total: 50 = co2t u(t) F F H 2 (0) = 0 H Fgure F (0) = 0 H Fgure 2 Fgure 3 Appendx Trgonometrc dentte: Network model Acot + Bnt = A2 B 2 co (t tan - (B/A)) co = n( + /2) = B 2 n (t + tan - A2 (A/B)) n = co( /2) Euler rule: e j = co + jn co = ½ (e j + e j ) n = ½ j (e j e j ) L Laplace tranform: L[f(t)] = F() = - t (0) 0 f(t)e dt f(t) F() f(t) F() L(0) df(t)/dt F() f(0) te -at u(t) /(+a) 2 t 0 f(t)dt F()/ nt u(t) /(2 + 2 ) (t) cot u(t) /( ) u(t) / e -at nt u(t) /[(+a) ] e -at u(t) /(+a) e -at cot u(t) (+a)/[(+a) ] tu(t) / 2 2Ae -at co(t+)u(t) A A a j a j C (0) C(0) C L

7 VAAL UNIVERSITY OF TECHNOLOGY Coer Sheet for Memorandum (Unt 2 Frt Aement 28 September 207) Faculty: Engneerng Department: Proce Control and Computer Sytem Dploma: Baccalaureu Technologae: Engneerng: Electrcal Subject: Crcut Analy IV Internal code: EICAM4A Nne dgt code: Hour: ½ Examner: R Ftchat Moderator: L Coetee Total Mark: 50 Full mark: 50 Sgnature of Examner: Sgnature of Moderator: Date: Date:

8 [22] Stroombaananale IV EICAM4A Eenhed2 Eerte Ealuae 28 September 207 Memorandum Blady. a) ( )/ = + d/dt... () and = d/dt... (2) d/dt = + d 2 /dt 2 d 2 /dt 2 + d/dt + = d 2 /dt 2 + d/dt + = co2t [5] we nt that = Aco2t + Bn2t, therefore d/dt = 2An2t + 2Bco2t and d 2 /dt 2 = 4Aco2t 4Bn2t 4Aco2t 4 Bn2t 2An2t + 2Bco2t + Aco2t + Bnt = co2t [ 3A + 2B]cot + [ 3B 2A]nt = cot 3A + 2B = en 3B 2A = 0 A = (3/3) = and B = (2/3) = (t) = (3/3)co2t + (2/3)n2t [4] = co(2t ) ampere [] (0) b) For (t) = e j2t d 2 /dt 2 + d/dt + = e j2t j(2t + ) [] we agan nt that (t) mut hae the form, (t) = Ae j(2t + ) therefore d/dt = j2ae j(2t + ) and d 2 /dt 2 = j 2 4Ae j(2t + ) = 4Ae 4Ae j(2t + ) + j2ae j(2t + ) + Ae j(2t + ) = e j2t ( 4 + j2 + )Ae j(2t + ) = e j2t ( 3 + j2)ae j e j2t = e j2t ( 3 + j2)ae j = Ae j = /( 3 + j2) = Ae j = e j A = [2] and = r [2] (t) = e j(2t ) amp [] (6) c) Z = //290) = + [( )/( )] = + (0/.590) = + (2/3) 90= [2] I t = V /Z = 0/ = A [2] I = [0.5 90/( )] I t = [0.5 90/(.590] = = A [] (t) = co(2t r ) [] (6) {or V = [(2/3) 90/(+(2/3) 90)]0= I = /290= } 2. a) Z = + j + 2//(/j) [2] = + j + [2(/j)]/[2 + (/j)] = + j + [2/( + j2)] = + j + [2( j2)/( )] = + j + [2/( )] j[4/( )] j = { + [2/( )]} + j{ [4/( ]} [4] { = [( )/( )] + j{[( ) 4]/( )} 2 /j = [( )/( )] + j[(4 2 3)/( )] } For reonance: Im{Z} = 0 [4/( ] = 0 4/( ) = = = 3 = 3/2 ( r/a) [4] (0) [2] b) Z 0 = { + [2/( )]} = 3/2 = + 2/( + 3) = =.5 (2) [6] 3. [/( 2 + 4) ]/ = + /(/) /( 2 + 4) = + + But = /( 2 + 4) = ( ) = /( 2 + 4) = /( )( 2 + 4) [4] co2t e j2t = 2 r/ = /[( )( )( )( )] [2] = /( ) /( ) /( 2.57) /( 2.57) [4] = /( j ) /( j ) /( + 0 j2) /( j2) (t) = e -0.5t co( t ) e 0 co(2t ) = e -0.5t co( t ) co(2t ) [2] V 0 V 2 4 [] [] I t [] V I 290 / []

Electrical Circuits II (ECE233b)

Electrical Circuits II (ECE233b) Electrcal Crcut II (ECE33b) Applcaton of Laplace Tranform to Crcut Analy Anet Dounav The Unverty of Wetern Ontaro Faculty of Engneerng Scence Crcut Element Retance Tme Doman (t) v(t) R v(t) = R(t) Frequency

More information

S-Domain Analysis. s-domain Circuit Analysis. EE695K VLSI Interconnect. Time domain (t domain) Complex frequency domain (s domain) Laplace Transform L

S-Domain Analysis. s-domain Circuit Analysis. EE695K VLSI Interconnect. Time domain (t domain) Complex frequency domain (s domain) Laplace Transform L EE695K S nterconnect S-Doman naly -Doman rcut naly Tme doman t doman near rcut aplace Tranform omplex frequency doman doman Tranformed rcut Dfferental equaton lacal technque epone waveform aplace Tranform

More information

VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING

VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING VAAL UNIVERSITY OF TECHNOLOGY FACULTY OF ENGINEERING DEPARTMENT: PROCESS CONTROL AND COMPUTER SYSTEMS BACCALAUREUS TECHNOLOGIAE: ENGINEERING ELECTRICAL SUBJECT : DIGITAL CONTROL SYSTEMS IV EIDBS4A ASSESSMENT

More information

Electric and magnetic field sensor and integrator equations

Electric and magnetic field sensor and integrator equations Techncal Note - TN12 Electrc and magnetc feld enor and ntegrator uaton Bertrand Da, montena technology, 1728 oen, Swtzerland Table of content 1. Equaton of the derate electrc feld enor... 1 2. Integraton

More information

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web:     Ph: Serial : LS_N_A_Network Theory_098 Delhi Noida Bhopal Hyderabad Jaipur Lucknow ndore Pune Bhubanewar Kolkata Patna Web: E-mail: info@madeeay.in Ph: 0-4546 CLASS TEST 08-9 NSTRUMENTATON ENGNEERNG Subject

More information

ECE Linear Circuit Analysis II

ECE Linear Circuit Analysis II ECE 202 - Linear Circuit Analyi II Final Exam Solution December 9, 2008 Solution Breaking F into partial fraction, F 2 9 9 + + 35 9 ft δt + [ + 35e 9t ]ut A 9 Hence 3 i the correct anwer. Solution 2 ft

More information

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:

Delhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web:     Ph: Serial : LS_B_EC_Network Theory_0098 CLASS TEST (GATE) Delhi Noida Bhopal Hyderabad Jaipur Lucknow ndore Pune Bhubanewar Kolkata Patna Web: E-mail: info@madeeay.in Ph: 0-4546 CLASS TEST 08-9 ELECTRONCS

More information

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab

Boise 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 information

Boise State University Department of Electrical and Computer Engineering ECE 212L Circuit Analysis and Design Lab

Boise 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 information

EE215 FUNDAMENTALS OF ELECTRICAL ENGINEERING

EE215 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 information

Electrical Engineering Department Network Lab.

Electrical 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 information

1. /25 2. /30 3. /25 4. /20 Total /100

1. /25 2. /30 3. /25 4. /20 Total /100 Circuit Exam 2 Spring 206. /25 2. /30 3. /25 4. /20 Total /00 Name Pleae write your name at the top of every page! Note: ) If you are tuck on one part of the problem, chooe reaonable value on the following

More information

ECE-202 FINAL December 13, 2016 CIRCLE YOUR DIVISION

ECE-202 FINAL December 13, 2016 CIRCLE YOUR DIVISION ECE-202 Final, Fall 16 1 ECE-202 FINAL December 13, 2016 Name: (Pleae print clearly.) Student Email: CIRCLE YOUR DIVISION DeCarlo- 8:30-9:30 Talavage-9:30-10:30 2021 2022 INSTRUCTIONS There are 35 multiple

More information

Small signal analysis

Small signal analysis Small gnal analy. ntroducton Let u conder the crcut hown n Fg., where the nonlnear retor decrbed by the equaton g v havng graphcal repreentaton hown n Fg.. ( G (t G v(t v Fg. Fg. a D current ource wherea

More information

ECE-202 Exam 1 January 31, Name: (Please print clearly.) CIRCLE YOUR DIVISION DeCarlo DeCarlo 7:30 MWF 1:30 TTH

ECE-202 Exam 1 January 31, Name: (Please print clearly.) CIRCLE YOUR DIVISION DeCarlo DeCarlo 7:30 MWF 1:30 TTH ECE-0 Exam January 3, 08 Name: (Pleae print clearly.) CIRCLE YOUR DIVISION 0 0 DeCarlo DeCarlo 7:30 MWF :30 TTH INSTRUCTIONS There are multiple choice worth 5 point each and workout problem worth 40 point.

More information

Energy Storage Elements: Capacitors and Inductors

Energy 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 information

Introduction to Laplace Transform Techniques in Circuit Analysis

Introduction to Laplace Transform Techniques in Circuit Analysis Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found

More information

TMA4125 Matematikk 4N Spring 2016

TMA4125 Matematikk 4N Spring 2016 Norwegian Univerity of Science and Technology Department of Mathematical Science TMA45 Matematikk 4N Spring 6 Solution to problem et 6 In general, unle ele i noted, if f i a function, then F = L(f denote

More information

Electrical Circuits II (ECE233b)

Electrical Circuits II (ECE233b) Electrcal Crcuts (ECE33b SteadyState Power Analyss Anests Dounas The Unersty of Western Ontaro Faculty of Engneerng Scence SteadyState Power Analyss (t AC crcut: The steady state oltage and current can

More information

ME 375 FINAL EXAM Wednesday, May 6, 2009

ME 375 FINAL EXAM Wednesday, May 6, 2009 ME 375 FINAL EXAM Wedneday, May 6, 9 Diviion Meckl :3 / Adam :3 (circle one) Name_ Intruction () Thi i a cloed book examination, but you are allowed three ingle-ided 8.5 crib heet. A calculator i NOT allowed.

More information

KIRCHHOFF CURRENT LAW

KIRCHHOFF CURRENT LAW KRCHHOFF CURRENT LAW ONE OF THE FUNDAMENTAL CONSERATON PRNCPLES N ELECTRCAL ENGNEERNG CHARGE CANNOT BE CREATED NOR DESTROYED NODES, BRANCHES, LOOPS A NODE CONNECTS SEERAL COMPONENTS. BUT T DOES NOT HOLD

More information

(b) i(t) for t 0. (c) υ 1 (t) and υ 2 (t) for t 0. Solution: υ 2 (0 ) = I 0 R 1 = = 10 V. υ 1 (0 ) = 0. (Given).

(b) i(t) for t 0. (c) υ 1 (t) and υ 2 (t) for t 0. Solution: υ 2 (0 ) = I 0 R 1 = = 10 V. υ 1 (0 ) = 0. (Given). Problem 5.37 Pror to t =, capactor C 1 n the crcut of Fg. P5.37 was uncharged. For I = 5 ma, R 1 = 2 kω, = 5 kω, C 1 = 3 µf, and C 2 = 6 µf, determne: (a) The equvalent crcut nvolvng the capactors for

More information

Chapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1

Chapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1 Chapter Homework Solution P.-1,, 5 P.4-1, 3, 5, 6, 7 P.5-1, 3, 5 P.6-, 5 P.7-1, 4 P.8-1 P.9-1 P.-1 An element ha oltage and current i a hown in Figure P.-1a. Value of the current i and correponding oltage

More information

Math 334 Fall 2011 Homework 10 Solutions

Math 334 Fall 2011 Homework 10 Solutions Nov. 5, Math 334 Fall Homework Solution Baic Problem. Expre the following function uing the unit tep function. And ketch their graph. < t < a g(t = < t < t > t t < b g(t = t Solution. a We

More information

Complex Numbers, Signals, and Circuits

Complex 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 information

Circuit Theorems. Introduction

Circuit Theorems. Introduction //5 Crcut eorem ntroducton nearty Property uperpoton ource Tranformaton eenn eorem orton eorem Maxmum Power Tranfer ummary ntroducton To deelop analy technque applcable to lnear crcut. To mplfy crcut analy

More information

COLLEGE OF ENGINEERING PUTRAJAYA CAMPUS FINAL EXAMINATION SPECIAL SEMESTER 2013 / 2014

COLLEGE OF ENGINEERING PUTRAJAYA CAMPUS FINAL EXAMINATION SPECIAL SEMESTER 2013 / 2014 OLLEGE OF ENGNEENG PUTAJAYA AMPUS FNAL EXAMNATON SPEAL SEMESTE 03 / 04 POGAMME SUBJET ODE SUBJET : Bachelor of Electrcal & Electroncs Engneerng (Honours) Bachelor of Electrcal Power Engneerng (Honours)

More information

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: December 13, E Main Suite D Pullman, WA (509) Voice and Fax .9.1: AC power analyss Reson: Deceber 13, 010 15 E Man Sute D Pullan, WA 99163 (509 334 6306 Voce and Fax Oerew n chapter.9.0, we ntroduced soe basc quanttes relate to delery of power usng snusodal sgnals.

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Circuits and Electronics Spring 2001

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science Circuits and Electronics Spring 2001 Massachusetts Insttute of Technology Department of Electrcal Engneerng and Computer Scence Read Chapters 11 through 12. 6.002 Crcuts and Electroncs Sprng 2001 Homework #5 Handout S01031 Issued: 3/8/2001

More information

These are practice problems for the final exam. You should attempt all of them, but turn in only the even-numbered problems!

These are practice problems for the final exam. You should attempt all of them, but turn in only the even-numbered problems! Math 33 - ODE Due: 7 December 208 Written Problem Set # 4 Thee are practice problem for the final exam. You hould attempt all of them, but turn in only the even-numbered problem! Exercie Solve the initial

More information

ECE-320 Linear Control Systems. Spring 2014, Exam 1. No calculators or computers allowed, you may leave your answers as fractions.

ECE-320 Linear Control Systems. Spring 2014, Exam 1. No calculators or computers allowed, you may leave your answers as fractions. ECE-0 Linear Control Sytem Spring 04, Exam No calculator or computer allowed, you may leave your anwer a fraction. All problem are worth point unle noted otherwie. Total /00 Problem - refer to the unit

More information

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax:

Control Systems Engineering ( Chapter 7. Steady-State Errors ) Prof. Kwang-Chun Ho Tel: Fax: Control Sytem Engineering ( Chapter 7. Steady-State Error Prof. Kwang-Chun Ho kwangho@hanung.ac.kr Tel: 0-760-453 Fax:0-760-4435 Introduction In thi leon, you will learn the following : How to find the

More information

ELECTRIC POWER CIRCUITS BASIC CONCEPTS AND ANALYSIS

ELECTRIC POWER CIRCUITS BASIC CONCEPTS AND ANALYSIS Contents ELEC46 Power ystem Analysis Lecture ELECTRC POWER CRCUT BAC CONCEPT AND ANALY. Circuit analysis. Phasors. Power in single phase circuits 4. Three phase () circuits 5. Power in circuits 6. ingle

More information

ME 375 EXAM #1 Tuesday February 21, 2006

ME 375 EXAM #1 Tuesday February 21, 2006 ME 375 EXAM #1 Tueday February 1, 006 Diviion Adam 11:30 / Savran :30 (circle one) Name Intruction (1) Thi i a cloed book examination, but you are allowed one 8.5x11 crib heet. () You have one hour to

More information

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation:

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation: HPT 3 xercses 3. The emtter current s gen by the Shockley equaton: S exp VT For operaton wth, we hae exp >> S >>, and we can wrte VT S exp VT Solng for, we hae 3. 0 6ln 78.4 mv 0 0.784 5 4.86 V VT ln 4

More information

ME 375 FINAL EXAM SOLUTIONS Friday December 17, 2004

ME 375 FINAL EXAM SOLUTIONS Friday December 17, 2004 ME 375 FINAL EXAM SOLUTIONS Friday December 7, 004 Diviion Adam 0:30 / Yao :30 (circle one) Name Intruction () Thi i a cloed book eamination, but you are allowed three 8.5 crib heet. () You have two hour

More information

College of Engineering Department of Electronics and Communication Engineering. Test 1 With Model Answer

College of Engineering Department of Electronics and Communication Engineering. Test 1 With Model Answer Name: Student D Number: Secton Number: 01/0/03/04 A/B Lecturer: Dr Jamaludn/ Dr Jehana Ermy/ Dr Azn Wat Table Number: College of Engneerng Department of Electroncs and Communcaton Engneerng Test 1 Wth

More information

Formulation of Circuit Equations

Formulation 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 information

ENE 104 Electric Circuit Theory

ENE 104 Electric Circuit Theory ENE 4 Electrc rcut Theory ecture 8: The R rcut (cont. : Dejwoot KHAWPARISUTH http://webtaff.kmutt.ac.th/~dejwoot.kha/ ENE 4 Objectve : h9 The R rcut Page the charactertc dampng factor and reonant frequency

More information

Math 201 Lecture 17: Discontinuous and Periodic Functions

Math 201 Lecture 17: Discontinuous and Periodic Functions Math 2 Lecture 7: Dicontinuou and Periodic Function Feb. 5, 22 Many example here are taken from the textbook. he firt number in () refer to the problem number in the UA Cutom edition, the econd number

More information

INDUCTANCE. RC Cicuits vs LR Circuits

INDUCTANCE. 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 information

S.E. Sem. III [EXTC] Circuits and Transmission Lines

S.E. Sem. III [EXTC] Circuits and Transmission Lines S.E. Sem. III [EXTC] Circuit and Tranmiion Line Time : Hr.] Prelim Quetion Paper Solution [Mark : 80 Q.(a) Tet whether P() = 5 4 45 60 44 48 i Hurwitz polynomial. (A) P() = 5 4 45 60 44 48 5 45 44 4 60

More information

Linearity. 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

Linearity. 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 information

online learning Unit Workbook 4 RLC Transients

online learning Unit Workbook 4 RLC Transients online learning Pearon BTC Higher National in lectrical and lectronic ngineering (QCF) Unit 5: lectrical & lectronic Principle Unit Workbook 4 in a erie of 4 for thi unit Learning Outcome: RLC Tranient

More information

EE 2006 Electric Circuit Analysis Fall September 04, 2014 Lecture 02

EE 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 information

EE C128 / ME C134 Problem Set 1 Solution (Fall 2010) Wenjie Chen and Jansen Sheng, UC Berkeley

EE C128 / ME C134 Problem Set 1 Solution (Fall 2010) Wenjie Chen and Jansen Sheng, UC Berkeley EE C28 / ME C34 Problem Set Solution (Fall 200) Wenjie Chen and Janen Sheng, UC Berkeley. (0 pt) BIBO tability The ytem h(t) = co(t)u(t) i not BIBO table. What i the region of convergence for H()? A bounded

More information

1. Linear second-order circuits

1. Linear second-order circuits ear eco-orer crcut Sere R crcut Dyamc crcut cotag two capactor or two uctor or oe uctor a oe capactor are calle the eco orer crcut At frt we coer a pecal cla of the eco-orer crcut, amely a ere coecto of

More information

College of Engineering Department of Electronics and Communication Engineering. Test 2

College of Engineering Department of Electronics and Communication Engineering. Test 2 Name: Student D Number: Secton Number: 01/0/03/04 A/B Lecturer: Dr Jamaludn/ Dr Azn Wat/ Dr Jehana Ermy/ Prof Md Zan Table Number: ollege of Engneerng Department of Electroncs and ommuncaton Engneerng

More information

Coupling Element and Coupled circuits. Coupled inductor Ideal transformer Controlled sources

Coupling 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 information

TUTORIAL PROBLEMS. E.1 KCL, KVL, Power and Energy. Q.1 Determine the current i in the following circuit. All units in VAΩ,,

TUTORIAL 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 information

EE 2006 Electric Circuit Analysis Spring January 23, 2015 Lecture 02

EE 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 information

R L R L L sl C L 1 sc

R L R L L sl C L 1 sc 2260 N. Cotter PRACTICE FINAL EXAM SOLUTION: Prob 3 3. (50 point) u(t) V i(t) L - R v(t) C - The initial energy tored in the circuit i zero. 500 Ω L 200 mh a. Chooe value of R and C to accomplih the following:

More information

Solving Differential Equations by the Laplace Transform and by Numerical Methods

Solving Differential Equations by the Laplace Transform and by Numerical Methods 36CH_PHCalter_TechMath_95099 3//007 :8 PM Page Solving Differential Equation by the Laplace Tranform and by Numerical Method OBJECTIVES When you have completed thi chapter, you hould be able to: Find the

More information

MAE140 - Linear Circuits - Winter 16 Final, March 16, 2016

MAE140 - 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 information

I. INTRODUCTION. There are two other circuit elements that we will use and are special cases of the above elements. They are:

I. 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 information

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002 Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in

More information

Question 1 Equivalent Circuits

Question 1 Equivalent Circuits MAE 40 inear ircuit Fall 2007 Final Intruction ) Thi exam i open book You may ue whatever written material you chooe, including your cla note and textbook You may ue a hand calculator with no communication

More information

MAE140 Linear Circuits Fall 2012 Final, December 13th

MAE140 Linear Circuits Fall 2012 Final, December 13th MAE40 Linear Circuit Fall 202 Final, December 3th Intruction. Thi exam i open book. You may ue whatever written material you chooe, including your cla note and textbook. You may ue a hand calculator with

More information

Properties of Z-transform Transform 1 Linearity a

Properties of Z-transform Transform 1 Linearity a Midterm 3 (Fall 6 of EEG:. Thi midterm conit of eight ingle-ided page. The firt three page contain variou table followed by FOUR eam quetion and one etra workheet. You can tear out any page but make ure

More information

Selected Student Solutions for Chapter 2

Selected 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 information

Digital Control System

Digital Control System Digital Control Sytem Summary # he -tranform play an important role in digital control and dicrete ignal proceing. he -tranform i defined a F () f(k) k () A. Example Conider the following equence: f(k)

More information

EE C245 ME C218 Introduction to MEMS Design

EE C245 ME C218 Introduction to MEMS Design EE C45 ME C8 Introducton to MEM Desgn Fall 7 Prof. Clark T.C. Nguyen Dept. of Electrcal Engneerng & Computer cences Unersty of Calforna at Berkeley Berkeley, C 947 Dscusson: eew of Op mps EE C45: Introducton

More information

6.01: Introduction to EECS I Lecture 7 March 15, 2011

6.01: Introduction to EECS I Lecture 7 March 15, 2011 6.0: Introducton to EECS I Lecture 7 March 5, 20 6.0: Introducton to EECS I Crcuts The Crcut Abstracton Crcuts represent systems as connectons of elements through whch currents (through arables) flow and

More information

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances

ECE 3510 Root Locus Design Examples. PI To eliminate steady-state error (for constant inputs) & perfect rejection of constant disturbances ECE 350 Root Locu Deign Example Recall the imple crude ervo from lab G( ) 0 6.64 53.78 σ = = 3 23.473 PI To eliminate teady-tate error (for contant input) & perfect reection of contant diturbance Note:

More information

Lecture 6: Resonance II. Announcements

Lecture 6: Resonance II. Announcements EES 5 Spring 4, Lecture 6 Lecture 6: Reonance II EES 5 Spring 4, Lecture 6 Announcement The lab tart thi week You mut how up for lab to tay enrolled in the coure. The firt lab i available on the web ite,

More information

COLLEGE OF ENGINEERING PUTRAJAYA CAMPUS FINAL EXAMINATION SEMESTER / 2014

COLLEGE OF ENGINEERING PUTRAJAYA CAMPUS FINAL EXAMINATION SEMESTER / 2014 OLLEGE OF ENGNEERNG PUTRAJAYA AMPUS FNAL EXAMNATON SEMESTER 013 / 014 PROGRAMME SUBJET ODE SUBJET : Bachelor of Electrcal & Electrocs Egeerg (Hoours) Bachelor of Electrcal Power Egeerg (Hoours) : EEEB73

More information

Small-Signal Model for Buck/Boost Converter

Small-Signal Model for Buck/Boost Converter 4 Small-Sgnal Model for Buck/Boot Converter For the buck/boot converter, k k and k k becaue v v and v v. * f r m e The model can be ued to derve k, k, F, and H ( ),whch can be adapted to all the three

More information

Mathematical modeling of control systems. Laith Batarseh. Mathematical modeling of control systems

Mathematical modeling of control systems. Laith Batarseh. Mathematical modeling of control systems Chapter two Laith Batareh Mathematical modeling The dynamic of many ytem, whether they are mechanical, electrical, thermal, economic, biological, and o on, may be decribed in term of differential equation

More information

CONTROL SYSTEMS. Chapter 2 : Block Diagram & Signal Flow Graphs GATE Objective & Numerical Type Questions

CONTROL SYSTEMS. Chapter 2 : Block Diagram & Signal Flow Graphs GATE Objective & Numerical Type Questions ONTOL SYSTEMS hapter : Bloc Diagram & Signal Flow Graph GATE Objective & Numerical Type Quetion Quetion 6 [Practice Boo] [GATE E 994 IIT-Kharagpur : 5 Mar] educe the ignal flow graph hown in figure below,

More information

e st t u(t 2) dt = lim t dt = T 2 2 e st = T e st lim + e st

e st t u(t 2) dt = lim t dt = T 2 2 e st = T e st lim + e st Math 46, Profeor David Levermore Anwer to Quetion for Dicuion Friday, 7 October 7 Firt Set of Quetion ( Ue the definition of the Laplace tranform to compute Lf]( for the function f(t = u(t t, where u i

More information

6.302 Feedback Systems Recitation 6: Steady-State Errors Prof. Joel L. Dawson S -

6.302 Feedback Systems Recitation 6: Steady-State Errors Prof. Joel L. Dawson S - 6302 Feedback ytem Recitation 6: teadytate Error Prof Joel L Dawon A valid performance metric for any control ytem center around the final error when the ytem reache teadytate That i, after all initial

More information

ECE382/ME482 Spring 2004 Homework 4 Solution November 14,

ECE382/ME482 Spring 2004 Homework 4 Solution November 14, ECE382/ME482 Spring 2004 Homework 4 Solution November 14, 2005 1 Solution to HW4 AP4.3 Intead of a contant or tep reference input, we are given, in thi problem, a more complicated reference path, r(t)

More information

MECH321 Dynamics of Engineering System Week 4 (Chapter 6)

MECH321 Dynamics of Engineering System Week 4 (Chapter 6) MH3 Dynamc of ngnrng Sytm Wk 4 (haptr 6). Bac lctrc crcut thor. Mathmatcal Modlng of Pav rcut 3. ompl mpdanc Approach 4. Mchancal lctrcal analogy 5. Modllng of Actv rcut: Opratonal Amplfr rcut Bac lctrc

More information

EE/ME/AE324: Dynamical Systems. Chapter 8: Transfer Function Analysis

EE/ME/AE324: Dynamical Systems. Chapter 8: Transfer Function Analysis EE/ME/AE34: Dynamical Sytem Chapter 8: Tranfer Function Analyi The Sytem Tranfer Function Conider the ytem decribed by the nth-order I/O eqn.: ( n) ( n 1) ( m) y + a y + + a y = b u + + bu n 1 0 m 0 Taking

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 R. W. Erickon Department of Electrical, Computer, and Energy Engineering Univerity of Colorado, Boulder Cloed-loop buck converter example: Section 9.5.4 In ECEN 5797, we ued the CCM mall ignal model to

More information

Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 3A

Designing 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 information

Digital Simulation of Power Systems and Power Electronics using the MATLAB Power System Blockset 筑龙网

Digital Simulation of Power Systems and Power Electronics using the MATLAB Power System Blockset 筑龙网 Dgtal Smulaton of Power Sytem and Power Electronc ung the MATAB Power Sytem Blocket Power Sytem Blocket Htory Deeloped by IREQ (HydroQuébec) n cooperaton wth Teqm, Unerté aal (Québec), and École de Technologe

More information

matter consists, measured in coulombs (C) 1 C of charge requires electrons Law of conservation of charge: charge cannot be created or

matter 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 information

Lecture 10: Small Signal Device Parameters

Lecture 10: Small Signal Device Parameters Lecture 0: Small Sgnal Dece Parameters 06009 Lecture 9, Hgh Speed Deces 06 Lecture : Ballstc FETs Lu: 0, 394 06009 Lecture 9, Hgh Speed Deces 06 Large Sgnal / Small Sgnal e I E c I C The electrcal sgnal

More information

( ) = ( ) + ( 0) ) ( )

( ) = ( ) + ( 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 information

Graphical Analysis of a BJT Amplifier

Graphical Analysis of a BJT Amplifier 4/6/2011 A Graphcal Analyss of a BJT Amplfer lecture 1/18 Graphcal Analyss of a BJT Amplfer onsder agan ths smple BJT amplfer: ( t) = + ( t) O O o B + We note that for ths amplfer, the output oltage s

More information

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d)

G = G 1 + G 2 + G 3 G 2 +G 3 G1 G2 G3. Network (a) Network (b) Network (c) Network (d) Massachusetts Insttute of Technology Department of Electrcal Engneerng and Computer Scence 6.002 í Electronc Crcuts Homework 2 Soluton Handout F98023 Exercse 21: Determne the conductance of each network

More information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electronc Crcuts Feedback & Stablty Sectons of Chapter 2. Kruger Feedback & Stablty Confguraton of Feedback mplfer Negate feedback β s the feedback transfer functon S o S S o o S S o f S S S S fb

More information

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get

into a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}

More information

ECE 320 Energy Conversion and Power Electronics Dr. Tim Hogan. Chapter 1: Introduction and Three Phase Power

ECE 320 Energy Conversion and Power Electronics Dr. Tim Hogan. Chapter 1: Introduction and Three Phase Power ECE 3 Energy Conerson and Power Electroncs Dr. Tm Hogan Chapter : ntroducton and Three Phase Power. eew of Basc Crcut Analyss Defntons: Node - Electrcal juncton between two or more deces. Loop - Closed

More information

GATE SOLVED PAPER - EC

GATE SOLVED PAPER - EC 0 ONE MARK Q. Conider a delta connection of reitor and it equivalent tar connection a hown below. If all element of the delta connection are caled by a factor k, k > 0, the element of the correponding

More information

ANSWERS TO MA1506 TUTORIAL 7. Question 1. (a) We shall use the following s-shifting property: L(f(t)) = F (s) L(e ct f(t)) = F (s c)

ANSWERS TO MA1506 TUTORIAL 7. Question 1. (a) We shall use the following s-shifting property: L(f(t)) = F (s) L(e ct f(t)) = F (s c) ANSWERS O MA56 UORIAL 7 Quetion. a) We hall ue the following -Shifting property: Lft)) = F ) Le ct ft)) = F c) Lt 2 ) = 2 3 ue Ltn ) = n! Lt 2 e 3t ) = Le 3t t 2 ) = n+ 2 + 3) 3 b) Here u denote the Unit

More information

Modeling in the Frequency Domain

Modeling in the Frequency Domain T W O Modeling in the Frequency Domain SOLUTIONS TO CASE STUDIES CHALLENGES Antenna Control: Tranfer Function Finding each tranfer function: Pot: V i θ i 0 π ; Pre-Amp: V p V i K; Power Amp: E a V p 50

More information

PHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.

PHYSICS - 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 information

Driving your LED s. LED Driver. The question then is: how do we use this square wave to turn on and turn off the LED?

Driving your LED s. LED Driver. The question then is: how do we use this square wave to turn on and turn off the LED? 0//00 rng your LE.doc / rng your LE s As we hae preously learned, n optcal communcaton crcuts, a dgtal sgnal wth a frequency n the tens or hundreds of khz s used to ampltude modulate (on and off) the emssons

More information

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems

Wolfgang Hofle. CERN CAS Darmstadt, October W. Hofle feedback systems Wolfgang Hofle Wolfgang.Hofle@cern.ch CERN CAS Darmtadt, October 9 Feedback i a mechanim that influence a ytem by looping back an output to the input a concept which i found in abundance in nature and

More information

Circuits II EE221. Instructor: Kevin D. Donohue. Instantaneous, Average, RMS, and Apparent Power, and, Maximum Power Transfer, and Power Factors

Circuits 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 information

MATH 251 Examination II April 6, 2015 FORM A. Name: Student Number: Section:

MATH 251 Examination II April 6, 2015 FORM A. Name: Student Number: Section: MATH 251 Examination II April 6, 2015 FORM A Name: Student Number: Section: Thi exam ha 12 quetion for a total of 100 point. In order to obtain full credit for partial credit problem, all work mut be hown.

More information

Title 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

Title 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 information

PHYSICS - CLUTCH 1E CH 28: INDUCTION AND INDUCTANCE.

PHYSICS - 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 information

55:041 Electronic Circuits

55:041 Electronic Circuits 55:04 Electronc Crcuts Feedback & Stablty Sectons of Chapter 2. Kruger Feedback & Stablty Confguraton of Feedback mplfer S o S ε S o ( S β S ) o Negate feedback S S o + β β s the feedback transfer functon

More information

Diode. Current HmAL Voltage HVL Simplified equivalent circuit. V γ. Reverse bias. Forward bias. Designation: Symbol:

Diode. Current HmAL Voltage HVL Simplified equivalent circuit. V γ. Reverse bias. Forward bias. Designation: Symbol: Dode Materal: Desgnaton: Symbol: Poste Current flow: ptype ntype Anode Cathode Smplfed equalent crcut Ideal dode Current HmAL 0 8 6 4 2 Smplfed model 0.5.5 2 V γ eal dode Voltage HVL V γ closed open V

More information

I 2 V V. = 0 write 1 loop equation for each loop with a voltage not in the current set of equations. or I using Ohm s Law V 1 5.

I 2 V V. = 0 write 1 loop equation for each loop with a voltage not in the current set of equations. or I using Ohm s Law V 1 5. Krchoff s Laws Drect: KL, KL, Ohm s Law G G Ohm s Law: 6 (always get equaton/esor) Ω 5 Ω 6Ω 4 KL: : 5 : 5 eq. are dependent (n general, get n ndep. for nodes) KL: 4 wrte loop equaton for each loop wth

More information

Key component in Operational Amplifiers

Key component in Operational Amplifiers Key component n Operatonal Amplfers Objectve of Lecture Descrbe how dependent voltage and current sources functon. Chapter.6 Electrcal Engneerng: Prncples and Applcatons Chapter.6 Fundamentals of Electrc

More information

Physics 1202: Lecture 11 Today s Agenda

Physics 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 information