CAPACITANCE AND INDUCTANCE

Size: px
Start display at page:

Download "CAPACITANCE AND INDUCTANCE"

Transcription

1 APAITANE AND INDUTANE Inroduces wo passve, energy sorng devces: apacors and Inducors LEARNING GOALS APAITORS Sore energy n her elecrc feld (elecrosac energy) Model as crcu elemen INDUTORS Sore energy n her magnec feld Model as crcu elemen APAITOR AND INDUTOR OMBINATIONS Seres/parallel combnaons of elemens R OP-AMP IRUITS Inegraon and dfferenaon crcus

2 apacors-apacance The capacor s a passve elemen and follows he passve sgn convenon LEARNING BY DOING apacors only sore and release ELETROSTATI energy. They do no creae Lnear capacor crcu represenaon dv d

3 Q V apacance Law If he volage vares he charge vares and here s a dsplacemen curren One can also express he volage across n erms of he curren V ( ) Q ( x) dx Inegral form of apacance law Or one can express he curren hrough n erms of he volage across dq d dv d Dfferenal form of apacance law The mahemacal mplcaon of he negral form s... V ( ) V ( ); Volage across a capacor MUST be connuous Implcaons of dfferenal form?? V ons 0 D or seady sae behavor A capacor n seady sae acs as an OPEN IRUIT

4 APAITOR AS IRUIT ELEMENT v dvc d v ( x) dx v v v ( 0 ) ( x) dx ( x) dx 0 ( x) dx 0 The fac ha he volage s defned hrough an negral has mporan mplcaons... v v c ( O ) R R v R R R Ohm s Law R LEARNING EXAMPLE 5μF DETERMINE THE URRENT dv d 60mA 6 4 V 5 0 [ F ] 0mA s 0 elsewhere

5 dvc d dvc p v d d p ( ) v d w APAITOR AS ENERGY STORAGE DEVIE Insananeous power p v If s mnus nfny we alk abou energy sored a me. v (, ) v ( ) v ( ) Energy s he negral of power w (, ) p ( x) dx p v ( x) dx p q dq q d d q c d If boh lms are nfny hen we alk abou he oal energy sored. w W (, ) q ( ) q ( )

6 5μF LEARNING EXAMPLE w w Energy sored n 0-6 msec (0,6) v (6) v (0) 6 (0,6) 5*0 [ F ]*(4) [ V q harge sored a 3msec q ( 3) v (3) (3) 5*0 6 [ F]*[ V ] 60μ ] oal energy sored?... oal charge sored?... If charge s n oulombs and capacance n Farads hen he energy s n.

7 SAMPLE PROBLEM v() v 30sn (0π ) μ F WHAT VARIABLES AN BE OMPUTED? E(/ 40) q v ( (/0) Energy sored a a gven me E( ) v harge sored a a gven me ) urren hrough he capacor () 6 π *0 [ F]*30 sn 6 q *0 [ ]*sn( π )[ V ] 0 dv 6 (/0) *0 *30*0π cos( π ) d p v ( W Elecrc power suppled o capacor a a gven me ) Energy sored over a gven me nerval w(, ) v ( ) v ( ) J J A

8 A TIME VARYING MAGNETI FLUX INDUES A VOLTAGE v L dφ d Inducon law FOR A LINEAR INDUTOR THE FLUX IS PROPORTIONAL TO THE URRENT LL d DIFFERENTIAL FORM L vl L OF INDUTION LAW φ Inducors-Inducance d THE PROPORTIONALITY ONSTANT, L, IS ALLED THE INDUTANE OF THE OMPONENT LEARNING by Dong INDUTANE IS MEASURED IN UNITS OF henry (H). DIMENSIONALLY HENRY Vol Amp sec INDUTORS STORE ELETROMAGNETI ENERGY. THEY MAY SUPPLY STORED ENERGY BAK TO THE IRUIT BUT THEY ANNOT REATE ENERGY. THEY MUST ABIDE BY THE PASSIVE SIGN ONVENTION Follow passve sgn convenon

9 A drec consequence of negral form v L dl L d L( ) vl ( x) dx L L L ( L Dfferenal form of nducon law 0 ) vl ( x) dx; L A drec consequence of dfferenal forml ons. vl 0 w(, ) LL( ) LL( ) w ( ) L L L( ) Energy sored a me Mus be non-negave. Passve elemen!!! 0 Inegral form of nducon law ( ) ( ); urren MUST be connuous L Power and Energy sored dl d pl vl L W pl L L L ( ) d d L d wl(, ) LL( x) dx J urren n Amps, Inducance n Henrys d yeld energy n Joules Energy sored on he nerval an be posve or negave 0 D (seady sae) behavor

10 LEARNING EXAMPLE FIND THE TOTLA ENERGY STORED IN THE IRUIT In seady sae nducors ac as shor crcus and capacors ac as open crcus W V W LI L L V V 9 A A: 3A VA 8 [ V ] 5 I 3A I I.A L L L V 96I V 6.V L 6 V V 0.8V A 6 3 I L VA.8A 9

11 L v v

12 IDEAL AND PRATIAL ELEMENTS () () () () v() v() v() v() IDEAL ELEMENTS dv d v L d d APAITOR/INDUTOR MODELS INLUDING LEAKAGE RESISTANE v( ) dv R d leak MODEL FOR LEAKY APAITOR d v Rleak ( ) L d MODEL FOR LEAKY INDUTORS

13 SERIES APAITORS s Seres ombnaon of wo capacors 6μF μf 3 S μ F NOTIE SIMILARITY WITH RESITORS IN PARALLEL

14 LEARNING EXAMPLE DETERMINE EQUIVALENT APAITANE AND THE INITIAL VOLTAGE μ F μ F 3 6 OR WE AN REDUE TWO AT A TIME V 4V V ALGEBRAI SUM OF INITIAL VOLTAGES POLARITY IS DITATED BY THE REFERENE DIRETION FOR THE VOLTAGE

15 LEARNING EXAMPLE Two uncharged capacors are conneced as shown. Fnd he unknown capacance V 8V - 4V 30μ F FIND 8V SAME URRENT. ONNETED FOR THE SAME TIME PERIOD SAME HARGE ON BOTH APAITORS Q ( 30μ F )(8V ) 40μ Q V Q ( μf )(6V ) 7μ 7μ 8V 4μ F

16 PARALLEL APAITORS dv k d k () LEARNING EXAMPLE P μF

17 SERIES INDUTORS v d Lk d k LEARNING EXAMPLE d v LS d Leq 7H

18 PARALLEL INDUTORS () LEARNING EXAMPLE ( N 0 ) j ( 0) j INDUTORS OMBINE LIKE RESISTORS APAITORS OMBINE LIKE ONDUTANES 4mH mh ( 0 ) 3A 6A A A

19

20 R OPERATIONAL AMPLIFIER IRUITS INTRODUES TWO VERY IMPORTANT PRATIAL IRUITS BASED ON OPERATIONAL AMPLIFIERS THE IDEAL OP-AMP IDEAL RO 0, R, A R R O 0 v O A ( v v ) A

21 R OPERATIONAL AMPLIFIER IRUITS -THE INTEGRATOR v 0 v IDEAL OP-AMP ASSUMPTIONS v 0 ( A ) ( R )

22 R OPERATIONAL AMPLIFIER IRUITS - THE DIFFERENTIATOR R KVL v 0 KL@ v v : IDEAL OP-AMP ASSUMPTIONS v 0 ( A ) ( R ) R v ( x) dx d dv R d d R v O 0 DIFFERENTIATE replace n erms of v o ( v R dvo dv R vo R d d IF R OULD BE SET TO ZERO WE WOULD HAVE AN IDEAL DIFFERENTIATOR. IN PRATIE AN IDEAL DIFFERENTIATOR AMPLIFIES ELETRI NOISE AND DOES NOT OPERATE. THE RESISTOR INTRODUES A FILTERING ATION. ITS VALUE IS KEPT AS SMALL AS POSSIBLE TO APPROXIMATE A DIFFERENTIATOR o )

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore energy in heir

More information

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors LEARNING GOALS APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore

More information

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE APAITANE AND INDUTANE Inroduces wo passive, energy soring devices: apaciors and Inducors EARNING GOAS APAITORS Sore energy in heir elecric field (elecrosaic energy) Model as circui elemen INDUTORS Sore

More information

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc

A capacitor consists of two conducting plates, separated by an insulator. Conduction plates: e.g., Aluminum foil Insulator: air, mica, ceramic, etc 3//7 haper 6 apacors and Inducors Makng preparaon for dynamc crcus, whch hae far more applcaons han he sac crcus we hae learned so far. 6. apacors Sore energy n elecrc feld nsulaor onducng plaes A capacor

More information

Lecture 11 Inductance and Capacitance

Lecture 11 Inductance and Capacitance ecure Inducance and apacance EETRIA ENGINEERING: PRINIPES AND APPIATIONS, Fourh Edon, by Allan R. Hambley, 8 Pearson Educaon, Inc. Goals. Fnd he curren olage for a capacance or nducance gen he olage curren

More information

2/20/2013. EE 101 Midterm 2 Review

2/20/2013. EE 101 Midterm 2 Review //3 EE Mderm eew //3 Volage-mplfer Model The npu ressance s he equalen ressance see when lookng no he npu ermnals of he amplfer. o s he oupu ressance. I causes he oupu olage o decrease as he load ressance

More information

Energy Storage Devices

Energy Storage Devices Energy Sorage Deces Objece of Lecure Descrbe he consrucon of a capacor and how charge s sored. Inroduce seeral ypes of capacors Dscuss he elecrcal properes of a capacor The relaonshp beween charge, olage,

More information

Chapter 6: AC Circuits

Chapter 6: AC Circuits Chaper 6: AC Crcus Chaper 6: Oulne Phasors and he AC Seady Sae AC Crcus A sable, lnear crcu operang n he seady sae wh snusodal excaon (.e., snusodal seady sae. Complee response forced response naural response.

More information

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current :

10. A.C CIRCUITS. Theoretically current grows to maximum value after infinite time. But practically it grows to maximum after 5τ. Decay of current : . A. IUITS Synopss : GOWTH OF UNT IN IUIT : d. When swch S s closed a =; = d. A me, curren = e 3. The consan / has dmensons of me and s called he nducve me consan ( τ ) of he crcu. 4. = τ; =.63, n one

More information

Experiment 3: Basic Electronic Circuits II (tbc 1/7/2007)

Experiment 3: Basic Electronic Circuits II (tbc 1/7/2007) Experiment 3: Basi Eletroni iruits II (tb /7/007) Objetive: a) To study the first-order dynamis of a apaitive iruits with the appliation of Kirhoff s law, Ohm s law and apaitane formula. b) To learn how

More information

Capacitors & Inductors

Capacitors & Inductors apaciors & Inducors EEE5 Elecric ircuis Anawach Sangswang Dep. of Elecrical Engineering KMUTT Elecric Field Elecric flux densiy Elecric field srengh E Elecric flux lines always exend from a posiively charged

More information

7. Capacitors and Inductors

7. Capacitors and Inductors 7. Capaciors and Inducors 7. The Capacior The ideal capacior is a passive elemen wih circui symbol The curren-volage relaion is i=c dv where v and i saisfy he convenions for a passive elemen The capacior

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

Capacitance and Inductance. The Capacitor

Capacitance and Inductance. The Capacitor apaiane and Induane OUTINE apaiors apaior volage, urren, power, energy Induors eure 9, 9/9/5 Reading Hambley haper 3 (A) EE4 Fall 5 eure 9, Slide The apaior Two onduors (a,b) separaed by an insulaor: differene

More information

Transient Response in Electric Circuits

Transient Response in Electric Circuits Transen esponse n Elecrc rcus The elemen equaon for he branch of he fgure when he source s gven by a generc funcon of me, s v () r d r ds = r Mrs d d r (')d' () V The crcu s descrbed by he opology equaons

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

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1)

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) ECE 330 POWER CIRCUITS AND ELECTROMECHANICS LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1) Aknowledgment-These handouts and leture notes given in lass are based on material from Prof. Peter Sauer s ECE

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

Models for the simulation of electronic circuits with hysteretic inductors

Models for the simulation of electronic circuits with hysteretic inductors Proeedings of the 5th WSEAS Int. Conf. on Miroeletronis, Nanoeletronis, Optoeletronis, Prague, Czeh Republi, Marh 12-14, 26 (pp86-91) Models for the simulation of eletroni iruits with hystereti indutors

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

Chapter 16: Summary. Instructor: Jean-François MILLITHALER.

Chapter 16: Summary. Instructor: Jean-François MILLITHALER. Chaper 16: Summary Insrucor: Jean-François MILLITHALER hp://faculy.uml.edu/jeanfrancois_millihaler/funelec/spring2017 Slide 1 Curren & Charge Elecric curren is he ime rae of change of charge, measured

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

A Theorem of Mass Being Derived From Electrical Standing Waves (Adapted for a test by Jerry E. Bayles)

A Theorem of Mass Being Derived From Electrical Standing Waves (Adapted for a test by Jerry E. Bayles) EleMaEMCD A Theorem of Mass Being Derived From Eletrial Standing Waves (Adapted for a test by Jerry E Bayles) - by - Jerry E Bayles May 1, 000 This paper formalizes a onept presented in my book, "Eletrogravitation

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

2.4 Cuk converter example

2.4 Cuk converter example 2.4 Cuk converer example C 1 Cuk converer, wih ideal swich i 1 i v 1 2 1 2 C 2 v 2 Cuk converer: pracical realizaion using MOSFET and diode C 1 i 1 i v 1 2 Q 1 D 1 C 2 v 2 28 Analysis sraegy This converer

More information

Energy Storage Elements: Capacitors and Inductors

Energy Storage Elements: Capacitors and Inductors CHAPTER 6 Energy Storage Elements: Capacitors and Inductors To this point in our study of electronic circuits, time has not been important. The analysis and designs we have performed so far have been static,

More information

TRANSMISSION AND DISTRIBUTION LINES & CABLES

TRANSMISSION AND DISTRIBUTION LINES & CABLES ELEC46 Power ystem Analysis TANMON AND DTBUTON LNE & CABLE eading: hapters 4 and 5 of textbook (Glover et al). EE ETANCE Current in ondutor real power losses k = skin effet fator (.0) l = resistivity k

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

V R. Electronics and Microelectronics AE4B34EM. Electronics and Microelectronics AE4B34EM. Voltage. Basic concept. Voltage.

V R. Electronics and Microelectronics AE4B34EM. Electronics and Microelectronics AE4B34EM. Voltage. Basic concept. Voltage. Elecroncs and Mcroelecroncs AEBEM. lecure basc elecronc crcu conceps ressors, capacors, nducors Elecroncs and Mcroelecroncs AEBEM Sudng maerals: server MOODLE hp://moodle.kme.fel.cvu.cz AEBEM Elecroncs

More information

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2 Sensor and Simulation Notes Note 53 3 May 8 Combined Eletri and Magneti Dipoles for Mesoband Radiation, Part Carl E. Baum University of New Mexio Department of Eletrial and Computer Engineering Albuquerque

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

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents

EE40 Summer 2005: Lecture 2 Instructor: Octavian Florescu 1. Measuring Voltages and Currents Announemens HW # Due oday a 6pm. HW # posed online oday and due nex Tuesday a 6pm. Due o sheduling onflis wih some sudens, lasses will resume normally his week and nex. Miderm enaively 7/. EE4 Summer 5:

More information

Modes are solutions, of Maxwell s equation applied to a specific device.

Modes are solutions, of Maxwell s equation applied to a specific device. Mirowave Integrated Ciruits Prof. Jayanta Mukherjee Department of Eletrial Engineering Indian Institute of Tehnology, Bombay Mod 01, Le 06 Mirowave omponents Welome to another module of this NPTEL mok

More information

Chapter 2: Principles of steady-state converter analysis

Chapter 2: Principles of steady-state converter analysis Chaper 2 Principles of Seady-Sae Converer Analysis 2.1. Inroducion 2.2. Inducor vol-second balance, capacior charge balance, and he small ripple approximaion 2.3. Boos converer example 2.4. Cuk converer

More information

Conceptually, a capacitor consists of two conducting plates. Capacitors: Concept

Conceptually, a capacitor consists of two conducting plates. Capacitors: Concept apacitors and Inductors Overview Defining equations Key concepts and important properties Series and parallel equivalents Integrator Differentiator Portland State University EE 221 apacitors and Inductors

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

Dynamics of the Electromagnetic Fields

Dynamics of the Electromagnetic Fields Chapter 3 Dynamis of the Eletromagneti Fields 3.1 Maxwell Displaement Current In the early 1860s (during the Amerian ivil war!) eletriity inluding indution was well established experimentally. A big row

More information

ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES

ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES MISN-0-211 z ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES y È B` x ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES by J. S. Kovas and P. Signell Mihigan State University 1. Desription................................................

More information

Chapter 8 The Complete Response of RL and RC Circuits

Chapter 8 The Complete Response of RL and RC Circuits Chaper 8 he Complee Response of R and RC Ciruis Exerises Ex 8.3-1 Before he swih loses: Afer he swih loses: 2 = = 8 Ω so = 8 0.05 = 0.4 s. 0.25 herefore R ( ) Finally, 2.5 ( ) = o + ( (0) o ) = 2 + V for

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

BS7671:2008 +A3:2015 (Answers references to On-Site Guide) You may find it helpful to have a copy of BS7671:2008 +A3:2015 On-Site Guide.

BS7671:2008 +A3:2015 (Answers references to On-Site Guide) You may find it helpful to have a copy of BS7671:2008 +A3:2015 On-Site Guide. Eletrial supply systems: (Covering Outome 2 of Unit 304 Understand the priniples of internal and external earthing arrangements for eletrial installations for buildings, strutures and the environment (Level

More information

dv i= C. dt 1. Assuming the passive sign convention, (a) i = 0 (dc) (b) (220)( 9)(16.2) t t Engineering Circuit Analysis 8 th Edition

dv i= C. dt 1. Assuming the passive sign convention, (a) i = 0 (dc) (b) (220)( 9)(16.2) t t Engineering Circuit Analysis 8 th Edition . Assuming he passive sign convenion, dv i= C. d (a) i = (dc) 9 9 (b) (22)( 9)(6.2) i= e = 32.8e A 9 3 (c) i (22 = )(8 )(.) sin. = 7.6sin. pa 9 (d) i= (22 )(9)(.8) cos.8 = 58.4 cos.8 na 2. (a) C = 3 pf,

More information

Special Relativity Entirely New Explanation

Special Relativity Entirely New Explanation 8-1-15 Speial Relatiity Entirely New Eplanation Mourii Shahter mourii@gmail.om mourii@walla.o.il ISRAEL, HOLON 54-54855 Introdution In this paper I orret a minor error in Einstein's theory of Speial Relatiity,

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

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance ECE2262 Electric Circuits Chapter 6: Capacitance and Inductance Capacitors Inductors Capacitor and Inductor Combinations Op-Amp Integrator and Op-Amp Differentiator 1 CAPACITANCE AND INDUCTANCE Introduces

More information

a + b Time Domain i(τ)dτ.

a + b Time Domain i(τ)dτ. R, C, and L Elements and their v and i relationships We deal with three essential elements in circuit analysis: Resistance R Capacitance C Inductance L Their v and i relationships are summarized below.

More information

Control Systems. Mathematical Modeling of Control Systems.

Control Systems. Mathematical Modeling of Control Systems. Conrol Syem Mahemacal Modelng of Conrol Syem chbum@eoulech.ac.kr Oulne Mahemacal model and model ype. Tranfer funcon model Syem pole and zero Chbum Lee -Seoulech Conrol Syem Mahemacal Model Model are key

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

Inhomogeneous structure: Due to the fields within two guided-wave media, the microstrip does not support a pure TEM wave.

Inhomogeneous structure: Due to the fields within two guided-wave media, the microstrip does not support a pure TEM wave. Mirowave Filter Design Chp4. Transmission Lines and Components Prof. Tzong-Lin Wu Department of Eletrial Engineering National Taiwan University Mirostrip Lines Mirostrip Struture Inhomogeneous struture:

More information

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges.

Section 2.2 Charge and Current 2.6 b) The current direction is designated as the direction of the movement of positive charges. Chaper Soluions Secion. Inroducion. Curren source. Volage source. esisor.4 Capacior.5 Inducor Secion. Charge and Curren.6 b) The curren direcion is designaed as he direcion of he movemen of posiive charges..7

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

(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

Physics for Scientists & Engineers 2

Physics for Scientists & Engineers 2 Review Maxwell s Equations Physis for Sientists & Engineers 2 Spring Semester 2005 Leture 32 Name Equation Desription Gauss Law for Eletri E d A = q en Fields " 0 Gauss Law for Magneti Fields Faraday s

More information

CAPACITORS / CAPACITANCE ECET11

CAPACITORS / CAPACITANCE ECET11 APAITORS / APAITANE - apacitance - apacitor types - apacitors in series & parallel - R ircuit harging phase - R ircuit Discharging phase - R ircuit Steady State model - Source onversions - Superposition

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

Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Direct Current Motors for Sensorless Operation

Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Direct Current Motors for Sensorless Operation Amerian Journal of Applied Sienes 9 (7): 1046-1054, 2012 ISSN 1546-9239 2012 Siene Publiations Simplified Modeling, Analysis and Simulation of Permanent Magnet Brushless Diret Current Motors for Sensorless

More information

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS

DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS CHAPTER 4 DIGITAL DISTANCE RELAYING SCHEME FOR PARALLEL TRANSMISSION LINES DURING INTER-CIRCUIT FAULTS 4.1 INTRODUCTION Around the world, environmental and ost onsiousness are foring utilities to install

More information

Pre/Post Charge Control using IGBT for Relay Contact Protection in Electric Vehicle

Pre/Post Charge Control using IGBT for Relay Contact Protection in Electric Vehicle WSEAS TRANSATONS on POWER SYSTEMS Surahai Wongfookeat, Thanathai Kulworawanihpong Pre/Post har ontrol using GBT for Relay ontat Protetion in Eletri ehile Shool of Eletrial Engineering, nstitute of Engineering

More information

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data

Comparison of Alternative Equivalent Circuits of Induction Motor with Real Machine Data Comparison of Alternative Equivalent Ciruits of Indution Motor with Real Mahine Data J. radna, J. auer, S. Fligl and V. Hlinovsky Abstrat The algorithms based on separated ontrol of the motor flux and

More information

DOING PHYSICS WITH MATLAB

DOING PHYSICS WITH MATLAB DOING PHYSIS WITH MATAB THE FINITE DIFFERENE METHOD FOR THE NUMERIA ANAYSIS OF IRUITS ONTAINING RESISTORS, APAITORS AND INDUTORS MATAB DOWNOAD DIRETORY N01.m Voltage and current for a resistor, capacitor

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

Class XII - Physics Electromagnetic Waves Chapter-wise Problems

Class XII - Physics Electromagnetic Waves Chapter-wise Problems Class XII - Physis Eletromagneti Waves Chapter-wise Problems Multiple Choie Question :- 8 One requires ev of energy to dissoiate a arbon monoxide moleule into arbon and oxygen atoms The minimum frequeny

More information

Example: MOSFET Amplifier Distortion

Example: MOSFET Amplifier Distortion 4/25/2011 Example MSFET Amplfer Dsoron 1/9 Example: MSFET Amplfer Dsoron Recall hs crcu from a prevous handou: ( ) = I ( ) D D d 15.0 V RD = 5K v ( ) = V v ( ) D o v( ) - K = 2 0.25 ma/v V = 2.0 V 40V.

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

Unit 2: Modeling in the Frequency Domain. Unit 2, Part 4: Modeling Electrical Systems. First Example: Via DE. Resistors, Inductors, and Capacitors

Unit 2: Modeling in the Frequency Domain. Unit 2, Part 4: Modeling Electrical Systems. First Example: Via DE. Resistors, Inductors, and Capacitors Unit 2: Modeling in the Frequency Domain Part 4: Modeling Electrical Systems Engineering 582: Control Systems I Faculty of Engineering & Applied Science Memorial University of Newfoundland January 20,

More information

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

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

More information

Linear Circuit Elements

Linear Circuit Elements 1/25/2011 inear ircui Elemens.doc 1/6 inear ircui Elemens Mos microwave devices can be described or modeled in erms of he hree sandard circui elemens: 1. ESISTANE () 2. INDUTANE () 3. APAITANE () For he

More information

Lecture #4 Capacitors and Inductors Energy Stored in C and L Equivalent Circuits Thevenin Norton

Lecture #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 information

( ) () we define the interaction representation by the unitary transformation () = ()

( ) () we define the interaction representation by the unitary transformation () = () Hgher Order Perurbaon Theory Mchael Fowler 3/7/6 The neracon Represenaon Recall ha n he frs par of hs course sequence, we dscussed he chrödnger and Hesenberg represenaons of quanum mechancs here n he chrödnger

More information

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance ECE2262 Electric Circuits Chapter 6: Capacitance and Inductance Capacitors Inductors Capacitor and Inductor Combinations 1 CAPACITANCE AND INDUCTANCE Introduces two passive, energy storing devices: Capacitors

More information

Experimental Buck Converter

Experimental Buck Converter Experimenal Buck Converer Inpu Filer Cap MOSFET Schoky Diode Inducor Conroller Block Proecion Conroller ASIC Experimenal Synchronous Buck Converer SoC Buck Converer Basic Sysem S 1 u D 1 r r C C R R X

More information

3. Alternating Current

3. Alternating Current 3. Alernaing Curren TOPCS Definiion and nroducion AC Generaor Componens of AC Circuis Series LRC Circuis Power in AC Circuis Transformers & AC Transmission nroducion o AC The elecric power ou of a home

More information

FREE Download Study Package from website: &

FREE Download Study Package from website:  & EXERISE- * MARK IS MORE THAN ONE ORRET QUESTIONS. SETION A : DEFINITION OF APAIT ITANE A. A. When 0µ charge is given to an isolated conductor of capacitance 5µF. Find out following (i) Potential of the

More information

BME/ISE 3511 Bioelectronics - Test Six Course Notes Fall 2016

BME/ISE 3511 Bioelectronics - Test Six Course Notes Fall 2016 BME/ISE 35 Bioelectronics - Test Six ourse Notes Fall 06 Alternating urrent apacitive & Inductive Reactance and omplex Impedance R & R ircuit Analyses (D Transients, Time onstants, Steady State) Electrical

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 10 INDUCTANCE Recommended Problems:

Chapter 10 INDUCTANCE Recommended Problems: Chaper 0 NDUCTANCE Recommended Problems: 3,5,7,9,5,6,7,8,9,,,3,6,7,9,3,35,47,48,5,5,69, 7,7. Self nducance Consider he circui shown in he Figure. When he swich is closed, he curren, and so he magneic field,

More information

Directional Coupler. 4-port Network

Directional Coupler. 4-port Network Diretional Coupler 4-port Network 3 4 A diretional oupler is a 4-port network exhibiting: All ports mathed on the referene load (i.e. S =S =S 33 =S 44 =0) Two pair of ports unoupled (i.e. the orresponding

More information

First Order RC and RL Transient Circuits

First Order RC and RL Transient Circuits First Order R and RL Transient ircuits Objectives To introduce the transients phenomena. To analyze step and natural responses of first order R circuits. To analyze step and natural responses of first

More information

ELECTRONICS E # 1 FUNDAMENTALS 2/2/2011

ELECTRONICS E # 1 FUNDAMENTALS 2/2/2011 FE Review 1 ELECTRONICS E # 1 FUNDAMENTALS Electric Charge 2 In an electric circuit it there is a conservation of charge. The net electric charge is constant. There are positive and negative charges. Like

More information

CAPACITANCE. Capacitor. Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized.

CAPACITANCE. Capacitor. Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized. D ircuits APAITANE APAITANE Because of the effect of capacitance, an electrical circuit can store energy, even after being de-energized. EO 1.5 EO 1.6 EO 1.7 EO 1.8 EO 1.9 DESRIBE the construction of a

More information

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product

- If one knows that a magnetic field has a symmetry, one may calculate the magnitude of B by use of Ampere s law: The integral of scalar product 11.1 APPCATON OF AMPEE S AW N SYMMETC MAGNETC FEDS - f one knows ha a magneic field has a symmery, one may calculae he magniude of by use of Ampere s law: The inegral of scalar produc Closed _ pah * d

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

ELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW. P. М. Меdnis

ELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW. P. М. Меdnis ELECTROMAGNETIC WAVES WITH NONLINEAR DISPERSION LAW P. М. Меdnis Novosibirs State Pedagogial University, Chair of the General and Theoretial Physis, Russia, 636, Novosibirs,Viljujsy, 8 e-mail: pmednis@inbox.ru

More information

Lesson 2 Transmission Lines Fundamentals

Lesson 2 Transmission Lines Fundamentals Lesson Transmsson Lnes Funamenals 楊尚達 Shang-Da Yang Insue of Phooncs Technologes Deparmen of Elecrcal Engneerng Naonal Tsng Hua Unersy Tawan Sec. -1 Inroucon 1. Why o scuss TX lnes srbue crcus?. Crera

More information

Circuit Analysis-II. Circuit Analysis-II Lecture # 5 Monday 23 rd April, 18

Circuit Analysis-II. Circuit Analysis-II Lecture # 5 Monday 23 rd April, 18 Circuit Analysis-II Capacitors in AC Circuits Introduction ü The instantaneous capacitor current is equal to the capacitance times the instantaneous rate of change of the voltage across the capacitor.

More information

TUTORIAL SOLUTIONS. F.1 KCL, KVL, Power and Energy Q.1. i All units in VAΩ,,

TUTORIAL SOLUTIONS. F.1 KCL, KVL, Power and Energy Q.1. i All units in VAΩ,, F TUTOIAL SOLUTIONS F. KCL, KVL, Power and Energy Q. 8 9 6 All uns n VAΩ,, Appendx F Tuoral Soluons Applyng KCL o he doed surface: + + Q. All uns n V, A, Ω Nework A Nework B Applyng KCL o he doed surface:

More information

The simulation analysis of the bridge rectifier continuous operation in AC circuit

The simulation analysis of the bridge rectifier continuous operation in AC circuit Computer Appliations in Eletrial Engineering Vol. 4 6 DOI 8/j.8-448.6. The simulation analysis of the bridge retifier ontinuous operation in AC iruit Mirosław Wiślik, Paweł Strząbała Kiele University of

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

1 pasted at the origin. You have to apply an inward force to push the q. ( r) q :

1 pasted at the origin. You have to apply an inward force to push the q. ( r) q : letromagneti Theory (MT) Prof Ruiz, UNC Asheville, dotorphys on YouTube Chapter U Notes nergy U nergy in an letri Field ring a harge q to a distane r away from q Consider the two harges positive and q

More information

The RLC circuits have a wide range of applications, including oscillators and frequency filters

The RLC circuits have a wide range of applications, including oscillators and frequency filters 9. The RL ircuit The RL circuits have a wide range of applications, including oscillators and frequency filters This chapter considers the responses of RL circuits The result is a second-order differential

More information

Special Relativity Electromagnetic and Gravitation combined Into one theory

Special Relativity Electromagnetic and Gravitation combined Into one theory --5 Speial Relatiity Eletromagneti and Graitation ombined Into one theory Mourii Shahter mourii@gmail.om mourii@walla.o.il ISRAE, HOON 54-54855 Introdution In this paper, I try to ombine Eletromagneti

More information

The homopolar generator: an analytical example

The homopolar generator: an analytical example The homopolar generator: an analytial example Hendrik van Hees August 7, 214 1 Introdution It is surprising that the homopolar generator, invented in one of Faraday s ingenious experiments in 1831, still

More information

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: June 12, E Main Suite D Pullman, WA (509) Voice and Fax .: apacors Reson: June, 5 E Man Sue D Pullman, WA 9963 59 334 636 Voce an Fax Oerew We begn our suy of energy sorage elemens wh a scusson of capacors. apacors, lke ressors, are passe wo-ermnal crcu elemens.

More information

Capacitors. C d. An electrical component which stores charge. parallel plate capacitor. Scale in cm

Capacitors. C d. An electrical component which stores charge. parallel plate capacitor. Scale in cm apaciors An elecrical componen which sores charge E 2 2 d A 2 parallel plae capacior Scale in cm Leyden Jars I was invened independenly by German cleric Ewald Georg von Kleis on Ocober 745 and by Duch

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

AP Physics C. Electricity and Magne4sm Review

AP Physics C. Electricity and Magne4sm Review AP Physics C Electricity and Magne4sm Review Electrosta4cs 30% Chap 22-25 Charge and Coulomb s Law Electric Field and Electric Poten4al (including point charges) Gauss Law Fields and poten4als of other

More information

General Closed-form Analytical Expressions of Air-gap Inductances for Surfacemounted Permanent Magnet and Induction Machines

General Closed-form Analytical Expressions of Air-gap Inductances for Surfacemounted Permanent Magnet and Induction Machines General Closed-form Analytial Expressions of Air-gap Indutanes for Surfaemounted Permanent Magnet and Indution Mahines Ronghai Qu, Member, IEEE Eletroni & Photoni Systems Tehnologies General Eletri Company

More information

To determine the biasing conditions needed to obtain a specific gain each stage must be considered.

To determine the biasing conditions needed to obtain a specific gain each stage must be considered. PHYSIS 56 Experiment 9: ommon Emitter Amplifier A. Introdution A ommon-emitter oltage amplifier will be tudied in thi experiment. You will inetigate the fator that ontrol the midfrequeny gain and the low-and

More information

Physics Electricity and Magnetism Lecture 06 - Capacitance. Y&F Chapter 24 Sec. 1-6

Physics Electricity and Magnetism Lecture 06 - Capacitance. Y&F Chapter 24 Sec. 1-6 Physics - lectricity and Magnetism Lecture 6 - apacitance Y&F hapter 4 Sec. - 6 Overview Definition of apacitance alculating the apacitance Parallel Plate apacitor Spherical and ylindrical apacitors apacitors

More information

Chapter 6 Objectives

Chapter 6 Objectives hapter 6 Engr8 ircuit Analysis Dr urtis Nelson hapter 6 Objectives Understand relationships between voltage, current, power, and energy in inductors and capacitors; Know that current must be continuous

More information