CAPACITANCE AND INDUCTANCE

Similar documents
CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE

CAPACITANCE AND INDUCTANCE

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

Lecture 11 Inductance and Capacitance

2/20/2013. EE 101 Midterm 2 Review

Energy Storage Devices

Chapter 6: AC Circuits

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

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

Capacitors & Inductors

7. Capacitors and Inductors

First Order RC and RL Transient Circuits

Capacitance and Inductance. The Capacitor

Transient Response in Electric Circuits

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

LECTURE 5 PER-PHASE CIRCUITS AND MAGNETICS (1)

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

Models for the simulation of electronic circuits with hysteretic inductors

INDEX. Transient analysis 1 Initial Conditions 1

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

Chapter 7 Response of First-order RL and RC Circuits

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

ES 250 Practice Final Exam

2.4 Cuk converter example

Energy Storage Elements: Capacitors and Inductors

TRANSMISSION AND DISTRIBUTION LINES & CABLES

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

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

Combined Electric and Magnetic Dipoles for Mesoband Radiation, Part 2

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

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

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

Chapter 2: Principles of steady-state converter analysis

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

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

Dynamics of the Electromagnetic Fields

ENERGY AND MOMENTUM IN ELECTROMAGNETIC WAVES

Chapter 8 The Complete Response of RL and RC Circuits

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

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.

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

Special Relativity Entirely New Explanation

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

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance

a + b Time Domain i(τ)dτ.

Control Systems. Mathematical Modeling of Control Systems.

Basic Circuit Elements Professor J R Lucas November 2001

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

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

Chapter 4 AC Network Analysis

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

Physics for Scientists & Engineers 2

CAPACITORS / CAPACITANCE ECET11

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

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

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

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

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

DOING PHYSICS WITH MATLAB

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

Class XII - Physics Electromagnetic Waves Chapter-wise Problems

Example: MOSFET Amplifier Distortion

CHAPTER 6: FIRST-ORDER CIRCUITS

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

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

Linear Circuit Elements

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

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

ECE2262 Electric Circuits. Chapter 6: Capacitance and Inductance

Experimental Buck Converter

3. Alternating Current

FREE Download Study Package from website: &

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

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

Chapter 10 INDUCTANCE Recommended Problems:

Directional Coupler. 4-port Network

First Order RC and RL Transient Circuits

ELECTRONICS E # 1 FUNDAMENTALS 2/2/2011

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

- 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

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

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

Lesson 2 Transmission Lines Fundamentals

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

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

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

EE100 Lab 3 Experiment Guide: RC Circuits

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

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

Special Relativity Electromagnetic and Gravitation combined Into one theory

The homopolar generator: an analytical example

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

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

EEEB113 CIRCUIT ANALYSIS I

AP Physics C. Electricity and Magne4sm Review

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

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

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

Chapter 6 Objectives

Transcription:

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

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

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

APAITOR AS IRUIT ELEMENT v dvc d v ( x) dx v v 0 0 0 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 3 6 0 s 0 elsewhere

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 ( )

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.

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

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

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

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 @ A: 3A 0 9 6 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

L v v

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

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

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

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

PARALLEL APAITORS dv k d k () LEARNING EXAMPLE P 4 6 3 5μF

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

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

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

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

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 )