DC and AC Impedance of Reactive Elements

Similar documents
Single Phase Parallel AC Circuits

Frequency Bands. ω the numeric value of G ( ω ) depends on the frequency ω of the basis

AC analysis - many examples

REACTANCE. By: Enzo Paterno Date: 03/2013

AC Circuits Homework Set

Sinusoidal Response of RLC Circuits

Unit 21 Capacitance in AC Circuits

Consider a simple RC circuit. We might like to know how much power is being supplied by the source. We probably need to find the current.

Electronics. Basics & Applications. group talk Daniel Biesinger

EE221 Circuits II. Chapter 14 Frequency Response

MODULE-4 RESONANCE CIRCUITS

INTC 1307 Instrumentation Test Equipment Teaching Unit 6 AC Bridges

EE313 Fall 2013 Exam #1 (100 pts) Thursday, September 26, 2013 Name. 1) [6 pts] Convert the following time-domain circuit to the RMS Phasor Domain.

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

R-L-C Circuits and Resonant Circuits

EE221 Circuits II. Chapter 14 Frequency Response

EE221 - Practice for the Midterm Exam

Handout 11: AC circuit. AC generator

ELEC 2501 AB. Come to the PASS workshop with your mock exam complete. During the workshop you can work with other students to review your work.

Switched Mode Power Conversion

1 Phasors and Alternating Currents

SINUSOIDAL STEADY STATE CIRCUIT ANALYSIS

Solution: K m = R 1 = 10. From the original circuit, Z L1 = jωl 1 = j10 Ω. For the scaled circuit, L 1 = jk m ωl 1 = j10 10 = j100 Ω, Z L

mywbut.com Lesson 16 Solution of Current in AC Parallel and Seriesparallel

Module 4. Single-phase AC circuits. Version 2 EE IIT, Kharagpur

Prof. Anyes Taffard. Physics 120/220. Voltage Divider Capacitor RC circuits

CHAPTER 22 ELECTROMAGNETIC INDUCTION

RLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance:

ELECTROMAGNETIC OSCILLATIONS AND ALTERNATING CURRENT

Physics 1c practical, 2015 Homework 5 Solutions

Lecture 4: R-L-C Circuits and Resonant Circuits

Chapter 2 Circuit Elements

Power Factor Improvement

Electric Circuits I Final Examination

rms high f ( Irms rms low f low f high f f L

ENGR-4300 Spring 2009 Test 2. Name: SOLUTION. Section: 1(MR 8:00) 2(TF 2:00) 3(MR 6:00) (circle one) Question I (20 points): Question II (20 points):

Two-Port Networks Admittance Parameters CHAPTER16 THE LEARNING GOALS FOR THIS CHAPTER ARE THAT STUDENTS SHOULD BE ABLE TO:

BME/ISE 3511 Bioelectronics - Test Five Review Notes Fall 2015

Phasors: Impedance and Circuit Anlysis. Phasors

Filters and Tuned Amplifiers

Stepped-Impedance Low-Pass Filters

Impedance and Loudspeaker Parameter Measurement

EXP. NO. 3 Power on (resistive inductive & capacitive) load Series connection

Designing Information Devices and Systems II Fall 2018 Elad Alon and Miki Lustig Discussion 5A

Sinusoidal Steady State Analysis (AC Analysis) Part I

LOW & HIGH RESISTANCE MEASUREMENTS and A.C. BRIDGES

EXPERIMENT 07 TO STUDY DC RC CIRCUIT AND TRANSIENT PHENOMENA

ECE 524: Reducing Capacitor Switching Transients

Sinusoidal Steady-State Analysis

ECE 524: Lecture 15 Reducing Capacitor Switching Transients. jx s C 2 C 1. Define units: MW 1000kW MVA MW MVAr MVA. rad s

Annexure-I. network acts as a buffer in matching the impedance of the plasma reactor to that of the RF

Radio Frequency Electronics

Alternating Current Circuits. Home Work Solutions

AC Circuit Analysis and Measurement Lab Assignment 8

PHYS 241 EXAM #2 November 9, 2006

6.1 Introduction

To investigate further the series LCR circuit, especially around the point of minimum impedance. 1 Electricity & Electronics Constructor EEC470


Review of DC Electric Circuit. DC Electric Circuits Examples (source:

RLC Circuit (3) We can then write the differential equation for charge on the capacitor. The solution of this differential equation is

Lecture 15. LC Circuit. LC Oscillation - Qualitative. LC Oscillator

Alternating Current Circuits

Electric Circuits I Final Examination

Physics 142 AC Circuits Page 1. AC Circuits. I ve had a perfectly lovely evening but this wasn t it. Groucho Marx

Sinusoidal Steady-State Analysis

FUNDAMENTALS. Introduction. 1.1 Electric Signals. Chapter 1

CHAPTER 5 DC AND AC BRIDGE

The general form for the transform function of a second order filter is that of a biquadratic (or biquad to the cool kids).

ELECTRO MAGNETIC INDUCTION

Ver 3537 E1.1 Analysis of Circuits (2014) E1.1 Circuit Analysis. Problem Sheet 1 (Lectures 1 & 2)

Lecture 24. Impedance of AC Circuits.

EE292: Fundamentals of ECE

Lecture 6: Impedance (frequency dependent. resistance in the s- world), Admittance (frequency. dependent conductance in the s- world), and

Pre-Lab. Introduction

Refinements to Incremental Transistor Model

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

Module 4. Single-phase AC Circuits. Version 2 EE IIT, Kharagpur 1

EE 205 Dr. A. Zidouri. Electric Circuits II. Frequency Selective Circuits (Filters) Low Pass Filter. Lecture #36

'XNH8QLYHUVLW\ (GPXQG73UDWW-U6FKRRORI(QJLQHHULQJ. EGR 224 Spring Test II. Michael R. Gustafson II

Chapter 3: Capacitors, Inductors, and Complex Impedance

Schedule. ECEN 301 Discussion #20 Exam 2 Review 1. Lab Due date. Title Chapters HW Due date. Date Day Class No. 10 Nov Mon 20 Exam Review.

Resonant Matching Networks

AC Source and RLC Circuits

Dynamic circuits: Frequency domain analysis

Experiment 3: Resonance in LRC Circuits Driven by Alternating Current

Chapter 6 Objectives

11. AC Circuit Power Analysis

The Transmission Line Wave Equation

Electromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.

Homework 2 SJTU233. Part A. Part B. Problem 2. Part A. Problem 1. Find the impedance Zab in the circuit seen in the figure. Suppose that R = 5 Ω.

Test II Michael R. Gustafson II

Learnabout Electronics - AC Theory

analyse and design a range of sine-wave oscillators understand the design of multivibrators.

Mutual Inductance: This is the magnetic flux coupling of 2 coils where the current in one coil causes a voltage to be induced in the other coil.

FINAL EXAM - Physics Patel SPRING 1998 FORM CODE - A

SCHOOL OF MATHEMATICS MATHEMATICS FOR PART I ENGINEERING. Self-paced Course

'XNH8QLYHUVLW\ (GPXQG73UDWW-U6FKRRORI(QJLQHHULQJ. ECE 110 Fall Test II. Michael R. Gustafson II

EE292: Fundamentals of ECE

'XNH8QLYHUVLW\ (GPXQG73UDWW-U6FKRRORI(QJLQHHULQJ. EGR 224 Spring Test II. Michael R. Gustafson II

Experiment 9 Equivalent Circuits

Transcription:

3/6/20 D and A Impedance of Reactive Elements /6 D and A Impedance of Reactive Elements Now, recall from EES 2 the complex impedances of our basic circuit elements: ZR = R Z = jω ZL = jωl For a D signal ( ω = 0), we find that: ZR = R Z = lim = ω 0 jω Z = j(0) L = 0 L Thus, at D we know that: * a capacitor acts as an open circuit (I =0). * an inductor acts as a short circuit (V L = 0).

3/6/20 D and A Impedance of Reactive Elements 2/6 Now, let s consider two important cases:. A capacitor whose capacitance is unfathomably large. 2. An inductor whose inductance L is unfathomably large.. The Unfathomably Large apacitor In this case, we consider a capacitor whose capacitance is finite, but very, very, very large. For D signals ( ω = 0), this device acts still acts like an open circuit. However, now consider the A signal case (e.g., a small signal), where ω 0. The impedance of an unfathomably large capacitor is: Zero impedance! Z = lim = 0 jω An unfathomably large capacitor acts like an A short.

3/6/20 D and A Impedance of Reactive Elements 3/6 Quite a trick! The unfathomably large capacitance acts like an open to D signals, but likewise acts like a short to A (small) signals! + v ( t) = 0 c I = 0 = lim Q: I fail to see the relevance of this analysis at this juncture. After all, unfathomably large capacitors do not exist, and are impossible to make (being unfathomable and all). A: True enough! However, we can make very big (but fathomably large) capacitors. Big capacitors will not act as a perfect A short circuit, but will exhibit an impedance of very small magnitude (e.g., a few Ohms), provided that the A signal frequency is sufficiently large. In this way, a very large capacitor acts as an approximate A short, and as a perfect D open.

3/6/20 D and A Impedance of Reactive Elements 4/6 We call these large capacitors D blocking capacitors, as they allow no D current to flow through them, while allowing A current to flow nearly unimpeded! Q: But you just said this is true provided that the A signal frequency is sufficiently large. Just how large does the signal frequency ω need to be? A: Say we desire the A impedance of our capacitor to have a magnitude of less than ten Ohms: Z < 0 Rearranging, we find that this will occur if the frequency ω is: 0 > Z 0 > ω ω > 0 For example, a 50 µf capacitor will exhibit an impedance whose magnitude is less than 0 Ohms for all A signal frequencies above 320 Hz.

3/6/20 D and A Impedance of Reactive Elements 5/6 Likewise, almost all A signals in modern electronics will operate in a spectrum much higher than 320 Hz. Thus, a 50 µf blocking capacitor will approximately act as an A short and (precisely) act as a D open. 2. The Unfathomably Large Inductor Similarly, we can consider an unfathomably large inductor. In addition to a D impedance of zero (a D short), we find for the A case (where ω 0): Z = lim jωl = L L In other words, an unfathomably large inductor acts like an A open circuit! V + = 0 i ( t ) = 0 L = lim L L The unfathomably large inductor acts like an short to D signals, but likewise acts like an open to A (small) signals!

3/6/20 D and A Impedance of Reactive Elements 6/6 As before, an unfathomably large inductor is impossible to build. However, a very large inductor will typically exhibit a very large A impedance for all but the lowest of signal frequencies ω. We call these large inductors A chokes (also known RF chokes), as they act as a perfect short to D signals, yet so effectively impede A signals (with sufficiently high frequency) that they act approximately as an A open circuit. For example, if we desire an A choke with an impedance magnitude greater than 00 kω, we find that: Z L > 0 5 ωl > 0 5 ω > 5 0 L Thus, an A choke of 50 mh would exhibit an impedance magnitude of greater than 00 kω for all signal frequencies greater than 320 khz. Note that this is still a fairly low signal frequency for many modern electronic applications, and thus this inductor would be an adequate A choke. Note however, that building and A choke for audio signals (20 Hz to 20 khz) is typically very difficult!