Review of Electrical Filters
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Electrical Circuits Lab. 0903219 Series RC Circuit Phasor Diagram
Electrical Circuits Lab. 0903219 Series RC Circuit Phasor Diagram - Simple steps to draw phasor diagram of a series RC circuit without memorizing: * Start with the quantity (voltage or current) that is common for the resistor R and the capacitor C, which is here the source current I (because it passes through both R and C without being divided). Figure (1) Series RC circuit * Now we know that I and resistor voltage VR are in phase or have the same phase angle (there zero crossings are the same on the time axis) and VR is greater than I in magnitude. * Since I equal the capacitor current IC and we know that IC leads the capacitor voltage VC by 90 degrees, we will add VC on the phasor diagram as follows: * Now, the source voltage VS equals the vector summation of VR and VC: Figure (2) Series RC circuit Phasor Diagram Prepared by: Eng. Wiam Anabousi - Important notes on the phasor diagram of series RC circuit shown in figure (2): A- All the vectors are rotating in the same angular speed ω. B- This circuit acts as a capacitive circuit and I leads VS by a phase shift of Ө (which is the current angle if the source voltage is the reference signal). Ө ranges from 0o to 90o (0o < Ө <90o). If Ө=0o then this circuit becomes a resistive circuit and if Ө=90o then the circuit becomes a pure capacitive circuit. C- The phase shift between the source voltage and its current Ө is important and you have two ways to find its value: a- b- = - = - D- Using the phasor diagram, you can find all needed quantities in the circuit like all the voltages magnitude and phase and all the currents magnitude and phase. -
C I L Q LC Circuit
Your Comments I am not feeling great about this midterm...some of this stuff is really confusing still and I don't know if I can shove everything into my brain in time, especially after spring break. Can you go over which topics will be on the exam Wednesday? This was a very confusing prelecture. Do you think you could go over thoroughly how the LC circuits work qualitatively? I may have missed something simple, but in question 1 during the prelecture why does the charge on the capacitor have to be 0 at t=0? I feel like that bit of knowledge will help me with the test wednesday I remember you mentioning several weeks ago that there was one equation you were going to add to the 2013 equation sheet... which formula was that? Thanks! Electricity & Magnetism Lecture 19, Slide 1 Some Exam Stuff Exam Wed. night (March 27th) at 7:00 Covers material in Lectures 9 – 18 Bring your ID: Rooms determined by discussion section (see link) Conflict exam at 5:15 Don’t forget: • Worked examples in homeworks (the optional questions) • Other old exams For most people, taking old exams is most beneficial Final Exam dates are now posted The Big Ideas L9-18 Kirchoff’s Rules Sum of voltages around a loop is zero Sum of currents into a node is zero Kirchoff’s rules with capacitors and inductors • In RC and RL circuits: charge and current involve exponential functions with time constant: “charging and discharging” Q dQ Q • E.g. IR R V C dt C Capacitors and inductors store energy Magnetic fields Generated by electric currents (no magnetic charges) Magnetic -
Damping of Ringing in Audio Transformers 22.1.12
Damping of ringing in audio transformers 22.1.12. 11.50 Damping Ringing in LC Circuits First edition 01/19/01 Damping a circuit is to reduce the ringing in it. Dampening a circuit is to throw a wet towel on it (probably because it is on fire and you just got done pulling the wall plug.) Star Trek is not the same any more once I had the difference pointed out to me that way. I can't keep a straight face when the say "put a dampening field on the Klingon vessel". What are they trying to do? Everybody knows Klingons don't like being wet so they are going to throw a field of wet blankets on them. No wonder they always react so violently to the dampening field. Overview of Damping Overshoot and ringing in a circuit is caused by having an under damped two or more pole network. This is an L and a C in a passive network, two L's in a feedback network or two C's in a feedback network. The feedback network can be intentional (feedback in an amp) or unintentional (parasitics.) There are many ways to reduce overshoot. They all rely on removing energy from the tank that is ringing at the ringing frequency. If you remove energy at frequencies other than the ringing frequency, you'll have a loss in gain and/or efficiency of the circuit. Even thought this page isn't a full dissertation on damping, it should get you started with the concept of RC damping. -
Phasor Analysis of Circuits
Phasor Analysis of Circuits Concepts Frequency-domain analysis of a circuit is useful in understanding how a single-frequency wave undergoes an amplitude change and phase shift upon passage through the circuit. The concept of impedance or reactance is central to frequency-domain analysis. For a resistor, the impedance is Z ω = R , a real quantity independent of frequency. For capacitors and R ( ) inductors, the impedances are Z ω = − i ωC and Z ω = iω L. In the complex plane C ( ) L ( ) these impedances are represented as the phasors shown below. Im ivL R Re -i/vC These phasors are useful because the voltage across each circuit element is related to the current through the equation V = I Z . For a series circuit where the same current flows through each element, the voltages across each element are proportional to the impedance across that element. Phasor Analysis of the RC Circuit R V V in Z in Vout R C V ZC out The behavior of this RC circuit can be analyzed by treating it as the voltage divider shown at right. The output voltage is then V Z −i ωC out = C = . V Z Z i C R in C + R − ω + The amplitude is then V −i 1 1 out = = = , V −i +ω RC 1+ iω ω 2 in c 1+ ω ω ( c ) 1 where we have defined the corner, or 3dB, frequency as 1 ω = . c RC The phasor picture is useful to determine the phase shift and also to verify low and high frequency behavior. The input voltage is across both the resistor and the capacitor, so it is equal to the vector sum of the resistor and capacitor voltages, while the output voltage is only the voltage across capacitor. -
Transmission of Stereo Audio Signals with Lasers William Austin Curbow University of Arkansas, Fayetteville
University of Arkansas, Fayetteville ScholarWorks@UARK Electrical Engineering Undergraduate Honors Electrical Engineering Theses 5-2014 Transmission of Stereo Audio Signals with Lasers William Austin Curbow University of Arkansas, Fayetteville Follow this and additional works at: http://scholarworks.uark.edu/eleguht Part of the Signal Processing Commons Recommended Citation Curbow, William Austin, "Transmission of Stereo Audio Signals with Lasers" (2014). Electrical Engineering Undergraduate Honors Theses. 31. http://scholarworks.uark.edu/eleguht/31 This Thesis is brought to you for free and open access by the Electrical Engineering at ScholarWorks@UARK. It has been accepted for inclusion in Electrical Engineering Undergraduate Honors Theses by an authorized administrator of ScholarWorks@UARK. For more information, please contact [email protected], [email protected]. Dr. Jingxian Wu Transmission of Stereo Audio Signals with Lasers An Undergraduate Honors College Thesis in the Department of Electrical Engineering College of Engineering University of Arkansas Fayetteville, AR by William Austin Curbow TABLE OF CONTENTS I. ABSTRACT ............................................................................................................................ 1 II. INTRODUCTION ............................................................................................................... 2 III. THEORETICAL BACKGROUND ..................................................................................... 3 IV. DESIGN PROCEDURE ..................................................................................................... -
Analysis of Magnetic Resonance in Metamaterial Structure
Analysis of magnetic resonance in Metamaterial structure Rajni#1, Anupma Marwaha#2 #1 Asstt. Prof. Shaheed Bhagat Singh College of Engg. And Technology,Ferozepur(Pb.)(India), #2 Assoc. Prof., Sant Longowal Institute of Engg. And Technology,Sangrur(Pb.)(India) [email protected] 2 [email protected] Abstract: ‘Metamaterials’ is one of the most 1. Introduction recent topics in several areas of science and technology due to its vast potential in various Metamaterials are artificial materials synthesized applications. These are artificially fabricated by embedding specific inclusions like periodic materials which exhibit negative permittivity structures in host media. These materials have and/or negative permeability. The unusual the unique property of negative permittivity electromagnetic properties of metamaterial and/or negative permeability not encountered in have opened more opportunities for better the nature. If materials have both parameters antenna design to surmount the limitations of negative at the same time, then they exhibit an conventional antennas. Metamaterials have effective negative index of refraction and are created many designs in a broad frequency referred to as Left-Handed Metamaterials spectrum from microwave to millimeter wave (LHM). This name is given to these materials to optical structures. The edifice building because the electric field, magnetic field and the blocks of metamaterials are synthetically wave vector form a left-handed system. These fabricated periodic structures of having materials offer a new dimension to the antenna lattice constants smaller than the wavelength applications. The phase velocity and group of the incident radiation. Thus metamaterial velocity in these materials are anti-parallel to properties can be controlled by the design of each other i.e. -
Network Analysis
LECTURE NOTES ON NETWORK ANALYSIS B. Tech III Semester (IARE-R18) Ms. S Swathi Asistant professor ELECTRICAL AND ELECTRONICS ENGINEERING INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) DUNDIGAL, HYDERABAD - 50043 1 SYLLABUS MODULE-I NETWORK THEOREMS (DC AND AC) Network Theorems: Tellegen‘s, superposition, reciprocity, Thevenin‘s, Norton‘s, maximum power transfer, Milliman‘s and compensation theorems for DC and AC excitations, numerical problems. MODULE-II SOLUTION OF FIRST AND SECOND ORDER NETWORKS Transient response: Initial conditions, transient response of RL, RC and RLC series and parallel circuits with DC and AC excitations, differential equation and Laplace transform approach. MODULE-III LOCUS DIAGRAMS AND NETWORKS FUNCTIONS Locus diagrams: Locus diagrams of RL, RC, RLC circuits. Network Functions: The concept of complex frequency, physical interpretation, transform impedance, series and parallel combination of elements, terminal ports, network functions for one port and two port networks, poles and zeros of network functions, significance of poles and zeros, properties of driving point functions and transfer functions, necessary conditions for driving point functions and transfer functions, time domain response from pole-zero plot. MODULE-IV TWO PORTNETWORK PARAMETERS Two port network parameters: Z, Y, ABCD, hybrid and inverse hybrid parameters, conditions for symmetry and reciprocity, inter relationships of different parameters, interconnection (series, parallel and cascade) of two port networks, image parameters. MODULE-V FILTERS Filters: Classification of filters, filter networks, classification of pass band and stop band, characteristic impedance in the pass and stop bands, constant-k low pass filter, high pass filter, m- derived T-section, band pass filter and band elimination filter. Text Books: 1. -
Tpa324x and Tpa325x Post-Filter Feedback (Rev. A)
Application Report SLAA788A–September 2017–Revised March 2018 TPA324x and TPA325x Post-Filter Feedback Dan Kisling, Matthew Beardsworth ABSTRACT The TPA324x and TPA325x (TPA3244, TPA3245, TPA3250, TPA3251, TPA3255) Class-D audio amplifier families deliver high audio performance with less than 0.01% total harmonic distortion and noise (THD+N) to clipping. The high level of audio performance makes this device an ideal candidate for high resolution and high fidelity audio applications, which previously could only be achieved by Class-AB amplifiers. The TPA324x and TPA325x devices are analog input, closed loop (internal feedback network) Class-D audio amplifiers that can be further enhanced by adding an additional post-filter feedback (PFFB) or PFFB loop. This application report shows one optional implementation of PFFB for the TPA3244, TPA3245, TPA3250, TPA3251, and TPA3255 amplifiers. PFFB offers many benefits including lower output noise, improved THD+N performance, improved IMD performance, lower output impedance, frequency response less affected by load impedance, and suppression of nonlinearities of the LC filter. Contents 1 PFFB Implementation ....................................................................................................... 2 2 Closed Loop Gain............................................................................................................ 4 3 LC Filter Distortion........................................................................................................... 5 4 Performance Results ....................................................................................................... -
Constant K High Pass Filter
Constant k High Pass Filter Presentation by: S.KARTHIE Assistant Professor/ECE SSN College of Engineering Objective At the end of this section students will be able to understand, • What is a constant k high pass filter section • Characteristic impedance, attenuation and phase constant of high pass filters. • Design equations of high pass filters. High Pass Ladder Networks • A high-pass network arranged as a ladder is shown below. • As mentioned earlier, the repetitive network may be considered as a number of T or ∏ sections in cascade . C C C CC LL L L High Pass Ladder Networks • A T section may be taken from the ladder by removing ABED, producing the high-pass filter section as shown below. AB C CC 2C 2C 2C 2C LL L L D E High Pass Ladder Networks • Similarly, a ∏ section may be taken from the ladder by removing FGHI, producing the high- pass filter section as shown below. F G CCC 2L 2L 2L 2L I H Constant- K High Pass Filter • Constant k HPF is obtained by interchanging Z 1 and Z 2. 1 Z1 === & Z 2 === jωωωL jωωωC L 2 • Also, Z 1 Z 2 === === R k is satisfied. C Constant- K High Pass Filter • The HPF filter sections are 2C 2C C L 2L 2L Constant- K High Pass Filter Reactance curve X Z2 fC f Z1 Z1= -4Z 2 Stopband Passband Constant- K High Pass Filter • The cutoff frequency is 1 fC === 4πππ LC • The characteristic impedance of T and ∏ high pass filters sections are R k 2 Oπππ fC Z === ZOT === R k 1 −−− f 2 f 2 1 −−− C f 2 Constant- K High Pass Filter Characteristic impedance curves ZO ZOπ Nominal R k Impedance ZOT fC Frequency Stopband Passband Constant- K High Pass Filter • The attenuation and phase constants are fC fC ααα === 2cosh −−−1 βββ === −−− 2sin −−−1 f f f C f f ααα −−−πππ f C f βββ f Constant- K High Pass Filter Design equations • The expression for Inductance and Capacitance is obtained using cutoff frequency. -
33. RLC Parallel Circuit. Resonant Ac Circuits
University of Rhode Island DigitalCommons@URI PHY 204: Elementary Physics II -- Lecture Notes PHY 204: Elementary Physics II (2021) 12-4-2020 33. RLC parallel circuit. Resonant ac circuits Gerhard Müller University of Rhode Island, [email protected] Robert Coyne University of Rhode Island, [email protected] Follow this and additional works at: https://digitalcommons.uri.edu/phy204-lecturenotes Recommended Citation Müller, Gerhard and Coyne, Robert, "33. RLC parallel circuit. Resonant ac circuits" (2020). PHY 204: Elementary Physics II -- Lecture Notes. Paper 33. https://digitalcommons.uri.edu/phy204-lecturenotes/33https://digitalcommons.uri.edu/ phy204-lecturenotes/33 This Course Material is brought to you for free and open access by the PHY 204: Elementary Physics II (2021) at DigitalCommons@URI. It has been accepted for inclusion in PHY 204: Elementary Physics II -- Lecture Notes by an authorized administrator of DigitalCommons@URI. For more information, please contact [email protected]. PHY204 Lecture 33 [rln33] AC Circuit Application (2) In this RLC circuit, we know the voltage amplitudes VR, VC, VL across each device, the current amplitude Imax = 5A, and the angular frequency ω = 2rad/s. • Find the device properties R, C, L and the voltage amplitude of the ac source. Emax ~ εmax A R C L V V V 50V 25V 25V tsl305 We pick up the thread from the previous lecture with the quantitative anal- ysis of another RLC series circuit. Here our reasoning must be in reverse direction compared to that on the last page of lecture 32. Given the -
5 RC Circuits
Physics 212 Lab Lab 5 RC Circuits What You Need To Know: The Physics In the previous two labs you’ve dealt strictly with resistors. In today’s lab you’ll be using a new circuit element called a capacitor. A capacitor consists of two small metal plates that are separated by a small distance. This is evident in a capacitor’s circuit diagram symbol, see Figure 1. When a capacitor is hooked up to a circuit, charges will accumulate on the plates. Positive charge will accumulate on one plate and negative will accumulate on the other. The amount of charge that can accumulate is partially dependent upon the capacitor’s capacitance, C. With a charge distribution like this (i.e. plates of charge), a uniform electric field will be created between the plates. [You may remember this situation from the Equipotential Surfaces lab. In the lab, you had set-ups for two point-charges and two lines of charge. The latter set-up represents a capacitor.] A main function of a capacitor is to store energy. It stores its energy in the electric field between the plates. Battery Capacitor (with R charges shown) C FIGURE 1 - Battery/Capacitor FIGURE 2 - RC Circuit If you hook up a battery to a capacitor, like in Figure 1, positive charge will accumulate on the side that matches to the positive side of the battery and vice versa. When the capacitor is fully charged, the voltage across the capacitor will be equal to the voltage across the battery. You know this to be true because Kirchhoff’s Loop Law must always be true. -
Electronic Filters Design Tutorial - 3
Electronic filters design tutorial - 3 High pass, low pass and notch passive filters In the first and second part of this tutorial we visited the band pass filters, with lumped and distributed elements. In this third part we will discuss about low-pass, high-pass and notch filters. The approach will be without mathematics, the goal will be to introduce readers to a physical knowledge of filters. People interested in a mathematical analysis will find in the appendix some books on the topic. Fig.2 ∗ The constant K low-pass filter: it was invented in 1922 by George Campbell and the Running the simulation we can see the response meaning of constant K is the expression: of the filter in fig.3 2 ZL* ZC = K = R ZL and ZC are the impedances of inductors and capacitors in the filter, while R is the terminating impedance. A look at fig.1 will be clarifying. Fig.3 It is clear that the sharpness of the response increase as the order of the filter increase. The ripple near the edge of the cutoff moves from Fig 1 monotonic in 3 rd order to ringing of about 1.7 dB for the 9 th order. This due to the mismatch of the The two filter configurations, at T and π are various sections that are connected to a 50 Ω displayed, all the reactance are 50 Ω and the impedance at the edges of the filter and filter cells are all equal. In practice the two series connected to reactive impedances between cells.