An Indepth Look at Duals and Their Circuits

Total Page:16

File Type:pdf, Size:1020Kb

An Indepth Look at Duals and Their Circuits An Indepth Look at Duals and Their Circuits Jeffrey Phillips Freeman 2020-09-28 Duality is an approach that has been applied across countless disciplines where one takes an existing structure and transforms it into an equivalent structure, often with the intention of making it more useful for a particular context. In electronic circuits this usually means we take an existing circuit schematic and transform it in such a way that it serves a similar purpose but suited to our specific use case. One extremely trivial example of this would be converting two resistors in series, which act as a voltage divider, into two resistors in parallel producing a current divider. Another similarly trivial example would be to take a voltage divider and double the values of its resistors such that it divides the voltage by the same ratio but uses half the current to do so. In both cases the fundamental idea of dividing a value by a given ratio is the same, we just transform the circuit in different ways that are suited to our needs. One of the key advantages of duality is that it is feature-preserving, as such if the original circuit has particular desirable features but otherwise may not be well suited for our application we can transform the circuit into a dual in such a way as to preserve the desirable features but transform the undesirable features. For example a resistor based voltage divider has the advantageous feature of being relatively stable across various frequencies where other types of voltage dividers may have a very limited frequency range, so a resistor based voltage divider may be best suited for an extremely broadband application (large range of frequencies). However our application may require low-power consumption and the voltage divider may not need to drive a load and only need to be provided as an input to an IC with high impedance. As such if our reference circuit is for a voltage divider that uses relatively small values for resistors, and thus draws too much power, we can transform the voltage divider into its dual that preserves the frequency-stability of the original but reduces the current draw. This of course is a very trivial example, the concept of duality can, and often is, applied to much larger complex circuits as well. For this reason understanding circuit duality, and duality in general, specifically how to recognize it, apply it, and common circuit applications is a vital tool in anyone’s mental toolbox. 1 What is a Dual? Duality is the transformation of a mathematical model or structure into an equivalent mathematical model or structure such that each element of the original has a one-to-one relationship with an element in the result. The transformation between its elements usually represents an involution, which means if the same transformation is applied twice you wind up with the original; at the very least the transformation must be reversible (invertible) back to its original form. This implies that the transformation must be unique for any given input. Both the overall structure once converted is said to be the dual of the original, but so too are the individual elements of the structure considered the dual of their counterpart in the dual structure. Taking the reciprocal is an example of an involution, and thus a trivial example of duality. 1 f(x) = x Since f(x) is an involution the following must be true for any involution function. f(f(x)) = x Of course for the reciprocal this holds true. x = 5 1 f(5) = 5 1 f( ) = 5 5 1 Therefore we can say 5 is the dual of 5 under the reciprocal transformation. An involution can sometimes be an identity function, and thus create fixed points where the involution of one element is unchanged. This of course still holds true to the rules of a duality transformation whereby if the involution is applied twice you still wind up at the original, it is invertible. The identity transformation would be: f(x) = x Therefore it is trivial to see this holds true as an involution since the following is true. 2 f(f(x)) = x In this case any value is the dual of itself under the identity transformation. Which isn’t really saying much, but it is important to understand a fixed point is still a dual caused by an involution. As stated earlier duals are usually transformed between each other through an involution function, but this does not need to be the case. Any invertible (reversible) function can be a valid way to express duality. The technical term for the property of a function to be reversible is to say it is bijective But this is just a fancy way of saying you can reverse the function to get to where you started. For example adding one to a value is a bijective function since you can also subtract one and always get to where you started and there is no ambiguity in doing so. However multiplying by 0 is not bijective (invertible) because once you multiply by 0 you have no way of getting back to where you started, all numbers would transform into 0. In other words in order for a function to be invertible the output of the function must be a unique value for any given input of the function, otherwise ambiguity is introduced and there would be no way to reverse the process. f(x) = x + 1 As stated equation () is invertible as you can always subtract 1 and get back to where you started. f −1(x) = x − 1 f −1(f(x)) = x In this case f −1(x) is called the inverse function to f(x) and the notation used in equation () is the typical notation used to represent an inverse function. It should be trivially obvious but keep in mind an inverse function must work in both directions, in other words. f(f −1(x)) = f −1(f(x)) = x It should be noted that an involution function is closely related to a function and its inverse. All an involution function really is is a function where its inverse is itself. Also bear in mind not all values will have a dual, consider the reciprocal function, which is an involution (its own inverse) and thus a valid transformation. 3 1 f(x) = f −1(x) = x In the case of the reciprocal function a value of 0 for x is undefined since you can not divide by 0, any other real value other than 0, however, is valid. Therefore we can say that under the reciprocal transformation all real number values have a dual except for 0, which does not have a dual. Examples of Duals There are many common examples of duals in almost every subject from philos- ophy, to mechanical engineering, it is a pervasive idea that can often be useful in many fields. Here are a few example values and their duals under different inversion transformations. • True is the dual of False under the negation transformation • 10 is the dual of 0.1 under the reciprocal transformation • 5 is the dual of -5 under the negation transformation. • A current divider circuit is the dual of a voltage divider circuit under series-parallel transformation • A capacitor based high-pass filter is the dual of an inductor based high-pass filter under reciprocal impedance transformation • A bandpass filter is the dual of a band-stop filter under series-parallel transformation • Position is the dual of velocity under the derivative/integral transformation • Up is the dual of Down under vertical flip transformation • In philosophy the mind is the dual of the physical world under dual-aspect theory Similarly here are some examples of transformations and their inverse that are therefore capable of producing duals • Reciprocal transformation is its own inverse, an involution. • Negation transformation is its own inverse, an involution. • derivative transformation is the inverse of an integral transformation • A geometric flip transformation is its own inverse, an involution • doubling a value is the inverse of halving a value The Dual of a function Just as we have shown above that individual variables and values have a dual under an invertible function, likewise functions can also have duals in the same manner. Imagine we have an invertible function T (x) which will convert something to its dual, and we have some function f(x) we wish to find the dual of, then simply by passing the function into T we can produce its dual. Specifically T (f(x)) = f T (x) where the functions f(x) and f T (x) are duals of each other. 4 It is important to note here only T (x) needs to be invertible; neither f(x) nor f T (x) needs to have this property. For example; say the transformation under which we create the duals is the reciprocal function, which is invertible, but f(x) is the square function, which is not invertible. We know it isn’t invertible because 10 squared is 100 and -10 squared is also 100. So there is no way to reverse the value of 100 and get the original value since some information was lost, we no longer know if the original value was positive or negative. 1 T (x) = X f(x) = x2 1 f T (x) = T (f(x)) = x2 2 T 1 We can now see the function f(x) = x is the dual of f (x) = x2 under the reciprocal transformation. Manipulating A System of Equations Things get slightly more complicated when we start talking about systems rather than single variables or functions.
Recommended publications
  • A Novel Solid State Ultracapacitor
    National Aeronautics and NASA/TM—2017–219686 Space Administration IS02 George C. Marshall Space Flight Center Huntsville, Alabama 35812 A Novel Solid State Ultracapacitor A.Y. Cortés-Peña Johnson Space Center, Houston, Texas T.D. Rolin and S.M. Strickland Marshall Space Flight Center, Huntsville, Alabama C.W. Hill CK Technologies, Meridianville, Alabama August 2017 The NASA STI Program…in Profile Since its founding, NASA has been dedicated to the • CONFERENCE PUBLICATION. Collected advancement of aeronautics and space science. The papers from scientific and technical conferences, NASA Scientific and Technical Information (STI) symposia, seminars, or other meetings sponsored Program Office plays a key part in helping NASA or cosponsored by NASA. maintain this important role. • SPECIAL PUBLICATION. Scientific, technical, The NASA STI Program Office is operated by or historical information from NASA programs, Langley Research Center, the lead center for projects, and mission, often concerned with NASA’s scientific and technical information. The subjects having substantial public interest. NASA STI Program Office provides access to the NASA STI Database, the largest collection of • TECHNICAL TRANSLATION. aeronautical and space science STI in the world. English-language translations of foreign The Program Office is also NASA’s institutional scientific and technical material pertinent to mechanism for disseminating the results of its NASA’s mission. research and development activities. These results are published by NASA in the NASA STI Report Specialized services that complement the STI Series, which includes the following report types: Program Office’s diverse offerings include creating custom thesauri, building customized databases, • TECHNICAL PUBLICATION. Reports of organizing and publishing research results…even completed research or a major significant providing videos.
    [Show full text]
  • Permanent Magnet Guidelines
    MMPA PMG-88 PERMANENT MAGNET GUIDELINES I. Basic physics of permanent magnet materials II. Design relationships, figures of merit and optimizing techniques III. Measuring IV. Magnetizing V. Stabilizing and handling VI. Specifications, standards and communications VII. Bibliography MAGNETIC MATERIALS PRODUCERS ASSOCIATION 8 SOUTH MICHIGAN AVENUE • SUITE 1000 • CHICAGO, ILLINOIS 60603 INTRODUCTION This guide is a supplement to our MMPA Standard No. 0100. It relates the information in the Standard to permanent magnet circuit problems. The guide is a bridge between unit property data and a permanent magnet component having a specific size and geometry in order to establish a magnetic field in a given magnetic circuit environment. The MMPA 0100 defines magnetic, thermal, physical and mechanical properties. The properties given are descriptive in nature and not intended as a basis of acceptance or rejection. Magnetic measure- ments are difficult to make and less accurate than corresponding electrical mea- surements. A considerable amount of detailed information must be exchanged between producer and user if magnetic quantities are to be compared at two locations. MMPA member companies feel that this publication will be helpful in allowing both user and producer to arrive at a realistic and meaningful specifica- tion framework. Acknowledgment The Magnetic Materials Producers Association acknowledges the out- standing contribution of Rollin J. Parker to this industry and designers and manufacturers of products usingpermanent magnet materials. Mr Parker the Technical Consultant to MMPA compiled and wrote this document. We also wish to thank the Standards and Engineering Com- mittee of MMPA which reviewed and edited this document. December 1987 3M July 1988 5M August 1996 1M December 1998 1 M CONTENTS The guide is divided into the following sections: Glossary of terms and conversion tables- A very important starting point since the whole basis of communication in the magnetic material industry involves measurement of defined unit properties.
    [Show full text]
  • Compact Current Reference Circuits with Low Temperature Drift and High Compliance Voltage
    sensors Article Compact Current Reference Circuits with Low Temperature Drift and High Compliance Voltage Sara Pettinato, Andrea Orsini and Stefano Salvatori * Engineering Department, Università degli Studi Niccolò Cusano, via don Carlo Gnocchi 3, 00166 Rome, Italy; [email protected] (S.P.); [email protected] (A.O.) * Correspondence: [email protected] Received: 7 July 2020; Accepted: 25 July 2020; Published: 28 July 2020 Abstract: Highly accurate and stable current references are especially required for resistive-sensor conditioning. The solutions typically adopted in using resistors and op-amps/transistors display performance mainly limited by resistors accuracy and active components non-linearities. In this work, excellent characteristics of LT199x selectable gain amplifiers are exploited to precisely divide an input current. Supplied with a 100 µA reference IC, the divider is able to exactly source either a ~1 µA or a ~0.1 µA current. Moreover, the proposed solution allows to generate a different value for the output current by modifying only some connections without requiring the use of additional components. Experimental results show that the compliance voltage of the generator is close to the power supply limits, with an equivalent output resistance of about 100 GW, while the thermal coefficient is less than 10 ppm/◦C between 10 and 40 ◦C. Circuit architecture also guarantees physical separation of current carrying electrodes from voltage sensing ones, thus simplifying front-end sensor-interface circuitry. Emulating a resistive-sensor in the 10 kW–100 MW range, an excellent linearity is found with a relative error within 0.1% after a preliminary calibration procedure.
    [Show full text]
  • The Voltage Divider
    Book Author c01 V1 06/14/2012 7:46 AM 1 DC Review and Pre-Test Electronics cannot be studied without first under- standing the basics of electricity. This chapter is a review and pre-test on those aspects of direct current (DC) that apply to electronics. By no means does it cover the whole DC theory, but merely those topics that are essentialCOPYRIGHTED to simple electronics. MATERIAL This chapter reviews the following: ■■ Current flow ■■ Potential or voltage difference ■■ Ohm’s law ■■ Resistors in series and parallel c01.indd 1 6/14/2012 7:46:59 AM Book Author c01 V1 06/14/2012 7:46 AM 2 CHAPTER 1 DC REVIEW AND PRE-TEST ■■ Power ■■ Small currents ■■ Resistance graphs ■■ Kirchhoff’s Voltage Law ■■ Kirchhoff’s Current Law ■■ Voltage and current dividers ■■ Switches ■■ Capacitor charging and discharging ■■ Capacitors in series and parallel CURRENT FLOW 1 Electrical and electronic devices work because of an electric current. QUESTION What is an electric current? ANSWER An electric current is a flow of electric charge. The electric charge usually consists of negatively charged electrons. However, in semiconductors, there are also positive charge carriers called holes. 2 There are several methods that can be used to generate an electric current. QUESTION Write at least three ways an electron flow (or current) can be generated. c01.indd 2 6/14/2012 7:47:00 AM Book Author c01 V1 06/14/2012 7:46 AM CUrrENT FLOW 3 ANSWER The following is a list of the most common ways to generate current: ■■ Magnetically—This includes the induction of electrons in a wire rotating within a magnetic field.
    [Show full text]
  • Analysis of Magnetic Field and Electromagnetic Performance of a New Hybrid Excitation Synchronous Motor with Dual-V Type Magnets
    energies Article Analysis of Magnetic Field and Electromagnetic Performance of a New Hybrid Excitation Synchronous Motor with dual-V type Magnets Wenjing Hu, Xueyi Zhang *, Hongbin Yin, Huihui Geng, Yufeng Zhang and Liwei Shi School of Transportation and Vehicle Engineering, Shandong University of Technology, Zibo 255049, China; [email protected] (W.H.); [email protected] (H.Y.); [email protected] (H.G.); [email protected] (Y.Z.); [email protected] (L.S.) * Correspondence: [email protected]; Tel.: +86-137-089-41973 Received: 15 February 2020; Accepted: 17 March 2020; Published: 22 March 2020 Abstract: Due to the increasing energy crisis and environmental pollution, the development of drive motors for new energy vehicles (NEVs) has become the focus of popular attention. To improve the sine of the air-gap flux density and flux regulation capacity of drive motors, a new hybrid excitation synchronous motor (HESM) has been proposed. The HESM adopts a salient pole rotor with built-in dual-V permanent magnets (PMs), non-arc pole shoes and excitation windings. The fundamental topology, operating principle and analytical model for a magnetic field are presented. In the analytical model, the rotor magnetomotive force (MMF) is derived based on the minimum reluctance principle, and the permeance function considering a non-uniform air-gap is calculated using the magnetic equivalent circuit (MEC) method. Besides, the electromagnetic performance including the air-gap magnetic field and flux regulation capacity is analyzed by the finite element method (FEM). The simulation results of the air-gap magnetic field are consistent with the analytical results. The experiment and simulation results of the performance show that the flux waveform is sinusoidal-shaped and the air-gap flux can be adjusted effectively by changing the excitation current.
    [Show full text]
  • TION GALVANOMETERS in the Vibration Galvanorneter
    A paper to be presented at the 29th Annual Con* vention of the American Institute of Electrical Engineers, Boston, Mass., June 25, 1912. Copyright, 1912. By Α. I. Ε. E. (Subject to final revision for the Transactions.) CHARACTERISTICS AND APPLICATIONS OF VIBRA- TION GALVANOMETERS BY FRANK WENNER In the vibration galvanorneter we have a type of synchronous motor which is distinctly different from all the ordinary types of dynamo electric machines. Further it does not have any of the characteristics of any of the ordinary galvanometers and except for the fact that it is used in the detection or measure­ ment of small currents and voltages, it should not be called a galvanometer. In galvanometers, except when used in the measurement of transient currents or quantity of electricity, the moving system is displaced until we have an equality of static couples acting on it. In the vibration galvanometer the equilibrium condition is an equality between integral values of the product of the current and generated voltage and the mechanical power dissipated in various ways as in ordinary electric motors when operated without a load. It therefore behaves more like an electric motor than like a galvanometer. Further, since it is used only with alternating currents and op­ erates in synchronism with the current it must necessarily have some of the characteristics of a synchronous motor. As a motor the efficiency of conversion was found in a particular case to be as high as 97J per cent while the power required to maintain an easily discernable amplitude of vibration was of the order of 10-11 watts.
    [Show full text]
  • HOW the SCIO TECHNOLOGY WORKS Many Have Asked What Is
    HOW THE SCIO TECHNOLOGY WORKS Many have asked what is measured by the SCIO/QXCI medical device. This incredible advancement in medicine measures subtle electrical factors of the body. The history of alternative medicine has been dominated by old style resistance measuring devices. These antique devices depended on the operator to apply the probe to the acupuncture point. By subtle changing the speed of probe delivery (not the pressure), the operator could influence the outcome. This prevented true results. The other complication was the limits of just resistance testing. The body is much more complicated than just resistance. The electrical factors of the body include voltage, amperage, capacitance, inductance, frequency, and many others. The basics of bio-electrical medicine lie in the voltage, amperage, and resistance. The only thing that can truly be measured in electricity is the voltage and amperage. Everything else is a mathematical variation of voltage and amperage. So the QXCI device starts by measuring multiple channels of this information. Multiple channels are needed so that we can see variations in the electrical potential and flow of the body total. So we measure the extremities and the head. This direct measurement is of four channels of voltage, four of amperage, and four of resistance. These come into the computer for amplification and the computer acts as a frequency counter for receiving this data. This makes an active twelve channel measuring device. Other calculations are made mathematically. Resistance cannot be measured directly. It must be calculated from an amperage or voltage meter. Same as that any capacitance meters cannot directly measure capacitance it must do a mathematical adjustment of voltage and amperage flow.
    [Show full text]
  • Arxiv:1708.02856V1 [Cond-Mat.Mes-Hall] 9 Aug 2017 Systems Close to Equilibrium
    Probing the energy reactance with adiabatically driven quantum dots Mar´ıaFlorencia Ludovico,1, 2 Liliana Arrachea,1, 3 Michael Moskalets,4 and David S´anchez5 1International Center for Advanced Studies, UNSAM, Campus Miguelete, 25 de Mayo y Francia, 1650 Buenos Aires, Argentina 2The Abdus Salam International Centre for Theoretical Physics, Strada Costiera 11, I-34151 Trieste, Italy 3Dahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universit¨atBerlin, 14195 Berlin, Germany 4Department of Metal and Semiconductor Physics, NTU "Kharkiv Polytechnic Institute", 61002 Kharkiv, Ukraine 5Institute for Cross-Disciplinary Physics and Complex Systems IFISC (UIB-CSIC), E-07122 Palma de Mallorca, Spain The tunneling Hamiltonian describes a particle transfer from one region to the other. While there is no particle storage in the tunneling region itself, it has associated certain amount of energy. We name the corresponding flux energy reactance since, like an electrical reactance, it manifests itself in time-dependent transport only. Noticeably, this quantity is crucial to reproduce the universal charge relaxation resistance for a single-channel quantum capacitor at low temperatures. We show that a conceptually simple experiment is capable of demonstrating the existence of the energy reactance. PACS numbers: 73.23.-b, 72.10.Bg, 73.63.Kv, 44.10.+i Motivation. A very exciting experimental activity is lately taking place in search of controlling on-demand quantum coherent charge transport in the time domain. The recent burst of activity started with the experimen- Floating contact tal realization of quantum capacitors in quantum dots under ac driving [1], single particle emitters [2], and was followed by the generation of quantum charged solitons over the Fermi sea (levitons) [3].
    [Show full text]
  • PET4I101 ELECTROMAGNETICS ENGINEERING (4Th Sem ECE- ETC) Module-I (10 Hours)
    PET4I101 ELECTROMAGNETICS ENGINEERING (4th Sem ECE- ETC) Module-I (10 Hours) 1. Cartesian, Cylindrical and Spherical Coordinate Systems; Scalar and Vector Fields; Line, Surface and Volume Integrals. 2. Coulomb’s Law; The Electric Field Intensity; Electric Flux Density and Electric Flux; Gauss’s Law; Divergence of Electric Flux Density: Point Form of Gauss’s Law; The Divergence Theorem; The Potential Gradient; Energy Density; Poisson’s and Laplace’s Equations. Module-II3. Ampere’s (8 Magnetic Hours) Circuital Law and its Applications; Curl of H; Stokes’ Theorem; Divergence of B; Energy Stored in the Magnetic Field. 1. The Continuity Equation; Faraday’s Law of Electromagnetic Induction; Conduction Current: Point Form of Ohm’s Law, Convection Current; The Displacement Current; 2. Maxwell’s Equations in Differential Form; Maxwell’s Equations in Integral Form; Maxwell’s Equations for Sinusoidal Variation of Fields with Time; Boundary Module-IIIConditions; (8The Hours) Retarded Potential; The Poynting Vector; Poynting Vector for Fields Varying Sinusoid ally with Time 1. Solution of the One-Dimensional Wave Equation; Solution of Wave Equation for Sinusoid ally Time-Varying Fields; Polarization of Uniform Plane Waves; Fields on the Surface of a Perfect Conductor; Reflection of a Uniform Plane Wave Incident Normally on a Perfect Conductor and at the Interface of Two Dielectric Regions; The Standing Wave Ratio; Oblique Incidence of a Plane Wave at the Boundary between Module-IVTwo Regions; (8 ObliqueHours) Incidence of a Plane Wave on a Flat Perfect Conductor and at the Boundary between Two Perfect Dielectric Regions; 1. Types of Two-Conductor Transmission Lines; Circuit Model of a Uniform Two- Conductor Transmission Line; The Uniform Ideal Transmission Line; Wave AReflectiondditional at Module a Discontinuity (Terminal in an Examination-Internal) Ideal Transmission Line; (8 MatchingHours) of Transmission Lines with Load.
    [Show full text]
  • Transient Simulation of Magnetic Circuits Using the Permeance-Capacitance Analogy
    Transient Simulation of Magnetic Circuits Using the Permeance-Capacitance Analogy Jost Allmeling Wolfgang Hammer John Schonberger¨ Plexim GmbH Plexim GmbH TridonicAtco Schweiz AG Technoparkstrasse 1 Technoparkstrasse 1 Obere Allmeind 2 8005 Zurich, Switzerland 8005 Zurich, Switzerland 8755 Ennenda, Switzerland Email: [email protected] Email: [email protected] Email: [email protected] Abstract—When modeling magnetic components, the R1 Lσ1 Lσ2 R2 permeance-capacitance analogy avoids the drawbacks of traditional equivalent circuits models. The magnetic circuit structure is easily derived from the core geometry, and the Ideal Transformer Lm Rfe energy relationship between electrical and magnetic domain N1:N2 is preserved. Non-linear core materials can be modeled with variable permeances, enabling the implementation of arbitrary saturation and hysteresis functions. Frequency-dependent losses can be realized with resistors in the magnetic circuit. Fig. 1. Transformer implementation with coupled inductors The magnetic domain has been implemented in the simulation software PLECS. To avoid numerical integration errors, Kirch- hoff’s current law must be applied to both the magnetic flux and circuit, in which inductances represent magnetic flux paths the flux-rate when solving the circuit equations. and losses incur at resistors. Magnetic coupling between I. INTRODUCTION windings is realized either with mutual inductances or with ideal transformers. Inductors and transformers are key components in modern power electronic circuits. Compared to other passive com- Using coupled inductors, magnetic components can be ponents they are difficult to model due to the non-linear implemented in any circuit simulator since only electrical behavior of magnetic core materials and the complex structure components are required.
    [Show full text]
  • 6.685 Electric Machines, Course Notes 2: Magnetic Circuit Basics
    Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.685 Electric Machines Class Notes 2 Magnetic Circuit Basics c 2003 James L. Kirtley Jr. 1 Introduction Magnetic Circuits offer, as do electric circuits, a way of simplifying the analysis of magnetic field systems which can be represented as having a collection of discrete elements. In electric circuits the elements are sources, resistors and so forth which are represented as having discrete currents and voltages. These elements are connected together with ‘wires’ and their behavior is described by network constraints (Kirkhoff’s voltage and current laws) and by constitutive relationships such as Ohm’s Law. In magnetic circuits the lumped parameters are called ‘Reluctances’ (the inverse of ‘Reluctance’ is called ‘Permeance’). The analog to a ‘wire’ is referred to as a high permeance magnetic circuit element. Of course high permeability is the analog of high conductivity. By organizing magnetic field systems into lumped parameter elements and using network con- straints and constitutive relationships we can simplify the analysis of such systems. 2 Electric Circuits First, let us review how Electric Circuits are defined. We start with two conservation laws: conser- vation of charge and Faraday’s Law. From these we can, with appropriate simplifying assumptions, derive the two fundamental circiut constraints embodied in Kirkhoff’s laws. 2.1 KCL Conservation of charge could be written in integral form as: dρ J~ · ~nda + f dv = 0 (1) ZZ Zvolume dt This simply states that the sum of current out of some volume of space and rate of change of free charge in that space must be zero.
    [Show full text]
  • 1Basic Amplifier Configurations for Optimum Transfer of Information From
    1 Basic amplifier configurations for optimum transfer of 1 information from signal sources to loads 1.1 Introduction One of the aspects of amplifier design most treated — in spite of its importance — like a stepchild is the adaptation of the amplifier input and output impedances to the signal source and the load. The obvious reason for neglect in this respect is that it is generally not sufficiently realized that amplifier design is concerned with the transfer of signal information from the signal source to the load, rather than with the amplification of voltage, current, or power. The electrical quantities have, as a matter of fact, no other function than represent- ing the signal information. Which of the electrical quantities can best serve as the information representative depends on the properties of the signal source and load. It will be pointed out in this chapter that the characters of the input and output impedances of an amplifier have to be selected on the grounds of the types of information representing quantities at input and output. Once these selections are made, amplifier design can be continued by considering the transfer of electrical quantities. By speaking then, for example, of a voltage amplifier, it is meant that voltage is the information representing quantity at input and output. The relevant information transfer function is then indicated as a voltage gain. After the discussion of this impedance-adaptation problem, we will formulate some criteria for optimum realization of amplifiers, referring to noise performance, accuracy, linearity and efficiency. These criteria will serve as a guide in looking for the basic amplifier configurations that can provide the required transfer properties.
    [Show full text]