The Philosophical Significance of the Concept of Superposition in Quantum Field Theory
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Origin of Probability in Quantum Mechanics and the Physical Interpretation of the Wave Function
Origin of Probability in Quantum Mechanics and the Physical Interpretation of the Wave Function Shuming Wen ( [email protected] ) Faculty of Land and Resources Engineering, Kunming University of Science and Technology. Research Article Keywords: probability origin, wave-function collapse, uncertainty principle, quantum tunnelling, double-slit and single-slit experiments Posted Date: November 16th, 2020 DOI: https://doi.org/10.21203/rs.3.rs-95171/v2 License: This work is licensed under a Creative Commons Attribution 4.0 International License. Read Full License Origin of Probability in Quantum Mechanics and the Physical Interpretation of the Wave Function Shuming Wen Faculty of Land and Resources Engineering, Kunming University of Science and Technology, Kunming 650093 Abstract The theoretical calculation of quantum mechanics has been accurately verified by experiments, but Copenhagen interpretation with probability is still controversial. To find the source of the probability, we revised the definition of the energy quantum and reconstructed the wave function of the physical particle. Here, we found that the energy quantum ê is 6.62606896 ×10-34J instead of hν as proposed by Planck. Additionally, the value of the quality quantum ô is 7.372496 × 10-51 kg. This discontinuity of energy leads to a periodic non-uniform spatial distribution of the particles that transmit energy. A quantum objective system (QOS) consists of many physical particles whose wave function is the superposition of the wave functions of all physical particles. The probability of quantum mechanics originates from the distribution rate of the particles in the QOS per unit volume at time t and near position r. Based on the revision of the energy quantum assumption and the origin of the probability, we proposed new certainty and uncertainty relationships, explained the physical mechanism of wave-function collapse and the quantum tunnelling effect, derived the quantum theoretical expression of double-slit and single-slit experiments. -
Engineering Viscoelasticity
ENGINEERING VISCOELASTICITY David Roylance Department of Materials Science and Engineering Massachusetts Institute of Technology Cambridge, MA 02139 October 24, 2001 1 Introduction This document is intended to outline an important aspect of the mechanical response of polymers and polymer-matrix composites: the field of linear viscoelasticity. The topics included here are aimed at providing an instructional introduction to this large and elegant subject, and should not be taken as a thorough or comprehensive treatment. The references appearing either as footnotes to the text or listed separately at the end of the notes should be consulted for more thorough coverage. Viscoelastic response is often used as a probe in polymer science, since it is sensitive to the material’s chemistry and microstructure. The concepts and techniques presented here are important for this purpose, but the principal objective of this document is to demonstrate how linear viscoelasticity can be incorporated into the general theory of mechanics of materials, so that structures containing viscoelastic components can be designed and analyzed. While not all polymers are viscoelastic to any important practical extent, and even fewer are linearly viscoelastic1, this theory provides a usable engineering approximation for many applications in polymer and composites engineering. Even in instances requiring more elaborate treatments, the linear viscoelastic theory is a useful starting point. 2 Molecular Mechanisms When subjected to an applied stress, polymers may deform by either or both of two fundamen- tally different atomistic mechanisms. The lengths and angles of the chemical bonds connecting the atoms may distort, moving the atoms to new positions of greater internal energy. -
Basic Electrical Engineering
BASIC ELECTRICAL ENGINEERING V.HimaBindu V.V.S Madhuri Chandrashekar.D GOKARAJU RANGARAJU INSTITUTE OF ENGINEERING AND TECHNOLOGY (Autonomous) Index: 1. Syllabus……………………………………………….……….. .1 2. Ohm’s Law………………………………………….…………..3 3. KVL,KCL…………………………………………….……….. .4 4. Nodes,Branches& Loops…………………….……….………. 5 5. Series elements & Voltage Division………..………….……….6 6. Parallel elements & Current Division……………….………...7 7. Star-Delta transformation…………………………….………..8 8. Independent Sources …………………………………..……….9 9. Dependent sources……………………………………………12 10. Source Transformation:…………………………………….…13 11. Review of Complex Number…………………………………..16 12. Phasor Representation:………………….…………………….19 13. Phasor Relationship with a pure resistance……………..……23 14. Phasor Relationship with a pure inductance………………....24 15. Phasor Relationship with a pure capacitance………..……….25 16. Series and Parallel combinations of Inductors………….……30 17. Series and parallel connection of capacitors……………...…..32 18. Mesh Analysis…………………………………………………..34 19. Nodal Analysis……………………………………………….…37 20. Average, RMS values……………….……………………….....43 21. R-L Series Circuit……………………………………………...47 22. R-C Series circuit……………………………………………....50 23. R-L-C Series circuit…………………………………………....53 24. Real, reactive & Apparent Power…………………………….56 25. Power triangle……………………………………………….....61 26. Series Resonance……………………………………………….66 27. Parallel Resonance……………………………………………..69 28. Thevenin’s Theorem…………………………………………...72 29. Norton’s Theorem……………………………………………...75 30. Superposition Theorem………………………………………..79 31. -
The Tuning Fork: an Amazing Acoustics Apparatus
FEATURED ARTICLE The Tuning Fork: An Amazing Acoustics Apparatus Daniel A. Russell It seems like such a simple device: a U-shaped piece of metal and Helmholtz resonators were two of the most impor- with a stem to hold it; a simple mechanical object that, when tant items of equipment in an acoustics laboratory. In 1834, struck lightly, produces a single-frequency pure tone. And Johann Scheibler, a silk manufacturer without a scientific yet, this simple appearance is deceptive because a tuning background, created a tonometer, a set of precisely tuned fork exhibits several complicated vibroacoustic phenomena. resonators (in this case tuning forks, although others used A tuning fork vibrates with several symmetrical and asym- Helmholtz resonators) used to determine the frequency of metrical flexural bending modes; it exhibits the nonlinear another sound, essentially a mechanical frequency ana- phenomenon of integer harmonics for large-amplitude lyzer. Scheibler’s tonometer consisted of 56 tuning forks, displacements; and the stem oscillates at the octave of the spanning the octave from A3 220 Hz to A4 440 Hz in steps fundamental frequency of the tines even though the tines of 4 Hz (Helmholtz, 1885, p. 441); he achieved this accu- have no octave component. A tuning fork radiates sound as racy by modifying each fork until it produced exactly 4 a linear quadrupole source, with a distinct transition from beats per second with the preceding fork in the set. At the a complicated near-field to a simpler far-field radiation pat- 1876 Philadelphia Centennial Exposition, Rudolph Koenig, tern. This transition from near field to far field can be seen the premier manufacturer of acoustics apparatus during in the directivity patterns, time-averaged vector intensity, the second half of the nineteenth century, displayed his and the phase relationship between pressure and particle Grand Tonometer with 692 precision tuning forks ranging velocity. -
Apparatus Named After Our Academic Ancestors, III
Digital Kenyon: Research, Scholarship, and Creative Exchange Faculty Publications Physics 2014 Apparatus Named After Our Academic Ancestors, III Tom Greenslade Kenyon College, [email protected] Follow this and additional works at: https://digital.kenyon.edu/physics_publications Part of the Physics Commons Recommended Citation “Apparatus Named After Our Academic Ancestors III”, The Physics Teacher, 52, 360-363 (2014) This Article is brought to you for free and open access by the Physics at Digital Kenyon: Research, Scholarship, and Creative Exchange. It has been accepted for inclusion in Faculty Publications by an authorized administrator of Digital Kenyon: Research, Scholarship, and Creative Exchange. For more information, please contact [email protected]. Apparatus Named After Our Academic Ancestors, III Thomas B. Greenslade Jr. Citation: The Physics Teacher 52, 360 (2014); doi: 10.1119/1.4893092 View online: http://dx.doi.org/10.1119/1.4893092 View Table of Contents: http://scitation.aip.org/content/aapt/journal/tpt/52/6?ver=pdfcov Published by the American Association of Physics Teachers Articles you may be interested in Crystal (Xal) radios for learning physics Phys. Teach. 53, 317 (2015); 10.1119/1.4917450 Apparatus Named After Our Academic Ancestors — II Phys. Teach. 49, 28 (2011); 10.1119/1.3527751 Apparatus Named After Our Academic Ancestors — I Phys. Teach. 48, 604 (2010); 10.1119/1.3517028 Physics Northwest: An Academic Alliance Phys. Teach. 45, 421 (2007); 10.1119/1.2783150 From Our Files Phys. Teach. 41, 123 (2003); 10.1119/1.1542054 This article is copyrighted as indicated in the article. Reuse of AAPT content is subject to the terms at: http://scitation.aip.org/termsconditions. -
Superposition of Waves
Superposition of waves 1 Superposition of waves Superposition of waves is the common conceptual basis for some optical phenomena such as: £ Polarization £ Interference £ Diffraction ¢ What happens when two or more waves overlap in some region of space. ¢ How the specific properties of each wave affects the ultimate form of the composite disturbance? ¢ Can we recover the ingredients of a complex disturbance? 2 Linearity and superposition principle ∂2ψ (r,t) 1 ∂2ψ (r,t) The scaler 3D wave equation = is a linear ∂r 2 V 2 ∂t 2 differential equation (all derivatives apper in first power). So any n linear combination of its solutions ψ (r,t) = Ciψ i (r,t) is a solution. i=1 Superposition principle: resultant disturbance at any point in a medium is the algebraic sum of the separate constituent waves. We focus only on linear systems and scalar functions for now. At high intensity limits most systems are nonlinear. Example: power of a typical focused laser beam=~1010 V/cm compared to sun light on earth ~10 V/cm. Electric field of the laser beam triggers nonlinear phenomena. 3 Superposition of two waves Two light rays with same frequency meet at point p traveled by x1 and x2 E1 = E01 sin[ωt − (kx1 + ε1)] = E01 sin[ωt +α1 ] E2 = E02 sin[ωt − (kx2 + ε 2 )] = E02 sin[ωt +α2 ] Where α1 = −(kx1 + ε1 ) and α2 = −(kx2 + ε 2 ) Magnitude of the composite wave is sum of the magnitudes at a point in space & time or: E = E1 + E2 = E0 sin (ωt +α ) where 2 2 2 E01 sinα1 + E02 sinα2 E0 = E01 + E02 + 2E01E02 cos(α2 −α1) and tanα = E01 cosα1 + E02 cosα2 The resulting wave has same frequency but different amplitude and phase. -
Linear Superposition Principle Applying to Hirota Bilinear Equations
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Computers and Mathematics with Applications 61 (2011) 950–959 Contents lists available at ScienceDirect Computers and Mathematics with Applications journal homepage: www.elsevier.com/locate/camwa Linear superposition principle applying to Hirota bilinear equations Wen-Xiu Ma a,∗, Engui Fan b,1 a Department of Mathematics and Statistics, University of South Florida, Tampa, FL 33620-5700, USA b School of Mathematical Sciences and Key Laboratory of Mathematics for Nonlinear Science, Fudan University, Shanghai 200433, PR China article info a b s t r a c t Article history: A linear superposition principle of exponential traveling waves is analyzed for Hirota Received 6 October 2010 bilinear equations, with an aim to construct a specific sub-class of N-soliton solutions Accepted 21 December 2010 formed by linear combinations of exponential traveling waves. Applications are made for the 3 C 1 dimensional KP, Jimbo–Miwa and BKP equations, thereby presenting their Keywords: particular N-wave solutions. An opposite question is also raised and discussed about Hirota's bilinear form generating Hirota bilinear equations possessing the indicated N-wave solutions, and a few Soliton equations illustrative examples are presented, together with an algorithm using weights. N-wave solution ' 2010 Elsevier Ltd. All rights reserved. 1. Introduction It is significantly important in mathematical physics to search for exact solutions to nonlinear differential equations. Exact solutions play a vital role in understanding various qualitative and quantitative features of nonlinear phenomena. There are diverse classes of interesting exact solutions, such as traveling wave solutions and soliton solutions, but it often needs specific mathematical techniques to construct exact solutions due to the nonlinearity present in dynamics (see, e.g., [1,2]). -
Chapter 14 Interference and Diffraction
Chapter 14 Interference and Diffraction 14.1 Superposition of Waves.................................................................................... 14-2 14.2 Young’s Double-Slit Experiment ..................................................................... 14-4 Example 14.1: Double-Slit Experiment................................................................ 14-7 14.3 Intensity Distribution ........................................................................................ 14-8 Example 14.2: Intensity of Three-Slit Interference ............................................ 14-11 14.4 Diffraction....................................................................................................... 14-13 14.5 Single-Slit Diffraction..................................................................................... 14-13 Example 14.3: Single-Slit Diffraction ................................................................ 14-15 14.6 Intensity of Single-Slit Diffraction ................................................................. 14-16 14.7 Intensity of Double-Slit Diffraction Patterns.................................................. 14-19 14.8 Diffraction Grating ......................................................................................... 14-20 14.9 Summary......................................................................................................... 14-22 14.10 Appendix: Computing the Total Electric Field............................................. 14-23 14.11 Solved Problems .......................................................................................... -
1. GROUNDWORK 1.1. Superposition Principle. This Principle States That, for Linear Systems, the Effects of a Sum of Stimuli Equals the Sum of the Individual Stimuli
1. GROUNDWORK 1.1. Superposition Principle. This principle states that, for linear systems, the effects of a sum of stimuli equals the sum of the individual stimuli. Linearity will be mathematically defined in section 1.2.; for now we will gain a physical intuition for what it means Stimulus is quite general, it can refer to a force applied to a mass on a spring, a voltage applied to an LRC circuit, or an optical field impinging on a piece of tissue. Effect can be anything from the displacement of the mass attached to the spring, the transport of charge through a wire, to the optical field scattered by the tissue. The stimulus and effect are referred to as input and output of the system. By system we understand the mechanism that transforms the input into output; e.g. the mass-spring ensemble, LRC circuit, or the tissue in the example above. 1 The consequence of the superposition principle is that the solution (output) to a complicated input can be obtained by solving a number of simpler problems, the results of which can be summed up in the end. Figure 1. The superposition principle. The response of the system (e.g. a piece of glass) to the sum of two fields is the sum of the output of each field. 2 To find the response to the two fields through the system, we have two choices: o i) add the two inputs UU12 and solve for the output; o ii) find the individual outputs and add them up, UU''12 . -
Early Use of the Scott-Koenig Phonautograph for Documenting Performance G
Acoustics 08 Paris Early use of the Scott-Koenig phonautograph for documenting performance G. Brock-Nannestada and J.-M. Fontaineb aPatent Tactics, Resedavej 40, DK-2820 Gentofte, Denmark bUniversit´eUPMC - Minist`erede la Culture - CNRS - IJRA - LAM, 11, rue de Lourmel, F-75015 Paris, France [email protected] 6239 Acoustics 08 Paris Acoustics of phenomena in the air in the 1850s combined listening, observation and tabulation. This was "real-time", catching any phenomenon as it appeared. If it was repeatable, one could be prepared. Continuous, rather than tabular data enabled a very different analysis from observation plus notebooks. Édouard-Léon Scott's invention of the phonautograph enabled this. A surface moved below a stylus vibrated by sound in air. Originally the surface was a blackened glass plate, and it became a sheet of blackened paper. The scientific instrument maker Rudolph Koenig contributed his craftsmanship by building a very professional apparatus. A two-dimensional representation of the individual vibrations was obtained. Scott deposited a sealed letter with the Paris Academy of Sciences in January, 1857 and filed a patent application in April, 1857. Later he deposited a further sealed letter and in 1859 he filed an application for patent of addition. Analyzing the thoughts expressed and documented in his manuscripts and by Koenig's licensed production it is feasible to see how they were dependent on each other, although they had different purposes in mind. The paper concentrates on Scott's interests in performance vs. Koenig's in partials, and the structure of original tracings are discussed. the air". Phillips [7] provides a very lucid explanation for these observations. -
ON the PRINCIPLE of SUPERPOSITION in QUANTUM MECHANICS GFD Duff
ON THE PRINCIPLE OF SUPERPOSITION IN QUANTUM MECHANICS G. F.D. Duff (received March 21, 1963) The principle of superposition of states requires that the states of a dynamical system form a linear vector space. This hypothesis of linearity has usually been regarded as a funda mental postulate in quantum mechanics, of a kind that cannot be explained by classical concepts. Indeed, Dirac [2, p. 14] comments that "the superposition that occurs in quantum mechanics is of an essentially different nature from any occurring in the classical theory, as is shown by the fact that the quantum superposition principle demands indeterminacy in the results of observations in order to be capable of a sensible physical interpretation. " It is therefore of interest to examine to what extent and in what form, if any, the principle of superposition might be latent in classical mechanics. This note presents a demon stration of the superposition principle as a consequence of four properties enjoyed by the Hamilton-Jacobi equation of classical mechanics. These properties are: (a) invariance under transformations of generalized coordinates, (b) direct additivity of the degrees of freedom, (c) linearity in the metric, (d) it is of first order with respect to the time. Canad. Math. Bull, vol.7, no.l, January 1964 77 Downloaded from https://www.cambridge.org/core. 28 Sep 2021 at 11:39:49, subject to the Cambridge Core terms of use. The method applies to systems with quadratic Hamiltonians, which include most of the leading elementary examples upon which the Schrôdinger quantum theory was founded [5]. Our results here will be concerned only with the non-relativistic theory.- Let q. -
Music and the Making of Modern Science
Music and the Making of Modern Science Music and the Making of Modern Science Peter Pesic The MIT Press Cambridge, Massachusetts London, England © 2014 Massachusetts Institute of Technology All rights reserved. No part of this book may be reproduced in any form by any electronic or mechanical means (including photocopying, recording, or information storage and retrieval) without permission in writing from the publisher. MIT Press books may be purchased at special quantity discounts for business or sales promotional use. For information, please email [email protected]. This book was set in Times by Toppan Best-set Premedia Limited, Hong Kong. Printed and bound in the United States of America. Library of Congress Cataloging-in-Publication Data Pesic, Peter. Music and the making of modern science / Peter Pesic. pages cm Includes bibliographical references and index. ISBN 978-0-262-02727-4 (hardcover : alk. paper) 1. Science — History. 2. Music and science — History. I. Title. Q172.5.M87P47 2014 509 — dc23 2013041746 10 9 8 7 6 5 4 3 2 1 For Alexei and Andrei Contents Introduction 1 1 Music and the Origins of Ancient Science 9 2 The Dream of Oresme 21 3 Moving the Immovable 35 4 Hearing the Irrational 55 5 Kepler and the Song of the Earth 73 6 Descartes ’ s Musical Apprenticeship 89 7 Mersenne ’ s Universal Harmony 103 8 Newton and the Mystery of the Major Sixth 121 9 Euler: The Mathematics of Musical Sadness 133 10 Euler: From Sound to Light 151 11 Young ’ s Musical Optics 161 12 Electric Sounds 181 13 Hearing the Field 195 14 Helmholtz and the Sirens 217 15 Riemann and the Sound of Space 231 viii Contents 16 Tuning the Atoms 245 17 Planck ’ s Cosmic Harmonium 255 18 Unheard Harmonies 271 Notes 285 References 311 Sources and Illustration Credits 335 Acknowledgments 337 Index 339 Introduction Alfred North Whitehead once observed that omitting the role of mathematics in the story of modern science would be like performing Hamlet while “ cutting out the part of Ophelia.