Terrestrial and Extraterrestrial Radiation Sources That Move Faster Than Light Andrea Caroline Schmidt Zweifel
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Retarded Potentials and Power Emission by Accelerated Charges
Alma Mater Studiorum Universita` di Bologna · Scuola di Scienze Dipartimento di Fisica e Astronomia Corso di Laurea in Fisica Classical Electrodynamics: Retarded Potentials and Power Emission by Accelerated Charges Relatore: Presentata da: Prof. Roberto Zucchini Mirko Longo Anno Accademico 2015/2016 1 Sommario. L'obiettivo di questo lavoro ´equello di analizzare la potenza emes- sa da una carica elettrica accelerata. Saranno studiati due casi speciali: ac- celerazione lineare e accelerazione circolare. Queste sono le configurazioni pi´u frequenti e semplici da realizzare. Il primo passo consiste nel trovare un'e- spressione per il campo elettrico e il campo magnetico generati dalla carica. Questo sar´areso possibile dallo studio della distribuzione di carica di una sor- gente puntiforme e dei potenziali che la descrivono. Nel passo successivo verr´a calcolato il vettore di Poynting per una tale carica. Useremo questo risultato per trovare la potenza elettromagnetica irradiata totale integrando su tutte le direzioni di emissione. Nell'ultimo capitolo, infine, faremo uso di tutto ci´oche ´e stato precedentemente trovato per studiare la potenza emessa da cariche negli acceleratori. 4 Abstract. This paper’s goal is to analyze the power emitted by an accelerated electric charge. Two special cases will be scrutinized: the linear acceleration and the circular acceleration. These are the most frequent and easy to realize configurations. The first step consists of finding an expression for electric and magnetic field generated by our charge. This will be achieved by studying the charge distribution of a point-like source and the potentials that arise from it. The following step involves the computation of the Poynting vector. -
H. G. Wells Time Traveler
Items on Exhibit 1. H. G. Wells – Teacher to the World 11. H. G. Wells. Die Zeitmaschine. (Illustrierte 21. H. G. Wells. Picshua [sketch] ‘Omaggio to 1. H. G. Wells (1866-1946). Text-book of Klassiker, no. 46) [Aachen: Bildschriftenverlag, P.C.B.’ [1900] Biology. London: W.B. Clive & Co.; University 196-]. Wells Picshua Box 1 H. G. Wells Correspondence College Press, [1893]. Wells Q. 823 W46ti:G Wells 570 W46t, vol. 1, cop. 1 Time Traveler 12. H. G. Wells. La machine à explorer le temps. 7. Fantasias of Possibility 2. H. G. Wells. The Outline of History, Being a Translated by Henry-D. Davray, illustrated by 22. H. G. Wells. The World Set Free [holograph Plain History of Life and Mankind. London: G. Max Camis. Paris: R. Kieffer, [1927]. manuscript, ca. 1913]. Simon J. James is Head of the Newnes, [1919-20]. Wells 823 W46tiFd Wells WE-001, folio W-3 Wells Q. 909 W46o 1919 vol. 2, part. 24, cop. 2 Department of English Studies, 13. H. G. Wells. Stroz času : Neviditelný. 23. H. G. Wells to Frederick Wells, ‘Oct. 27th 45’ Durham University, UK. He has 3. H. G. Wells. ‘The Idea of a World Translated by Pavla Moudrá. Prague: J. Otty, [Holograph letter]. edited Wells texts for Penguin and Encyclopedia.’ Nature, 138, no. 3500 (28 1905. Post-1650 MS 0667, folder 75 November 1936) : 917-24. Wells 823 W46tiCzm. World’s Classics and The Wellsian, the Q. 505N 24. H. G. Wells’ Things to Come. Produced by scholarly journal of the H. G. Wells Alexander Korda, directed by William Cameron Society. -
The Future of Robotics an Inside View on Innovation in Robotics
The Future of Robotics An Inside View on Innovation in Robotics FEATURE Robots, Humans and Work Executive Summary Robotics in the Startup Ecosystem The automation of production through three industrial revolutions has increased global output exponentially. Now, with machines increasingly aware and interconnected, Industry 4.0 is upon us. Leading the charge are fleets of autonomous robots. Built by major multinationals and increasingly by innovative VC-backed companies, these robots have already become established participants in many areas of the economy, from assembly lines to farms to restaurants. Investors, founders and policymakers are all still working to conceptualize a framework for these companies and their transformative Austin Badger technology. In this report, we take a data-driven approach to emerging topics in the industry, including business models, performance metrics, Director, Frontier Tech Practice and capitalization trends. Finally, we review leading theories of how automation affects the labor market, and provide quantitative evidence for and against them. It is our view that the social implications of this industry will be massive and will require a continual examination by those driving this technology forward. The Future of Robotics 2 Table of Contents 4 14 21 The Landscape VC and Robots Robots, Humans and Work Industry 4.0 and the An Emerging Framework Robotics Ecosystem The Interplay of Automation and Labor The Future of Robotics 3 The Landscape Industry 4.0 and the Robotics Ecosystem The Future of Robotics 4 COVID-19 and US Manufacturing, Production and Nonsupervisory Workers the Next 12.8M Automation Wave 10.2M Recessions tend to reduce 9.0M employment, and some jobs don’t come back. -
Arxiv:Physics/0303103V3
Comment on ‘About the magnetic field of a finite wire’∗ V Hnizdo National Institute for Occupational Safety and Health, 1095 Willowdale Road, Morgantown, WV 26505, USA Abstract. A flaw is pointed out in the justification given by Charitat and Graner [2003 Eur. J. Phys. 24, 267] for the use of the Biot–Savart law in the calculation of the magnetic field due to a straight current-carrying wire of finite length. Charitat and Graner (CG) [1] apply the Amp`ere and Biot-Savart laws to the problem of the magnetic field due to a straight current-carrying wire of finite length, and note that these laws lead to different results. According to the Amp`ere law, the magnitude B of the magnetic field at a perpendicular distance r from the midpoint along the length 2l of a wire carrying a current I is B = µ0I/(2πr), while the Biot–Savart law gives this quantity as 2 2 B = µ0Il/(2πr√r + l ) (the right-hand side of equation (3) of [1] for B cannot be correct as sin α on the left-hand side there must equal l/√r2 + l2). To explain the fact that the Amp`ere and Biot–Savart laws lead here to different results, CG say that the former is applicable only in a time-independent magnetostatic situation, whereas the latter is ‘a general solution of Maxwell–Amp`ere equations’. A straight wire of finite length can carry a current only when there is a current source at one end of the wire and a curent sink at the other end—and this is possible only when there are time-dependent net charges at both ends of the wire. -
A NEW SOCIAL COMPACT for Work and Workers
FUTURE OF WORK IN CALIFORNIA A NEW SOCIAL COMPACT for work and workers RE OF W TU OR FU K CO N M MISSIO E OF W TUR OR FU K CO N M MISSIO Commissioners Produced by Institute for the Future (IFTF) for the California Future of Members of the Future of Work Commission were appointed by Governor Work Commission, with the support Gavin Newsom to help create inclusive, long-term economic growth and ensure from The James Irvine Foundation, Californians share in that success. Blue Shield of California Foundation, the Ford Foundation and Lumina Mary Kay Henry, Co-Chair Ash Kalra Foundation. President, Service Employees State Assemblymember, California International Union District 27 James Manyika, Co-Chair Stephane Kasriel Chairman & Director, McKinsey Former CEO, Upwork Global Institute Commission Staff Fei-Fei Li Roy Bahat Professor & Co-Director, Human- Anmol Chaddha, Head, Bloomberg Beta Centered Artificial Intelligence Manager Institute, Stanford Doug Bloch Alyssa Andersen Political Director, Teamsters Joint John Marshall Julie Ericsson Council 7 Senior Capital Markets Economist, United Food and Commercial Ben Gansky Soraya Coley Workers President, California Polytechnic Georgia Gillan State University, Pomona Art Pulaski Executive Secretary-Treasurer Marina Gorbis Lloyd Dean & Chief Officer, California Labor CEO, CommonSpirit Health Jean Hagan Federation Jennifer Granholm* Lyn Jeffery Maria S. Salinas Former Governor, State of Michigan President & CEO, Los Angeles Area *Resigned from Commission Ilana Lipsett Chamber of Commerce upon nomination -
Near-Death Experiences and the Theory of the Extraneuronal Hyperspace
Near-Death Experiences and the Theory of the Extraneuronal Hyperspace Linz Audain, J.D., Ph.D., M.D. George Washington University The Mandate Corporation, Washington, DC ABSTRACT: It is possible and desirable to supplement the traditional neu rological and metaphysical explanatory models of the near-death experience (NDE) with yet a third type of explanatory model that links the neurological and the metaphysical. I set forth the rudiments of this model, the Theory of the Extraneuronal Hyperspace, with six propositions. I then use this theory to explain three of the pressing issues within NDE scholarship: the veridicality, precognition and "fear-death experience" phenomena. Many scholars who write about near-death experiences (NDEs) are of the opinion that explanatory models of the NDE can be classified into one of two types (Blackmore, 1993; Moody, 1975). One type of explana tory model is the metaphysical or supernatural one. In that model, the events that occur within the NDE, such as the presence of a tunnel, are real events that occur beyond the confines of time and space. In a sec ond type of explanatory model, the traditional model, the events that occur within the NDE are not at all real. Those events are merely the product of neurobiochemical activity that can be explained within the confines of current neurological and psychological theory, for example, as hallucination. In this article, I supplement this dichotomous view of explanatory models of the NDE by proposing yet a third type of explanatory model: the Theory of the Extraneuronal Hyperspace. This theory represents a Linz Audain, J.D., Ph.D., M.D., is a Resident in Internal Medicine at George Washington University, and Chief Executive Officer of The Mandate Corporation. -
On the First Electromagnetic Measurement of the Velocity of Light by Wilhelm Weber and Rudolf Kohlrausch
Andre Koch Torres Assis On the First Electromagnetic Measurement of the Velocity of Light by Wilhelm Weber and Rudolf Kohlrausch Abstract The electrostatic, electrodynamic and electromagnetic systems of units utilized during last century by Ampère, Gauss, Weber, Maxwell and all the others are analyzed. It is shown how the constant c was introduced in physics by Weber's force of 1846. It is shown that it has the unit of velocity and is the ratio of the electromagnetic and electrostatic units of charge. Weber and Kohlrausch's experiment of 1855 to determine c is quoted, emphasizing that they were the first to measure this quantity and obtained the same value as that of light velocity in vacuum. It is shown how Kirchhoff in 1857 and Weber (1857-64) independently of one another obtained the fact that an electromagnetic signal propagates at light velocity along a thin wire of negligible resistivity. They obtained the telegraphy equation utilizing Weber’s action at a distance force. This was accomplished before the development of Maxwell’s electromagnetic theory of light and before Heaviside’s work. 1. Introduction In this work the introduction of the constant c in electromagnetism by Wilhelm Weber in 1846 is analyzed. It is the ratio of electromagnetic and electrostatic units of charge, one of the most fundamental constants of nature. The meaning of this constant is discussed, the first measurement performed by Weber and Kohlrausch in 1855, and the derivation of the telegraphy equation by Kirchhoff and Weber in 1857. Initially the basic systems of units utilized during last century for describing electromagnetic quantities is presented, along with a short review of Weber’s electrodynamics. -
Back Or to the Future? Preferences of Time Travelers
Judgment and Decision Making, Vol. 7, No. 4, July 2012, pp. 373–382 Back or to the future? Preferences of time travelers Florence Ettlin∗ Ralph Hertwig† Abstract Popular culture reflects whatever piques our imagination. Think of the myriad movies and books that take viewers and readers on an imaginary journey to the past or the future (e.g., Gladiator, The Time Machine). Despite the ubiquity of time travel as a theme in cultural expression, the factors that underlie people’s preferences concerning the direction of time travel have gone unexplored. What determines whether a person would prefer to visit the (certain) past or explore the (uncertain) future? We identified three factors that markedly affect people’s preference for (hypothetical) travel to the past or the future, respectively. Those who think of themselves as courageous, those with a more conservative worldview, and—perhaps counterintuitively—those who are advanced in age prefer to travel into the future. We discuss implications of these initial results. Keywords: time travel; preferences; age; individual differences; conservative Weltanschauung. 1 Introduction of the future. But what determines whether the cultural time machine’s lever is pushed forward to an unknown 1.1 Hypothetical time traveling: A ubiqui- future or back to a more certain past? tous yet little understood activity Little is known about the factors that determine peo- ple’s preferences with regard to the “direction” of time “I drew a breath, set my teeth, gripped the starting lever travel. Past investigations of mental time travel have typ- with both hands, and went off with a thud” (p. -
The Fine Structure of Weber's Hydrogen Atom: Bohr–Sommerfeld Approach
Z. Angew. Math. Phys. (2019) 70:105 c 2019 Springer Nature Switzerland AG 0044-2275/19/040001-12 published online June 21, 2019 Zeitschrift f¨ur angewandte https://doi.org/10.1007/s00033-019-1149-4 Mathematik und Physik ZAMP The fine structure of Weber’s hydrogen atom: Bohr–Sommerfeld approach Urs Frauenfelder and Joa Weber Abstract. In this paper, we determine in second order in the fine structure constant the energy levels of Weber’s Hamiltonian that admit a quantized torus. Our formula coincides with the formula obtained by Wesley using the Schr¨odinger equation for Weber’s Hamiltonian. We follow the historical approach of Sommerfeld. This shows that Sommerfeld could have discussed the fine structure of the hydrogen atom using Weber’s electrodynamics if he had been aware of the at-his-time-already- forgotten theory of Wilhelm Weber (1804–1891). Mathematics Subject Classification. 53Dxx, 37J35, 81S10. Keywords. Semiclassical quantization, Integrable system, Hamiltonian system. Contents 1. Introduction 1 2. Weber’s Hamiltonian 3 3. Quantized tori 4 4. Bohr–Sommerfeld quantization 6 Acknowledgements 7 A. Weber’s Lagrangian and delayed potentials 8 B. Proton-proton system—Lorentzian metric 10 References 10 1. Introduction Although Weber’s electrodynamics was highly praised by Maxwell [22,p.XI],seealso[4, Preface],, it was superseded by Maxwell’s theory and basically forgotten. In contrast to Maxwell’s theory, which is a field theory, Weber’s theory is a theory of action-at-a-distance, like Newton’s theory. Weber’s force law can be used to explain Amp`ere’s law and Faraday’s induction law; see [4, Ch. -
Rotation Matrix - Wikipedia, the Free Encyclopedia Page 1 of 22
Rotation matrix - Wikipedia, the free encyclopedia Page 1 of 22 Rotation matrix From Wikipedia, the free encyclopedia In linear algebra, a rotation matrix is a matrix that is used to perform a rotation in Euclidean space. For example the matrix rotates points in the xy -Cartesian plane counterclockwise through an angle θ about the origin of the Cartesian coordinate system. To perform the rotation, the position of each point must be represented by a column vector v, containing the coordinates of the point. A rotated vector is obtained by using the matrix multiplication Rv (see below for details). In two and three dimensions, rotation matrices are among the simplest algebraic descriptions of rotations, and are used extensively for computations in geometry, physics, and computer graphics. Though most applications involve rotations in two or three dimensions, rotation matrices can be defined for n-dimensional space. Rotation matrices are always square, with real entries. Algebraically, a rotation matrix in n-dimensions is a n × n special orthogonal matrix, i.e. an orthogonal matrix whose determinant is 1: . The set of all rotation matrices forms a group, known as the rotation group or the special orthogonal group. It is a subset of the orthogonal group, which includes reflections and consists of all orthogonal matrices with determinant 1 or -1, and of the special linear group, which includes all volume-preserving transformations and consists of matrices with determinant 1. Contents 1 Rotations in two dimensions 1.1 Non-standard orientation -
NASA Tit It-462 &I -- .7, F
N ,! S’ A TECHNICAL, --NASA Tit it-462 &I REP0R.T .7,f ; .A. SPACE-TIME. TENsOR FQRMULATION _ ,~: ., : _. Fq. CONTINUUM MECHANICS IN ’ -. :- -. GENERAL. CURVILINEAR, : MOVING, : ;-_. \. AND DEFQRMING COORDIN@E. SYSTEMS _. Langley Research Center Ehnpton, - Va. 23665 NATIONAL AERONAUTICSAND SPACE ADhiINISTRATI0.N l WASHINGTON, D. C. DECEMBER1976 _. TECHLIBRARY KAFB, NM Illllll lllllIII lllll luII Ill Ill 1111 006857~ ~~_~- - ;. Report No. 2. Government Accession No. 3. Recipient’s Catalog No. NASA TR R-462 5. Report Date A SPACE-TIME TENSOR FORMULATION FOR CONTINUUM December 1976 MECHANICS IN GENERAL CURVILINEAR, MOVING, AND 6. Performing Organization Code DEFORMING COORDINATE SYSTEMS 7. Author(s) 9. Performing Orgamzation Report No. Lee M. Avis L-10552 10. Work Unit No. 9. Performing Organization Name and Address 1’76-30-31-01 NASA Langley Research Center 11. Contract or Grant No. Hampton, VA 23665 13. Type of Report and Period Covered 2. Sponsoring Agency Name and Address Technical Report National Aeronautics and Space Administration 14. Sponsoring Agency Code Washington, DC 20546 %. ~u~~l&~tary Notes 6. Abstract Tensor methods are used to express the continuum equations of motion in general curvilinear, moving, and deforming coordinate systems. The space-time tensor formula- tion is applicable to situations in which, for example, the boundaries move and deform. Placing a coordinate surface on such a boundary simplifies the boundary-condition treat- ment. The space-time tensor formulation is also applicable to coordinate systems with coordinate surfaces defined as surfaces of constant pressure, density, temperature, or any other scalar continuum field function. The vanishing of the function gradient com- ponents along the coordinate surfaces may simplify the set of governing equations. -
Weber's Law and Mach's Principle
Weber's Law and Mach's Principle Andre K. T. Assis 1. Introduction Recently we applied a Weber's force law for gravitation to implement quantitatively Mach's Principle (Assis 1989, 1992a). In this work we present a briefreview of Weher's electrodynamics and analyze in greater detail the compliance of a Weber's force law for gravitation with Mach's Principle. 2. Weber's Electrodynamics In this section we discuss Weber's original work as applied to electro magnetism. For detailed references of Weber's electrodynamics, see (Assis 1992b, 1994). In order to unify electrostatics (Coulomb's force, Gauss's law) with electrodynamics (Ampere's force between current elements), W. Weber proposed in 1846 that the force exerted by an electrical charge q2 on another ql should be given by (using vectorial notation and in the International System of Units): (1) In this equation, (;0=8.85'10- 12 Flm is the permittivity of free space; the position vectors of ql and qz are r 1 and r 2, respectively; the distance between the charges is r lZ == Ir l - rzl '" [(Xl -XJ2 + (yj -yJZ + (Zl -ZJ2j112; r12=(r) -r;JlrI2 is the unit vector pointing from q2 to ql; the radial velocity between the charges is given by fIZ==drlzfdt=rI2'vIZ; and the Einstein Studies, vol. 6: Mach's Principle: From Newton's Bucket to Quantum Gravity, pp. 159-171 © 1995 Birkhliuser Boston, Inc. Printed in the United States. 160 Andre K. T. Assis radial acceleration between the charges is [VIZ" VIZ - (riZ "VIZ)2 + r lz " a 12J r" where drlz dvlz dTI2 rIZ=rl-rl , V1l = Tt' a'l=Tt= dt2· Moreover, C=(Eo J4J)"'!12 is the ratio of electromagnetic and electrostatic units of charge %=41f·1O-7 N/Al is the permeability of free space).