Michael Faraday: a Virtuous Life Dedicated to Science Citation: F
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James Clerk Maxwell
James Clerk Maxwell JAMES CLERK MAXWELL Perspectives on his Life and Work Edited by raymond flood mark mccartney and andrew whitaker 3 3 Great Clarendon Street, Oxford, OX2 6DP, United Kingdom Oxford University Press is a department of the University of Oxford. It furthers the University’s objective of excellence in research, scholarship, and education by publishing worldwide. Oxford is a registered trade mark of Oxford University Press in the UK and in certain other countries c Oxford University Press 2014 The moral rights of the authors have been asserted First Edition published in 2014 Impression: 1 All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, without the prior permission in writing of Oxford University Press, or as expressly permitted by law, by licence or under terms agreed with the appropriate reprographics rights organization. Enquiries concerning reproduction outside the scope of the above should be sent to the Rights Department, Oxford University Press, at the address above You must not circulate this work in any other form and you must impose this same condition on any acquirer Published in the United States of America by Oxford University Press 198 Madison Avenue, New York, NY 10016, United States of America British Library Cataloguing in Publication Data Data available Library of Congress Control Number: 2013942195 ISBN 978–0–19–966437–5 Printed and bound by CPI Group (UK) Ltd, Croydon, CR0 4YY Links to third party websites are provided by Oxford in good faith and for information only. -
Electricity Outline
Electricity Outline A. Electrostatics 1. Charge q is measured in coulombs 2. Three ways to charge something. Charge by: Friction, Conduction and Induction 3. Coulomb’s law for point or spherical charges: q1 q2 2 FE FE FE = kq1q2/r r 9 2 2 where k = 9.0 x 10 Nm /Coul 4. Electric field E = FE/qo (qo is a small, + test charge) F = qE Point or spherically symmetric charge distribution: E = kq/r2 E is constant above or below an ∞, charged sheet. 5. Faraday’s Electric Lines of Force rules: E 1. Lines originate on + and terminate on - _ 2. The E field vector is tangent to the line of force + 3. Electric field strength is proportional to line density 4. Lines are ┴ to conducting surfaces. 5. E = 0 inside a hollow or solid conductor 6. Electric potential difference (voltage): ΔV = W/qo We usually drop the Δ and just write V. Sometimes the voltage provided by a battery is know as the electromotive force (emf) ε 7. Potential Energy due to point charges or spherically symmetric charge distribution V= kQ/r 8. Equipotential surfaces are surfaces with constant voltage. The electric field vector is always to an equipotential surface. 9. Emax Air = 3,000,000 N/coul = 30,000 V/cm. If you exceed this value, you will create a conducting path by ripping e-s off air molecules. B. Capacitors 1. Capacitors A. C = q/V; unit of capacitance is the Farad = coul/volt B. For Parallel plate capacitors: V = E d C is proportional to A/d where A is the area of the plates and d is the plate separation. -
Advanced Magnetism and Electromagnetism
ELECTRONIC TECHNOLOGY SERIES ADVANCED MAGNETISM AND ELECTROMAGNETISM i/•. •, / .• ;· ... , -~-> . .... ,•.,'. ·' ,,. • _ , . ,·; . .:~ ~:\ :· ..~: '.· • ' ~. 1. .. • '. ~:;·. · ·!.. ., l• a publication $2 50 ADVANCED MAGNETISM AND ELECTROMAGNETISM Edited by Alexander Schure, Ph.D., Ed. D. - JOHN F. RIDER PUBLISHER, INC., NEW YORK London: CHAPMAN & HALL, LTD. Copyright December, 1959 by JOHN F. RIDER PUBLISHER, INC. All rights reserved. This book or parts thereof may not be reproduced in any form or in any language without permission of the publisher. Library of Congress Catalog Card No. 59-15913 Printed in the United States of America PREFACE The concepts of magnetism and electromagnetism form such an essential part of the study of electronic theory that the serious student of this field must have a complete understanding of these principles. The considerations relating to magnetic theory touch almost every aspect of electronic development. This book is the second of a two-volume treatment of the subject and continues the attention given to the major theoretical con siderations of magnetism, magnetic circuits and electromagnetism presented in the first volume of the series.• The mathematical techniques used in this volume remain rela tively simple but are sufficiently detailed and numerous to permit the interested student or technician extensive experience in typical computations. Greater weight is given to problem solutions. To ensure further a relatively complete coverage of the subject matter, attention is given to the presentation of sufficient information to outline the broad concepts adequately. Rather than attempting to cover a large body of less important material, the selected major topics are treated thoroughly. Attention is given to the typical practical situations and problems which relate to the subject matter being presented, so as to afford the reader an understanding of the applications of the principles he has learned. -
Characterization and Design Requirements for Antennas in the Near-field and the Random-LOS Propagation Environment
Thesis for the Degree of Doctor of Philosophy Characterization and Design Requirements for Antennas in the Near-field and the Random-LOS Propagation Environment Aidin Razavi Department of Signals and Systems Chalmers University of Technology Göteborg, Sweden 2016 Characterization and Design Requirements for Antennas in the Near-field and the Random-LOS Propagation Environment Aidin Razavi ISBN 978-91-7597-494-1 c Aidin Razavi, 2016. Doktorsavhandlingar vid Chalmers tekniska högskola Ny serie nr 4175 ISSN 0346-718X Department of Signals and Systems Antenna Systems Division Chalmers University of Technology SE–412 96 Göteborg Sweden Telephone: +46 (0)31 – 772 1000 Email: [email protected] [email protected] Typeset by the author using LATEX. Chalmers Reproservice Göteborg, Sweden 2016 To Baba, Maman, Azin and my beloved Maryam Abstract The choice of antenna for a particular application depends on the require- ments imposed by that application. These include the field region (i.e., near-field or far-field), polarization, radiation pattern, radiation efficiency, system throughput, etc. Accordingly, during an antenna’s design process, different characteristics and characterization methods have to be taken into account. The present thesis focuses on two different aspects of antenna characterization and design: The first concerns antennas in near-field ap- plications dealing with lossy materials. The second is on the Over-The-Air (OTA) measurements of wireless devices and the Random-Line-Of-Sight (Random-LOS) environment. The characterization, design criteria, and fundamental limitations of antennas in the near-field, especially in lossy media, have not been addressed as thoroughly as in the far-field. -
08. Ampère and Faraday Darrigol (2000), Chap 1
08. Ampère and Faraday Darrigol (2000), Chap 1. A. Pre-1820. (1) Electrostatics (frictional electricity) • 1780s. Coulomb's description: ! Two electric fluids: positive and negative. ! Inverse square law: It follows therefore from these three tests, that the repulsive force that the two balls -- [which were] electrified with the same kind of electricity -- exert on each other, Charles-Augustin de Coulomb follows the inverse proportion of (1736-1806) the square of the distance."" (2) Magnetism: Coulomb's description: • Two fluids ("astral" and "boreal") obeying inverse square law. • No magnetic monopoles: fluids are imprisoned in molecules of magnetic bodies. (3) Galvanism • 1770s. Galvani's frog legs. "Animal electricity": phenomenon belongs to biology. • 1800. Volta's ("volatic") pile. Luigi Galvani (1737-1798) • Pile consists of alternating copper and • Charged rod connected zinc plates separated by to inner foil. brine-soaked cloth. • Outer foil grounded. • A "battery" of Leyden • Inner and outer jars that can surfaces store equal spontaeously recharge but opposite charges. themselves. 1745 Leyden jar. • Volta: Pile is an electric phenomenon and belongs to physics. • But: Nicholson and Carlisle use voltaic current to decompose Alessandro Volta water into hydrogen and oxygen. Pile belongs to chemistry! (1745-1827) • Are electricity and magnetism different phenomena? ! Electricity involves violent actions and effects: sparks, thunder, etc. ! Magnetism is more quiet... Hans Christian • 1820. Oersted's Experimenta circa effectum conflictus elecrici in Oersted (1777-1851) acum magneticam ("Experiments on the effect of an electric conflict on the magnetic needle"). ! Galvanic current = an "electric conflict" between decompositions and recompositions of positive and negative electricities. ! Experiments with a galvanic source, connecting wire, and rotating magnetic needle: Needle moves in presence of pile! "Otherwise one could not understand how Oersted's Claims the same portion of the wire drives the • Electric conflict acts on magnetic poles. -
A Beautiful Approach: Transformational Optics
A beautiful approach: “Transformational optics” [ several precursors, but generalized & popularized by Ward & Pendry (1996) ] warp a ray of light …by warping space(?) [ figure: J. Pendry ] Euclidean x coordinates transformed x'(x) coordinates amazing Solutions of ordinary Euclidean Maxwell equations in x' fact: = transformed solutions from x if x' uses transformed materials ε' and μ' Maxwell’s Equations constants: ε0, μ0 = vacuum permittivity/permeability = 1 –1/2 c = vacuum speed of light = (ε0 μ0 ) = 1 ! " B = 0 Gauss: constitutive ! " D = # relations: James Clerk Maxwell #D E = D – P 1864 Ampere: ! " H = + J #t H = B – M $B Faraday: ! " E = # $t electromagnetic fields: sources: J = current density E = electric field ρ = charge density D = displacement field H = magnetic field / induction material response to fields: B = magnetic field / flux density P = polarization density M = magnetization density Constitutive relations for macroscopic linear materials P = χe E ⇒ D = (1+χe) E = ε E M = χm H B = (1+χm) H = μ H where ε = 1+χe = electric permittivity or dielectric constant µ = 1+χm = magnetic permeability εµ = (refractive index)2 Transformation-mimicking materials [ Ward & Pendry (1996) ] E(x), H(x) J–TE(x(x')), J–TH(x(x')) [ figure: J. Pendry ] Euclidean x coordinates transformed x'(x) coordinates J"JT JµJT ε(x), μ(x) " ! = , µ ! = (linear materials) det J det J J = Jacobian (Jij = ∂xi’/∂xj) (isotropic, nonmagnetic [μ=1], homogeneous materials ⇒ anisotropic, magnetic, inhomogeneous materials) an elementary derivation [ Kottke (2008) ] consider× -
Fabrication and Characterization of Hybrid Energy Harvesting Microdevices Zhongcheng Gong
Louisiana Tech University Louisiana Tech Digital Commons Doctoral Dissertations Graduate School Spring 2012 Fabrication and characterization of hybrid energy harvesting microdevices Zhongcheng Gong Follow this and additional works at: https://digitalcommons.latech.edu/dissertations Part of the Electrical and Computer Engineering Commons, and the Nanoscience and Nanotechnology Commons FABRICATION AND CHARACTERIZATION OF HYBRID ENERGY HARVESTING MICRODEVICES by Zhongcheng Gong, B.E., M.S. A Dissertation Presented in Partial Fulfillment of the Requirement for the Degree Doctor of Philosophy COLLEGE OF ENGINEERING AND SCIENCE LOUISIANA TECH UNIVERSITY May 2012 UMI Number: 3515931 All rights reserved INFORMATION TO ALL USERS The quality of this reproduction is dependent upon the quality of the copy submitted. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if material had to be removed, a note will indicate the deletion. DiygrMution UMI 3515931 Published by ProQuest LLC 2012. Copyright in the Dissertation held by the Author. Microform Edition © ProQuest LLC. All rights reserved. This work is protected against unauthorized copying under Title 17, United States Code. ProQuest LLC 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 48106-1346 LOUISIANA TECH UNIVERSITY THE GRADUATE SCHOOL 3-2012 Date We hereby recommend that the dissertation prepared under our supervision by Zhorigcheng Gong entitled Fabrication and Characterization of Hybrid Energy Harvesting Microdevices be accepted in partial fulfillment of the requirements for the Degree of Doctor of Philosophy Long Que I of Department College of Engineering & Science Department Recommendation concurred in: Chester Wilson Hisham E. -
Faraday and the Electromagnetic Theory of Light - Openmind Search Private Area
8/9/2015 Faraday and the Electromagnetic Theory of Light - OpenMind Search Private area Sharing knowledge for a better future Home Faraday and the Electromagnetic Theory of Light Faraday and the Electromagnetic Theory of Light Share 24 August 2015 Physics, Science Sign in or register to rate this publication Michael Faraday (1791-1867) is probably best known for his discovery of electromagnetic induction, his contributions to electrical engineering and electrochemistry or due to the fact that he was responsible for introducing the concept of field in physics to describe electromagnetic interaction. But perhaps it is not so well known that he also made fundamental contributions to the electromagnetic theory of light. In 1845, just 170 years ago, Faraday discovered that a magnetic field influenced polarized light – a phenomenon known as the magneto-optical effect or Faraday effect. To be precise, he found that the plane of vibration of a beam of linearly polarized light incident on a piece of glass rotated when a magnetic field was applied in the direction of propagation of the beam. This was one of the first indications that electromagnetism and light were related. The following year, in May 1846, Faraday published the article Thoughts on Ray Vibrations, a prophetic publication in which he speculated that light could be a vibration of the electric and magnetic lines of force. Michael Faraday (1791-1867) / Credits: Wikipedia Faraday’s case is not common in the history of physics: although his training was very basic, the laws of electricity and magnetism are due much more to Faraday’s experimental discoveries than to any other https://www.bbvaopenmind.com/en/faraday-electromagnetic-theory-light/ 1/7 8/9/2015 Faraday and the Electromagnetic Theory of Light - OpenMind scientist. -
Energy Pioneers
Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Energy Pioneers The following pages will give an overview about famous people in history who studied energy and invented useful things we still use today. Read about these people then complete the matching activity on the last page. For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Thomas Edison (1847) Information comes from the Department of Energy, including sourced pictures. Source: Wikimedia Commons (Public Domain) Born in 1847. Not a very good student. Created many inventions including the phonograph (similar to a record player), the light bulb, the first power plant and the first movie camera. One of his most famous quotes is, “Invention is one percent inspiration and ninety-nine percent perspiration.” For more great energy resources visit: www.ConsumersEnergy.com/kids © 2015 Consumers Energy. All rights reserved. Providing energy education to students in the communities we serve. That’s our Promise to Michigan. Marie Curie (1867) Information comes from the Department of Energy, including sourced pictures. Source: Nobel Foundation, Wikimedia Commons (Public Domain) Born in 1867. Learned to read at 4. There were no universities in her native Poland that accepted women, so she had to move to France to attend college. She, along with her husband, discovered the first radioactive element. In 1903, she was awarded the Nobel Prize in Physics for the discovery of radium. Marie Curie was the first woman to win a Nobel Prize in Physics. -
Radio Science Bulletin Staff
INTERNATIONAL UNION UNION OF RADIO-SCIENTIFIQUE RADIO SCIENCE INTERNATIONALE ISSN 1024-4530 Bulletin Vol. 2017, No. 363 December 2017 Radio Science URSI, c/o Ghent University (INTEC) St.-Pietersnieuwstraat 41, B-9000 Gent (Belgium) Contents Radio Science Bulletin Staff ....................................................................................... 3 URSI Offi cers and Secretariat.................................................................................... 6 Editor’s Comments ..................................................................................................... 8 On Low-Pass, High-Pass, Bandpass, and Stop-Band NGD RF Passive Circuits 10 Recent Developments in Distributed Negative-Group-Delay Circuits .................28 A Zero-Order-Closure Turbulent Flux-Conservation Technique for Blending Refractivity Profi les in the Marine Atmospheric Boundary layer ................... 39 Conformal Antennas for Miniature In-Body Devices: The Quest to Improve Radiation Performance ........................................................................................ 52 In Memoriam: Jean Van Bladel ............................................................................... 65 In Memoriam: Karl Rawer ...................................................................................... 66 In Memoriam: Thomas J. (Tom) Brazil .................................................................. 68 Et Cetera .................................................................................................................... 70 -
From Carlo Matteucci to Giuseppe Moruzzi
THE INTERNATIONAL MEETING : FROM CARLO MATTEUCCI TO GIUSEPPE MORUZZI : TWO CENTURIES OF EUROPEAN PHYSIOLOGY A SATELLITE OF THE 15 TH ANNUAL MEETING OF THE INTERNATIONAL SOCIETY FOR THE HISTORY OF THE NEUROSCIENCES , ITALY, VILLA DI CORLIANO PISA 22-26 JUNE 2010 SPONSORING INSTITUTIONS Club d'histoire des neurosciences de la Société des Neurosciences, Paris. Galileo Museum, Firenze International Society for the History of Neurosciences. Università di Ferrara. Università di Pavia - Sistema Museale d’Ateneo. Université Pierre et Marie Curie – Paris. Université Diderot – Paris. Organizing Committee: Jean- Gaël Barbara, Cesira Batini, Michel Meulders, Marco Piccolino and Nicholas J. Wade. FINAL PROGRAM ND TUESDAY JUNE 22 VILLA DI CORLIANO 9:30-9:45 WELCOME BY THE HOSTS 9:45-10:15 HISTORICAL INTRODUCTION Alessandro Baldassari: The "Villa of Corliano " between art and history 10:15-11:45 OPENING SESSION : INTRODUCING MATTEUCCI AND MORUZZI : 10:15 Marco Piccolino, Ferrara. The electrophysiological work of Carlo Matteucci. 10:45 Michel Meulders Giuseppe Moruzzi: scientist and humanist. 11:15 COFFEE BREAK 11:45-12:15 Rita Levi-Montalcini, Roma. Giuseppe Moruzzi, a “formidable” scientist and a "formidable” man. 12:15 APERITIF AND LUNCH 15:00-16:00 MATTEUCCI AND HIS TIME 15:00 Simone Contardi and Mara Miniati, Firenze: Educating heart and mind: Vincenzo Antinori and the scientific culture in thee nineteenth century Florence. 15:30 Renato Mazzolini, Trento, Italy: Carlo Matteucci, between France and Italy. 16:00 COFFEE BREAK 16:15-18:30 THE BEGINNING AND DEVELOPMENT OF ELECTROPHYSIOLOGY 16:30 Nicholas J. Wade, Dundee, Stimulating the senses . 17:00 Marco Bresadola, Ferrara: Matteucci and the legacy of Luigi Galvani . -
Maxwell Discovers That Light Is Electromagnetic Waves in 1862
MAXWELL DISCOVERS LIGHT IS ELECTROMAGNETIC WAVES James Clerk Maxwell was a Scottish scientist. He worked in the mid-nineteenth century in Scotland and England. At that time, electricity and magnetism had been extensively studied, and it was known since 1831 that electric current produces magnetism. Maxwell added the idea that changing magnetism could produce electricity. The term that Maxwell added to the known equations (called Ampere's law) for magnetism allowed Maxwell to see that there were wave-like solutions, that is, solutions that look like a sine wave (as a function of time). The numbers in Maxwell's equations all came from laboratory experiments on electric- ity and magnetism. There was nothing in those equations about light, and radio waves were completely unknown at the time, so the existence of electromagnetic waves was also completely unknown. But mathematics showed that Maxwell's equations had wave-like solutions. What did that mean? Maxwell proceeded to calculate the speed of those waves, which of course depended on the numbers that came from lab experiments with electricity and magnetism (not with light!). He got the answer 310,740,000 meters per second. Maxwell must have had an \aha moment" when he recognized that number. He did recognize that number: it was the speed of light! He was lecturing at King's College, London, in 1862, and there he presented his result that the speed of propagation of an electromagnetic field is approximately that of the speed of light. He considered this to be more than just a coincidence, and commented: \We can scarcely avoid the conclusion that light consists in the transverse undulations of the same medium which is the cause of electric and magnetic phenomena." 1 2 MAXWELL DISCOVERS LIGHT IS ELECTROMAGNETIC WAVES He published his work in his 1864 paper, A dynamical theory of the electromagnetic field.