Nineteenth-Century Theories of the Voltaic Pile
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Quantum Mechanics Electromotive Force
Quantum Mechanics_Electromotive force . Electromotive force, also called emf[1] (denoted and measured in volts), is the voltage developed by any source of electrical energy such as a batteryor dynamo.[2] The word "force" in this case is not used to mean mechanical force, measured in newtons, but a potential, or energy per unit of charge, measured involts. In electromagnetic induction, emf can be defined around a closed loop as the electromagnetic workthat would be transferred to a unit of charge if it travels once around that loop.[3] (While the charge travels around the loop, it can simultaneously lose the energy via resistance into thermal energy.) For a time-varying magnetic flux impinging a loop, theElectric potential scalar field is not defined due to circulating electric vector field, but nevertheless an emf does work that can be measured as a virtual electric potential around that loop.[4] In a two-terminal device (such as an electrochemical cell or electromagnetic generator), the emf can be measured as the open-circuit potential difference across the two terminals. The potential difference thus created drives current flow if an external circuit is attached to the source of emf. When current flows, however, the potential difference across the terminals is no longer equal to the emf, but will be smaller because of the voltage drop within the device due to its internal resistance. Devices that can provide emf includeelectrochemical cells, thermoelectric devices, solar cells and photodiodes, electrical generators,transformers, and even Van de Graaff generators.[4][5] In nature, emf is generated whenever magnetic field fluctuations occur through a surface. -
Walter Dominic Wetzels Professor Emeritus
Walter Dominic Wetzels Professor emeritus Ph.D., German Literature, Princeton University Career Highlights Research Focus: Eighteenth-century literature; German literature and science; the literature which popularized science, with particular emphasis on the eighteenth century Education 1965-1968 PhD, German Literature, Princeton University 1964-1965 German Literature, University of Cologne 1949-1954 University of Cologne; Staatsexamen in mathematics and physics Employment 1996- Professor emeritus, Dept. of Germanic Languages, U of Texas at Austin 1984-1996 Professor, Department of Germanic Languages, UT Austin 1973-1984 Associate Professor, Department of Germanic Languages, UT Austin 1968-1973 Assistant Professor, Department of Germanic Languages, UT Austin Awards Spring 1989 University of Texas Faculty Research Assignment Fall 1988 University of Texas Presidential Leave Publications: Books (Edited with Leonard Schulze) Literature and History. Lanham, New York, London: University Press of America, 1983 Johann Wilhelm Ritter: Physik im WIrkungsfeld der deutschen Romantik. Quellen und Forschungen, N.F., 59. Berlin and New York: Walter de Gruyter, 1973. (Edited with and introduction) Myth and Reason. Austin: University of Texas Press, 1973 Publications: Articles "Physics for the Ladies: Early Literary Voices and Strategies For and Against the Popularization of Copernicus and Newton." In: Themes and Structures: Studies in German Literature from Goethe to the Present. Ed. Alexander Stephan. Columbia, SC: Camden House, 1997: 21-38 "Newton for the Ladies: Algarotti's Popularization of Newton's Optics." Studies on Voltaire and the Eighteenth Century. Vol. 304. Oxford: The Voltaire Foundation, 1992: 1152-55 "Johann Wilhelm Ritter: Romantic Physics in Germany." Romanticism and the Sciences, ed. A Cunningham and N. Jardino. Cambridge: Cambridge UP, 1990. -
Electrostatics of Two Suspended Spheres (Eletrost´Atica De Duas Esferas Suspensas)
Revista Brasileira de Ensino de F´ısica, v. 34, n. 3, 3308 (2012) www.sbfisica.org.br Electrostatics of two suspended spheres (Eletrost´atica de duas esferas suspensas) Fernando Fuzinatto Dall'Agnol1, Victor P. Mammana and Daniel den Engelsen Centro de Tecnologia da Informa¸c~aoRenato Archer, Campinas, SP, Brasil Recebido em 25/2/2011; Aceito em 6/2/2012; Publicado em 21/11/2012 Although the working principle of a traditional electroscope with thin metal deflection foils is simple, one needs numerical methods to calculate its foil's deflection. If the electroscope is made of hanging spheres instead of foils, then it is possible to obtain an analytical solution. Since the separation of the charged spheres is of the order of their radius the spheres cannot be described as point charges. We apply the method of image charges to find the electrostatic force between the spheres and then we relate the voltage applied to their separation. We also discuss the similarity with the sphere-plane electrostatic problem. This approach can be used as an analytical solution for practical problems in the field of electrodynamics and its complexity is compatible with undergraduate courses. Keywords: electroscope, electrometer, method of image, image charge, electrostatic, sphere-sphere. Apesar da simplicidade do princ´ıpiode funcionamento do eletrosc´opiotradicional feito de folhas met´alicas finas, ´enecess´ariom´etodos num´ericospara calcular a deflex˜aodas folhas. Se o eletrosc´opiofor feito de esferas penduradas ao inv´esde folhas, ent~ao´eposs´ıvel obter uma solu¸c~aoanal´ıtica. Como a deflex˜aodas esferas car- regadas ´eda ordem dos seus raios, as esferas n~aopodem ser descritas como cargas pontuais. -
Alessandro Volta and the Discovery of the Battery
1 Primary Source 12.2 VOLTA AND THE DISCOVERY OF THE BATTERY1 Alessandro Volta (1745–1827) was born in the Duchy of Milan in a town called Como. He was raised as a Catholic and remained so throughout his life. Volta became a professor of physics in Como, and soon took a significant interest in electricity. First, he began to work with the chemistry of gases, during which he discovered methane gas. He then studied electrical capacitance, as well as derived new ways of studying both electrical potential and charge. Most famously, Volta discovered what he termed a Voltaic pile, which was the first electrical battery that could continuously provide electrical current to a circuit. Needless to say, Volta’s discovery had a major impact in science and technology. In light of his contribution to the study of electrical capacitance and discovery of the battery, the electrical potential difference, voltage, and the unit of electric potential, the volt, were named in honor of him. The following passage is excerpted from an essay, written in French, “On the Electricity Excited by the Mere Contact of Conducting Substances of Different Kinds,” which Volta sent in 1800 to the President of the Royal Society in London, Joseph Banks, in hope of its publication. The essay, described how to construct a battery, a source of steady electrical current, which paved the way toward the “electric age.” At this time, Volta was working as a professor at the University of Pavia. For the excerpt online, click here. The chief of these results, and which comprehends nearly all the others, is the construction of an apparatus which resembles in its effects viz. -
A Fixed Surface Potential Probe with the Swing Capacitive Electrometer
Proc. 2017 Annual Meeting of the Electrostatics of America 1 A Fixed Surface Potential Probe with the Swing Capacitive Electrometer Compared to the Vibrating Kelvin Probe Michael Reznikov Dept. of Integrated Systems Physical Optics Corp., Torrance, CA phone: (1) 310-320-3088 e-mail: [email protected] Abstract— The novel fixed (non-vibrating) Volta potential probe was evaluated in compar- ison with the standard, vibrating (400 Hz) commercial Kelvin probe. While both tested probes demonstrated the similar behavior, there were significant practical advantages of the novel probe. Specifically, the novel probe allows for the elevated distance to the surface and provides more sensitivity to charge under the coating layer. These differences are explained by the analysis of probe circuitry together with the electrostatic approach to the dynamics of the Volta potential measurement. I. INTRODUCTION The capacitive probe method for the measurement of charge induced in the probe elec- trode was proposed by Lord Kelvin (W. Thomson) in 1898 as a capacitive quadrant elec- trometer switching between the immovable probe and discharge shunt while the biasing voltage is applied to the material specimen [1] (see Fig. 1(a)). The using of biasing volt- age and thus the "zero signal" measurement were implemented because the capacitance of the quadrant electrometer is varied during the measurement and thus the measured value depends on the capacitance between the probe electrode and the surface of the specimen. Due to the manual switching and adjustment of biasing voltage, the using of original Kelvin probe was very time-consuming.. In 1932 the vibrating probe method was developed by W.A. -
Volta, the German Controversy on Physics and Naturphilosophie and His Relations with Johann Wilhelm Ritter
Andreas Kleinert Volta, the German Controversy on Physics and Naturphilosophie and his Relations with Johann Wilhelm Ritter A characteristic of German science around 1800 is the violent debate about concepts and methods between the supporters and opponents of a certain philosophy of nature that is generally designed by the German term of Naturphilosophie.1 In the early nineteenth century, physicists who were arguing in the spirit of Naturphilosophie were defined as a community of people that could be sharply distinguished from the “normal” or traditional physicists. This was especially the standpoint of observers from outside Germany.2 But also German physicists spoke of “so-called philosophers of nature who declared that dualism is the principle of order everywhere in physics and chemistry”.3 The philosopher Friedrich Wilhem Schelling, who had given the term of “spekulative Physik”4 to the kind of science by which he wanted to overcome traditional experimental physics and chemistry, is often considered as the ideological forerunner of this group of scientists. Another way of dividing German physicists into different camps was the distinction between “Atomisten” and “Dynamisten”, atomists believing in the existence of matter, including imponderable matter, and dynamists believing only in 1 For more details, see the article of von Engelhardt in this volume. With regard to physics, see CANEVA (1997). 2 See OERSTED (1813). On p. XIV, the translator apologises for translating such an eccentric essay into French and mentions that Naturphilosophie was widely considered as having a detrimental influence on empirical sciences. (“Depuis peu on a fait aux Allemands le reproche très-grave de vouloir porter dans les sciences les spéculations, et pour ainsi dire les rêves d’une imagination exaltée. -
Lab 1 Electrostatics
Electrostatics Goal: To make observations of electrostatic phenomena and interpret the phenomena in terms of the behavior of electric charges. Lab Preparation Most of what you will see in this lab can be explained simply by the following: Like charges repel and unlike charges attract. These repelling and attracting forces that occur can be found using Coulomb’s law, which is stated as !! !! � = � !! where F is the electrostatic force, k is the Coulomb constant (8.99 x 109 Nm2/C2), q1 and q2 are the charges the objects carry, and r is how far apart the objects are. A neutral atom of a substance contains equal amounts of positive and negative charge. The positive charge resides in the nucleus, where each proton carries a charge of +1.602 x 10-19 C. The negative charge is provided by an equal number of electrons associated with and surrounding the nucleus, each carrying a charge of -1.602 x 10-19 C. Macroscopically sized samples of everyday materials usually contain very nearly equal numbers of positive and negative charges. When some dissimilar materials are rubbed together, some charges are transferred from one material to the other leaving each object with a small net charge. For example, when a glass rod is rubbed with silk, the rod usually ends up with a positive charge and the silk ends up with a negative charge. Materials can be cast into two electrical categories: insulators and conductors. The atomic or molecular structure of the material determines whether some charges are free to move (a conductor, such as metallic materials) or largely fixed in place (an insulator). -
Electric Charges Observations Observations
Welcome to PY106 Setting the Channel Number for Your Clicker -The syllabus is your guide to this course. It contains information about the discussions, labs., the class, lab. and 1. Press and release the “CH” button. exam. schedules and grading scheme, etc. 2. While the light is flashing red and green, enter the two digit - Discussion sessions begin today! channel code “41” for this class. - Labs. begin on Jan. 28. 3. After the second digit is entered, press and release the - Assignment 1 is a hand-in, and will be posted on Blackboard “CH” button. The light should flash green to confirm. soon. It is due on Tuesday (Jan. 28) 10:00pm. 4. Press and release the “1/A” button. The light should flash - Most other assignments are posted on WebAssign. To amber ONCE to confirm. If it flashes continuously, there is access the assignment, you need to acquire an access code probably an error and you should try it again. from WebAssign. Instructions for WebAssign can be found in the syllabus. - Lecture notes can be downloaded from http://physics.bu.edu/~okctsui/PY106.html. Note that the URL is case sensitive. 1 2 Electric charges There are two kinds of electric charge, positive and negative. Objects are generally charged by either acquiring extra electrons (a net negative charge), or giving up electrons (a net positive charge). Electric Charge Forces between charged objects can be very large. Such forces are really what stop us from falling through the floor. In other words, what we called the normal force is really associated with repulsive forces between electrons. -
Battery Technologies for Small Scale Embeded Generation
Battery Technologies for Small Scale Embedded Generation. by Norman Jackson, South African Energy Storage Association (SAESA) Content Provider – Wikipedia et al Small Scale Embedded Generation - SSEG • SSEG is very much a local South African term for Distributed Generation under 10 Mega Watt. Internationally they refer to: Distributed generation, also distributed energy, on-site generation (OSG) or district/decentralized energy It is electrical generation and storage performed by a variety of small, grid- connected devices referred to as distributed energy resources (DER) Types of Energy storage: • Fossil fuel storage • Thermal • Electrochemical • Mechanical • Brick storage heater • Compressed air energy storage • Cryogenic energy storage (Battery Energy • Fireless locomotive • Liquid nitrogen engine Storage System, • Flywheel energy storage • Eutectic system BESS) • Gravitational potential energy • Ice storage air conditioning • Hydraulic accumulator • Molten salt storage • Flow battery • Pumped-storage • Phase-change material • Rechargeable hydroelectricity • Seasonal thermal energy battery • Electrical, electromagnetic storage • Capacitor • Solar pond • UltraBattery • Supercapacitor • Steam accumulator • Superconducting magnetic • Thermal energy energy storage (SMES, also storage (general) superconducting storage coil) • Chemical • Biological • Biofuels • Glycogen • Hydrated salts • Starch • Hydrogen storage • Hydrogen peroxide • Power to gas • Vanadium pentoxide History of the battery This was a stack of copper and zinc Italian plates, -
Beyond Autonomy in Eighteenth-Century and German Aesthetics
10 Goethe’s Exploratory Idealism Mattias Pirholt “One has to always experiment with ideas.” Georg Christoph Lichtenberg “Everything that exists is an analogue to all existing things.” Johann Wolfgang Goethe Johann Wolfgang Goethe made his famous Italian journey in the late 1780s, approaching his forties, and it was nothing short of life-c hanging. Soon after his arrival in Rome on November 1, 1786, he writes to his mother that he would return “as a new man”1; in the retroactive account of the journey in Italienische Reise, he famously describes his entrance into Rome “as my second natal day, a true rebirth.”2 Latter- day crit- ics essentially confirm Goethe’s reflections, describing the journey and its outcome as “Goethe’s aesthetic catharsis” (Dieter Borchmeyer), “the artist’s self-d iscovery” (Theo Buck), and a “Renaissance of Goethe’s po- etic genius” (Jane Brown).3 Following a decade of frustrating unproduc- tivity, the Italian sojourn unleashed previously unseen creative powers which would deeply affect Goethe’s life and work over the decades to come. Borchmeyer argues that Goethe’s “new existence in Weimar bore an essentially different signature than his pre- Italian one.”4 With this, Borchmeyer refers to a particular brand of neoclassicism known as Wei- mar classicism, Weimarer Klassik, which is less an epochal term, seeing as it covers only a little more than a decade, than a reference to what Gerhard Schulz and Sabine Doering matter-o f- factly call “an episode in the creative history of a group of German writers around 1800.”5 Equally important as the aesthetic reorientation, however, was Goethe’s new- found interest in science, which was also a direct conse- quence of his encounter with the Italian nature. -
Physics 42 Lab: Static Electricity
Physics 42 Lab: Static Electricity Charge can neither be created nor destroyed: it can only be moved around! The purpose of the lab is to play with static electricity by moving charge around. You will charge objects by friction, induction and polarization and determine the charge with an electroscope. You will draw cute pictures showing each step and how the charges distribute to result in a final charge. The following cartoon sketch is an example of showing how a metallic sphere is charged by induction using a ground. This is the type of sketch you will draw today for each activity, describing what is happening for each step and summarizing your results. I will grade your lab based on neatness and clear explanations! Sample: Charging a metal sphere by induction using a negatively charged rod (a) A neutral metallic sphere, with equal numbers of positive and negative charges. (b) The electrons on the neutral sphere are redistributed when a charged negatively charge rubber rod is placed near the sphere. (c) When the sphere is grounded, some of its electrons leave through the ground wire. (d) When the ground connection is removed while leaving the rod close to the sphere, the sphere has excess positive charge that is nonuniformly distributed. (e) When the rod is removed, the remaining electrons redistribute uniformly and there is a net uniform distribution of positive charge on the sphere. Summary: Charging a neutral metal sphere by induction using a negative rod results in a positive charged sphere! **************************************************************************************** -
Dem-Cfd Analysis of Contact Electrification and Electrostatic Interactions During Powder Handling Processes
DEM-CFD ANALYSIS OF CONTACT ELECTRIFICATION AND ELECTROSTATIC INTERACTIONS DURING POWDER HANDLING PROCESSES CHUNLEI PEI BEng A thesis submitted to the University of Birmingham for the degree of DOCTOR OF PHILOSOPHY School of Chemical Engineering University of Birmingham September 2013 University of Birmingham Research Archive e-theses repository This unpublished thesis/dissertation is copyright of the author and/or third parties. The intellectual property rights of the author or third parties in respect of this work are as defined by The Copyright Designs and Patents Act 1988 or as modified by any successor legislation. Any use made of information contained in this thesis/dissertation must be in accordance with that legislation and must be properly acknowledged. Further distribution or reproduction in any format is prohibited without the permission of the copyright holder. ABSTRACT Electrostatic phenomena are pervasive in powder handling processes. In this study, contact electrification and electrostatic interactions during powder handling processes are explored using the discrete element method coupled with computational fluid dynamics (DEM-CFD), in which contact electrification and electrostatic interaction models are developed and implemented. The effects of particle shape on contact electrification are also investigated, for which multi-sphere methods are adapted and implemented into the DEM-CFD. The electrostatic and dynamic behaviours in various powder handling processes are then analyzed, which include contact electrification of spherical particles during fluidization; electrostatic interactions during deposition of mono-charged and bi-charged particles; contact electrification and electrostatic interactions of spherical particles during fluidization; contact electrification of elongated particles in a vibrating container and particles of arbitrary shapes in a rotating drum.