A History of Electrical Development
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Sparks, Shocks and Voltage Traces As Windows Into Experience: the Spiraled Conductor and Star Wheel Interrupter of Charles Grafton Page
| Sparks, Shocks and Voltage Traces as Windows into Experience | 123 | Sparks, Shocks and Voltage Traces as Windows into Experience: The Spiraled Conductor and Star Wheel Interrupter of Charles Grafton Page Elizabeth CAVICCHI a T Abstract When battery current flowing in his homemade spiraled conductor switched off, nineteenth century experimenter Charles Grafton Page saw sparks and felt shocks, even in parts of the spiral where no current passed. Reproducing his experiment today is improvisational: an oscilloscope replaces Page’s body; a copper star spinning through galinstan substitutes for Barlow’s wheel interrupter. Green and purple flashes accompanied my spinning wheel. Unlike what Page’s shocks showed, induced voltages probed across my spiral’s wider spans were variable, precipitating extensive explorations of its resonant fre - quencies. Redoing historical experiments extends our experience, fostering new observations about natural phenomena and experimental development. Keywords: electromagnetic induction, historical replication, Charles Grafton Page, exploratory learning, spiral, Barlow wheel, galinstan, autotransformer T Introduction real? Facing wires and wiggling magnetic needles firsthand, while trying to make sense of it, deepens Historical experiments come to us in fragments: our perspective; we become confused and curious handwritten data, published reports, and often non - (Cavicchi 2003). Redoing an experiment is not just a functioning apparatus. A further carry-over may per - check on facts, dates, whether Oersted’s needle went sist in ideas, procedures, materials and inventions east or west. It gives us access to experience congru - bearing imprints of the prior work. All these are clues ous with the past: “’to know an experimenter, you to something both more transitory and more coher - should replicate her study’” (Kurz 2001, p. -
Sensor Connectors
Sensor Connectors Thermocouple Connector - Two Pole Assembly Termination Code: 2 • Glass filled thermoplastic body provides high strength at temperatures up to 425°F 218°C) as well as low moisture absorption and good dielectric constant . • Heavy duty hollow pin construction prevents reverse mating of polarity.* • Body color coded to ISA and ANSI standards. 1” • Polarity indicated by symbols molded into body. • Contacts made of thermocouple materials which meet ISA and ANSI standards . • Jack spring loaded to insure firm grip to plug. • Accepts wire sizes to 14 awg. • Single screw cover cap for fast assembly. • Accepts crimp and tube adapter for product from .020 to .375. • Finger grips to permit ease of connection. 7/16” • Quick wiring hook up with large head screws and wire channel. Catalog Number Thermocouple Body Actual Alloy Plugs Jacks Type Color + In Connector - 1/2” LP-J L J-J Iron-Constantan® Black Iron Constantan® LP-K L J-K Chromel®-Alumel® Yellow Chromel® Alumel® 7/8” LP-E L J-E Chromel®-Constantan® Violet Chromel® Constantan® LP-T L J-T Copper-Constantan® Blue Copper Constantan® 1 3/8” LP-R/S L J-R/S Platinum/Rhodium- Green Copper #11 Alloy Platinum LP-CU L J-CU Uncompensated White Copper Copper Assembly Termination Code: 5 *Solid pin available on above construction. Add S to Part No. (i.e. LPS-J) Miniature Thermocouple Connector Assembly Termination Code: 3 • Thermoplastic body provides high strength at temperatures up to 425°F (218°C) as well as low moisture absorption and good dielectric constant . • Small, light weight and space saving. -
Smithsonian Miscellaneous Collections
BULLETIN PHILOSOPHICAL SOCIETY WASHINGTON. VOL. IV. Containing the Minutes of the Society from the 185th Meeting, October 9, 1880, to the 2020! Meeting, June 11, 1881. PUBLISHED BY THE CO-OPERATION OF THE SMITHSONIAN INSTITUTION. WASHINGTON JUDD & DETWEILER, PRINTERS, WASHINGTON, D. C. CONTENTS. PAGE. Constitution of the Philosophical Society of Washington 5 Standing Rules of the Society 7 Standing Rules of the General Committee 11 Rules for the Publication of the Bulletin 13 List of Members of the Society 15 Minutes of the 185th Meeting, October 9th, 1880. —Cleveland Abbe on the Aurora Borealis , 21 Minutes of the 186th Meeting, October 25th, 1880. —Resolutions on the decease of Prof. Benj. Peirce, with remarks thereon by Messrs. Alvord, Elliott, Hilgard, Abbe, Goodfellow, and Newcomb. Lester F. Ward on the Animal Population of the Globe 23 Minutes of the 187th Meeting, November 6th, 1880. —Election of Officers of the Society. Tenth Annual Meeting 29 Minutes of the 188th Meeting, November 20th, 1880. —John Jay Knox on the Distribution of Loans in the Bank of France, the National Banks of the United States, and the Imperial of Bank Germany. J. J. Riddell's Woodward on Binocular Microscope. J. S. Billings on the Work carried on under the direction of the National Board of Health, 30 Minutes of the 189th Meeting, December 4th, 1880. —Annual Address of the retiring President, Simon Newcomb, on the Relation of Scientific Method to Social Progress. J. E. Hilgard on a Model of the Basin of the Gulf of Mexico 39 Minutes of the 190th Meeting, December iSth, 1880. -
Chapter 1 Magnetic Circuits and Magnetic Materials
Chapter 1 Magnetic Circuits and Magnetic Materials The objective of this course is to study the devices used in the interconversion of electric and mechanical energy, with emphasis placed on electromagnetic rotating machinery. The transformer, although not an electromechanical-energy-conversion device, is an important component of the overall energy-conversion process. Practically all transformers and electric machinery use ferro-magnetic material for shaping and directing the magnetic fields that acts as the medium for transferring and converting energy. Permanent-magnet materials are also widely used. The ability to analyze and describe systems containing magnetic materials is essential for designing and understanding electromechanical-energy-conversion devices. The techniques of magnetic-circuit analysis, which represent algebraic approximations to exact field-theory solutions, are widely used in the study of electromechanical-energy-conversion devices. §1.1 Introduction to Magnetic Circuits Assume the frequencies and sizes involved are such that the displacement-current term in Maxwell’s equations, which accounts for magnetic fields being produced in space by time-varying electric fields and is associated with electromagnetic radiations, can be neglected. Z H : magnetic field intensity, amperes/m, A/m, A-turn/m, A-t/m Z B : magnetic flux density, webers/m2, Wb/m2, tesla (T) Z 1 Wb =108 lines (maxwells); 1 T =104 gauss Z From (1.1), we see that the source of H is the current density J . The line integral of the tangential component of the magnetic field intensity H around a closed contour C is equal to the total current passing through any surface S linking that contour. -
Joseph Henry
MEMOIR JOSEPH HENRY. SIMON NEWCOMB. BEAD BEFORE THE NATIONAL ACADEMY OP SCIENCES, APRIL 21, 1880. (1) BIOGRAPHICAL MEMOIR OF JOSEPH HENRY. In presenting to the Academy the following notice of its late lamented President the writer feels that an apology is due for the imperfect manner in which he has been obliged to perform the duty assigned him. The very richness of the material has been a source of embarrassment. Few have any conception of the breadth of the field occupied by Professor Henry's researches, or of the number of scientific enterprises of which he was either the originator or the effective supporter. What, under the cir- cumstances, could be said within a brief space to show what the world owes to him has already been so well said by others that it would be impracticable to make a really new presentation without writing a volume. The Philosophical Society of this city has issued two notices which together cover almost the whole ground that the writer feels competent to occupy. The one is a personal biography—the affectionate and eloquent tribute of an old and attached friend; the other an exhaustive analysis of his scientific labors by an honored member of the society well known for his philosophic acumen.* The Regents of the Smithsonian Institution made known their indebtedness to his administration in the memorial services held in his honor in the Halls of Congress. Under these circumstances the onl}*- practicable course has seemed to be to give a condensed resume of Professor Henry's life and works, by which any small occasional gaps in previous notices might be filled. -
Homotopy Perturbation Method with Laplace Transform (LT-HPM) Is Given in “Homotopy Perturbation Method” Section
Tripathi and Mishra SpringerPlus (2016) 5:1859 DOI 10.1186/s40064-016-3487-4 RESEARCH Open Access Homotopy perturbation method with Laplace Transform (LT‑HPM) for solving Lane–Emden type differential equations (LETDEs) Rajnee Tripathi and Hradyesh Kumar Mishra* *Correspondence: [email protected] Abstract Department In this communication, we describe the Homotopy Perturbation Method with Laplace of Mathematics, Jaypee University of Engineering Transform (LT-HPM), which is used to solve the Lane–Emden type differential equa- and Technology, Guna, MP tions. It’s very difficult to solve numerically the Lane–Emden types of the differential 473226, India equation. Here we implemented this method for two linear homogeneous, two linear nonhomogeneous, and four nonlinear homogeneous Lane–Emden type differential equations and use their appropriate comparisons with exact solutions. In the current study, some examples are better than other existing methods with their nearer results in the form of power series. The Laplace transform used to accelerate the convergence of power series and the results are shown in the tables and graphs which have good agreement with the other existing method in the literature. The results show that LT- HPM is very effective and easy to implement. Keywords: Homotopy Perturbation Method (HPM), Laplace Transform (LT), Singular Initial value problems (IVPs), Lane–Emden type equations Background Two astrophysicists, Jonathan Homer Lane and Robert had explained the Lane–Emden type differential equations. In this study, they had designed these types of differential equations, which is a dimensionless structure of Poisson’s equation for the gravitational potential of a self-gravitating, spherically symmetric, polytropic fluid and the thermal behavior of a spherical bunch of gas according to the laws of thermodynamics (Lane 1870; Richardson 1921). -
Design of Magnetic Circuits
Design of Magnetic Circuits Fundamental Equations Circuit laws similar to those of electric circuits apply in magnetic circuits as well. That is, a magnetic circuit can be replaced by an equivalent electric circuit for Ohm’s Law to be applied. If the magnetomotive force of a magnet is F and the total magnetic flux is Φt, and assuming the magnetic resistance (reluctance) of the circuit is R, then the following equation is valid. (1) Assuming the vacant length of the circuit as ℓg and the vacant cross-sectional area as ag, the magnetic resistance is then given by the following equation. (2) μ is the magnetic permeability of the magnetic path and is equivalent to the magnetic permeability μ0 of a vacuum in the case of air. (μ0=4π×10-7 [H/m]) Yoke 〈Figure 7〉 Although the current in an electric circuit rarely leaks outside the circuit, as the difference in the magnetic permeability between the conductor yoke and insulated area in a magnetic circuit is not very large, leakage of the magnetic flux also becomes large in reality. The amount of the magnetic flux leakage is expressed by the leakage factor σ, which is the ratio of the total magnetic flux Φt generated in the magnetic circuit to the effective magnetic flux Φg of the vacant space. (3) In addition, the loss in the magnetic flux due to the joints in the magnetic circuit must also be taken into consideration. This is represented by the reluctance factor f. Since the leakage factor σ is equivalent to the increase in the vacant space area, and the reluctance factor f refers to the correction coefficient of the vacant space length, the corrected magnetic resistance becomes as follows. -
!History of Lightingv2.Qxd
CONTENTS Introduction 3 The role of lighting in modern society 3 1. The oldest light sources 4 Before the advent of the lamp 4 The oldest lamps 4 Candles and torches 5 Further development of the oil lamp 6 2. Gaslight 9 Introduction 9 Early history 9 Gas production 10 Gaslight burners 10 The gas mantle 11 3. Electric lighting before the incandescent lamp 14 Introduction 14 Principle of the arc lamp 15 Further development of the arc lamp 16 Applications of the arc lamp 17 4. The incandescent lamp 20 The forerunners 20 The birth of the carbon-filament lamp 22 Further development of the carbon-filament lamp 25 Early metal-filament lamps 27 The Nernst lamp 28 The birth of the tungsten-filament lamp 29 Drawn tungsten filaments 30 Coiled filaments 30 The halogen incandescent lamp 31 5. Discharge lamps 32 Introduction 32 The beginning 32 High-voltage lamps 33 Early low-pressure mercury lamps 34 The fluorescent lamp 35 High-pressure mercury lamps 36 Sodium lamps 37 The xenon lamp 38 6. Electricity production and distribution 39 Introduction 39 Influence machines and batteries 39 Magneto-electric generators 40 Self-exciting generators 41 The oldest public electricity supply systems 41 The battle of systems 42 The advent of modern a.c. networks 43 The History of Light and Lighting While the lighting industry is generally recognized as being born in 1879 with the introduction of Thomas Alva Edison’s incandescent light bulb, the real story of light begins thousands of years earlier. This brochure was developed to provide an extensive look at one of the most important inventions in mankind’s history: artificial lighting. -
A Chronological History of Electrical Development from 600 B.C
From the collection of the n z m o PreTinger JJibrary San Francisco, California 2006 / A CHRONOLOGICAL HISTORY OF ELECTRICAL DEVELOPMENT FROM 600 B.C. PRICE $2.00 NATIONAL ELECTRICAL MANUFACTURERS ASSOCIATION 155 EAST 44th STREET NEW YORK 17, N. Y. Copyright 1946 National Electrical Manufacturers Association Printed in U. S. A. Excerpts from this book may be used without permission PREFACE presenting this Electrical Chronology, the National Elec- JNtrical Manufacturers Association, which has undertaken its compilation, has exercised all possible care in obtaining the data included. Basic sources of information have been search- ed; where possible, those in a position to know have been con- sulted; the works of others, who had a part in developments referred to in this Chronology, and who are now deceased, have been examined. There may be some discrepancies as to dates and data because it has been impossible to obtain unchallenged record of the per- son to whom should go the credit. In cases where there are several claimants every effort has been made to list all of them. The National Electrical Manufacturers Association accepts no responsibility as being a party to supporting the claims of any person, persons or organizations who may disagree with any of the dates, data or any other information forming a part of the Chronology, and leaves it to the reader to decide for him- self on those matters which may be controversial. No compilation of this kind is ever entirely complete or final and is always subject to revisions and additions. It should be understood that the Chronology consists only of basic data from which have stemmed many other electrical developments and uses. -
Joseph Saxton
MEMOIR OP JOSEPH SAXTON. 1799-1873. BY JOSEPH HENRY. HEAD BEFOEB THB NATIONAL ACADEMY, OCT. 4,1874. 28T BIOGRAPHICAL MEMOIR OF JOSEPH SAXTON. MR. PRESIDENT AND GENTLEMEN OF THE ACADEMY :— AT the last session of the National Academy of Sciences I was appointed to prepare an account of the life and labors of our lamented associate, Joseph Saxton, whose death we have been called to mourn. From long acquaintance and friendly relations with the deceased, the discharge of the duty thus devolved upon me has been a labor of love, but had he been personally unknown to me, the preparation of the eulogy would have been none the less a sacred duty, which I was not at liberty on any account to neglect. It is an obligation we owe to the Academy and the world to cherish the memory of our departed associates; their reputation is a precious inheritance to the Academy which exalts its character and extends its usefulness. Man is a sympathetic and imitative being, and through these characteristics of his nature the memories of good men produce an important influence on posterity, and therefore should be cherished and perpetuated. Moreover, the certainty of having a just tribute paid to our memory after our departure is one of the most powerful inducements to purity of life and propriety of deportment. The object of the National Academy is the advancement of science, and no one is considered eligible for membership who has not made positive additions to the sum of human knowledge, or in other words, has not done something to entitle him to the appellation of scientific. -
History of Electric Light
SMITHSONIAN MISCELLANEOUS COLLECTIONS VOLUME 76. NUMBER 2 HISTORY OF ELECTRIC LIGHT BY HENRY SGHROEDER Harrison, New Jersey PER\ ^"^^3^ /ORB (Publication 2717) CITY OF WASHINGTON PUBLISHED BY THE SMITHSONIAN INSTITUTION AUGUST 15, 1923 Zrtie Boxb QSaftitnore (prcee BALTIMORE, MD., U. S. A. CONTENTS PAGE List of Illustrations v Foreword ix Chronology of Electric Light xi Early Records of Electricity and Magnetism i Machines Generating Electricity by Friction 2 The Leyden Jar 3 Electricity Generated by Chemical Means 3 Improvement of Volta's Battery 5 Davy's Discoveries 5 Researches of Oersted, Ampere, Schweigger and Sturgeon 6 Ohm's Law 7 Invention of the Dynamo 7 Daniell's Battery 10 Grove's Battery 11 Grove's Demonstration of Incandescent Lighting 12 Grenet Battery 13 De Moleyns' Incandescent Lamp 13 Early Developments of the Arc Lamp 14 Joule's Law 16 Starr's Incandescent Lamp 17 Other Early Incandescent Lamps 19 Further Arc Lamp Developments 20 Development of the Dynamo, 1840-1860 24 The First Commercial Installation of an Electric Light 25 Further Dynamo Developments 27 Russian Incandescent Lamp Inventors 30 The Jablochkofif " Candle " 31 Commercial Introduction of the Differentially Controlled Arc Lamp ^3 Arc Lighting in the United States 3;^ Other American Arc Light Systems 40 " Sub-Dividing the Electric Light " 42 Edison's Invention of a Practical Incandescent Lamp 43 Edison's Three-Wire System 53 Development of the Alternating Current Constant Potential System 54 Incandescent Lamp Developments, 1884-1894 56 The Edison " Municipal -
Strain Gage Technical Data
STRAIN GAGE TECHNICAL DATA STRAIN GAGE MEASUREMENT The most universal measuring device for the electrical measurement of mechanical quantities is the strain gage. Several types of strain gages depend for their operation on the proportional variance of electrical resistance to strain: the piezoresistive or semi-conductor gage, the carbon resistive gage, the bonded metallic wire, and foil resistance gages. The bonded resistance strain gage is by far the most widely used in experimental stress analysis. This gage consists of a grid of very fine wire or foil bonded to a backing or carrier matrix. The electrical resistance of the grid varies linearly with strain. In use, the carrier matrix is bonded to the surface, force is applied, and the strain is found by measuring the change in resistance. The bonded resistance strain gage is low in cost, can be made with a short gage length, is only moderately affected by the bridge. This method assumes a wiring is located in a time-varying temperature changes, has small linear relationship between voltage magnetic field. out and strain, an initially balanced physical size and low mass, and Magnetic induction can be has fairly high sensitivity to strain. bridge, and a known VIN. In reality, the VOUT-strain relationship is controlled by using twisted lead In a strain gage application, the wires and forming minimum but carrier matrix and the adhesive nonlinear, but for strains up to a few thousand micro-strain, the error is equal loop areas in each side of must work together to transmit the the bridge. strain from the specimen to the grid.