Umrechnungstafeln1

Total Page:16

File Type:pdf, Size:1020Kb

Umrechnungstafeln1 Umrechnungstafeln1 Maßeinheiten mechanischer und kalorischer Größen Krafteinhelt dyn N kp , i 1 dyn = 1 10-5 i 1,020' 10-6 IN 105 1 ! 1,020' 10-1 1 kp 9,807 ·105 9,807 1 Drehmoment, Arbeit, Energie, erg Nm kpm cal kcal kWh Wärmemenge I 1 erg = 1 dyn cm= 1 10-7 1,020' 10-8 2,388' 10-8 2,388' 10-11 I 2,778' 10-14 1 J=INm=IWs=B 107 1 1,020' 10-1 2,388' 10-1 2,388' 10-4 . 2,778' 10-7 lkpm= 9,807' 107 9,807 1 2,342 2,342' 10-8 2,724· 10-6 I cal = 3 4,187 .107 4,187 4,269.10-1 1 10-3 1,163' 10-6 I kcal = 4,187' 1010 4,187' 103 4,269'102 I 103 1 1,163· 10-3 lkWh= 3,600' 1013 3,600' 108 3,670· 105 8,600' 105 I 8,600' 102 1 Leistung erg/s W i kpm/s PS 7 10 1 erg/s 1 10- 1 1,020' 10-8 1,360' 10- 1 W = 1 J/s = 107 1 1,020,10-1 1,360'10-3 1 kp m/s 9,807 .107 9,807 1 1,333 .10-2 1 PS 7,355' 109 7,355'102 I 75 1 Bezeichnung von Vielfachen und Teilen der Einheit' T Tera- = 1012 h Hekto- = 102 m Milli- = 10-3 G Giga- = 109 da Deka- = 101 IJ, Mikro- = 10-6 M Mega- = 106 d Dezi- = 10-1 n Nano- = 10-9 k Kilo- = 103 c Zenti- = 10-2 P Pico- = 10-12 1 Über die Schreibweise physikalischer Gleichungen s. DIN 1313, 2 Vgl. DIN 1345. 3 1 cal = 1 Gramm-Kalorie; 1 kcal = 1 WE = 103 cal. « Vgl. DIN 1301. Fußrwten zu S. 643. 1 Vgl. DIN 1301, 1339 und 1357. 2 Induktionskonstante (Permeabilität des leeren Raumes) flo = 4 n . 10-9 H/cm = 1,256637 . 10-8 H/cm, 3 Influenzkonstante (Dielektrizitätskonstante des leeren Raumes) BO = 0,88543 . 10-13 F Icm. Fortpflanzungsgeschwindigkeit der elektrischen Wellen im leeren Raum: 'I 1 c = 2,9979' 1010 cmI s, Es g1 t {to' EO =-c2 ' Umrechnungstafeln 643 Maßeinheiten elektrischer und magnetischer Größen l 1 elm = 1 elektromagnetische Einheit im CGS-System 1 es = 1 elektrostatische Einheit im CGS-System Praktisches Maßsystem I CGS-Maßsystem ~-IAb· - ~ Vergleich belder Größe ---- I Ab· Einheit kür-I Einheit kür• Einheiten zung !znng i Elektrische Q 1 Coulomb = 1 Ag C leim I - 1 C = 10-1 elm Ladung I Elektrische U I Volt V 1 elm 1 V = 108 elm Spannung C Elektrische I I Ampere = I B A leim 1 A = 10-1 elm Stromstärke A Elektrische S 1 Ampere/cms I­ leim 1~--- = 10-1 elm em2 Stromdichte V Elektrischer R 1 Ohm = I A !J leIm 1!J = 109 elm Widerstand Spezifischer 10hmem 1 elm l!Jom= elektrischer = 109 elm Widerstand . A Elektrischer G I SIemens = 1 V S leim 1 S = 10-9 elm Leitwert S Elektrische I Siemens/cm leim 1~=1O-gelm om Leitfähigkeit Vs Induktivität L 1 Henry = I T H lelm=lcm 1 H = 109 cm As Elektrische c I Farad = I V F les=lcm 1 F = 9·1011 cm Kapazität Vs Magnetische B 1- 1 elm = 1 Gauß G 1 Va = 108 G em2 ' em2 Induktion Vs (Flußdichte) 1-- = I Tesla = m2 =IT Magnetischer rp I Vs = I Weber Wb leim = I Max­ M 1 Vs = 108 1\1 Induktionsfluß well = 1 Gcm2 A A 4n Magnetische H 1- 1 elm = I Oersted Oe cm 1 cm =10 0e Feldstärke Magnetische v IA A 1 elm = I Gil- Gb 1 A = -~~- Gb Spannung bert = 1 Oe . cm H Vs G Absolute p l 1..!!..=~(} l-Cn} = I Acm Öe om 471: Oe PermeabilitätS V V Elektrische E I~ 1 elm 1- = 108 elm cm Feldstärke om C As C Elektrische D 1 elm 1- 1- = 1O-1 elm l-cm2 = 1 cm2 2 Verschiebung cm Durchflutung I Ampere A 1 elm 1 A = 10-1 elm F As 1 - 1--­ Absolute Di­ e cm - Vcm elektrizitäts• konstante 3 41* Tafel zur geschichtlichen Entwicklung der elektrischen Maschinen und Transformatoren Umlaufende Maschinen Allgemeine Grundlagen und erste Maschinen. 1825 Der Engländer W. STURGEON erfindet den Elektromagneten. 1831 Der Engländer M. FARADAY entdeckt die Gesetze der magnetischen Induktion. 1832 Erste Wechselpol-Wechselstrommaschine mit hin- und hergehender Beweglmg von dem Italiener S. DAL NEGRO. Ein Unbekannter P. M. beschreibt den ersten umlaufenden Wechselstrom­ erzeuger. Der Franzose H. PIXII fertigt den ersten Gleichstromerzeuger an, der zur Stromwendung die Amperesche Wippe verwendet. 1833 Der Engländer W. RITCHIE erfindet den Stromwender. H. F. E. LENZ entdeckt mit seinem Gesetze die Umkehrbarkeit von Motor und Generator. 1834 JACOBI treibt auf der Newa in St. Petersburg ein Boot elektrisch an. 1843 Der Deutsche E. STÖHRER baut die ersten mehrpoligen Maschinen. 1850 Magnetelektrische Maschine der Compagnie l'Alliance nach NOLLET und VAN MALDEREN. 1856 W. SIEMENS gibt den Doppel-T-Anker an, der den ersten Nutenanker darstellt. 1866 W. SIEMENS entdeckt das dynamoelektrische Prinzip, wodurch der Groß• maschinenbau ermöglicht wurde. Gleichstrommaschinen. 1860 Der Italiener A. P ACINOTTI baut eine magnetelektrische Maschine mit geschlossener Ringwicklung und mehrteiligem Stromwender . 1869 Der Belgier Z. TH. GRAMME vereinigt in seinen Maschinen den Ringanker P ACINOTTIS mit dem dynamoelektrischen Prinzip. 1872 Der Deutsche F. v. HEFNER-ALTENECK gibt den Trommelanker an mit einer Einschichtwicklung. 1882 Die Zweischichtwicklung wird von dem Amerikaner E. WESTON zum Patent angemeldet. Erfindung des Nutenankers der neuzeitlichen Maschinen durch den Schweden WENSTRÖM. 1883 THURY stellt vier- und sechspolige Außenpolmaschinen mit Trommelankern her. MORDEY gibt die Ausgleichsverbindungen an. 1884 Der Holländer MENGES gibt die Kompensationswicklung an. 1885 Die Kohlebürste wird in England und Amerika geschaffen. R. H. MATHER gibt die Wendepole an. Die Firma "Alioth" führt die Schablonenwicklung ein. 1887 Der Deutsche W. LAHMEYER entwickelt die Maschine mit eisengeschlossenem Außenpoljoch. 1891 Einführung der mehrgängigen Wellenwicklungen durch den Deutschen E. ARNOLD. Systematische Behandlung der Ankerwicklungen beginnt mit E. ARNOLDS Buch über "Die Ankerwicklungen der Gleichstrom-Dynamo­ maschine" . Tafel zur geschichtl. Entwicklung der elektr. Masohinen und Transformatoren 645 1895 Dreileitermaschine von den Österreichern ALBERT v. ETTINGSHAUSEN und F. PICHLER. 1899 Aufgeschnittene Cleichstromwicklungen von dem Südtiroler G. OSSANNA. 1903 Der AmerikanA!' NOEGGERATH gibt eine Unipolarmaschine an. 1904 Querfeldmasct,me des Wieners E. ROSENBERG. 1908 Theorie der ;:;tromwendung von K. PICKELMAYER. 1929 J. M. PESTARINI erhält einen Preis für seine Arbeiten über die Metadyne oder die I.wischenbürstenmaschinen. 1938 ALEXANDERSON und EDWARDS berichten über die von General Electric Company in Amerika entwickelte Verstärkermaschine Amplidyne. 1947 Der Deutsche O. SOHMUTZ meldet eine Unsymmetrie-Verstärkermaschine zum Patent an. Synchrone Wechselstrommaschinen. 1887 Der Deutsche F. A. HASELWANDER baut eine dreiphasige Ringanker-Innenpol­ maschine. TESLA meldet einen Zweiphasenmotor zum Patent an. BRADLEY entwickelt einen Mehrphasengenerator mit angezapfter Ringanker­ wicklung. 1890 Der Deutsche M. v. DOLIVO-DoBROWOLSKY verwendet zuerst Mantelspulen. 1891 Drehstrom-Kraftübertragung Lauffen-Frankfurt a. M. 1895 C. E. L. BROWN führt die Schirmtype ein. 1901 C. E. L. BROWN erfindet den Walzenturboläufer. 1905 Durch die Arbeiten von A. B. FIELD wird die Wirkung der vom Nutenquerfeld herrührenden zusätzlichen Kupferverluste in Wechselstromwicklungen erkannt. 1911 ROEBEL von Brown, Boveri & eie gibt den Kunststab zur Verminderung der zusätzlichen Verluste an. 1926 bis 1937 Behandlung von Ausgleichsvorgängen bei Synchronmaschinen durch die Amerikaner R. E. DOHERTY, C. A. NICKLE, R. H. PARK, B. L. ROBERTSON und G. KRON. I nduktionsma8chinen. 1885 Der Turiner GALILEO FERRARIS baut ein Modell eines asynchronen Mehr­ phasenmotors. 1887 Zweiphasiger Induktionsmotor mit kurzgeschlossener Phasenwicklung von NICOLA TESLA aus Smiljan (Jugoslawien). 1889 M. V. DOLIVO-DoBROWOLSKY baut den ersten Drehstrommotor mit Einfach- Käfiganker und entwickelt auch den ersten Motor mit Doppelkäfiganker. 1893 Polumschaltbare Ringwicklung der Maschinenfabrik Oerlikon. 1894 Kreisdiagramm von HEYLAND. 1897 Polumschaltbare Trommelwicklung von R. DAHLANDER. 1900 Kreisdiadramm von OSSANNA. H. \V. HOBART beginnt mit der Benutzung des Wirbelstromprinzips im Bau von Käfigankern. 1916 Induktionsmotoren mit Wirbelstromläufern. 1929 Induktionsmotoren mit Doppelstabläufern. Stromwendermotoren für Wechsel- und Drehstrom. Die Erkenntnis, daß ein Gleichstromhauptschlußmotor mit Wechselstrom betrieben werden kann, stammt aus der Mitte der achtziger Jahre. 1883 Nach ELIHU THOMSON laufen Stromwenderanker in Wechselfeldern in der Schaltung von Repulsionsmotoren. 1889 Der Franzose LEBLANO gibt den asynchronen Einankerumformer oder Stromwender-Frequenzwandler an. 1890/91 Der Deutsche GÖRGES erfindet den Drehstrom-Reihenschlußmotor und den ständergespeisten Drehstrom-Nebenschlußmot.or (WINTER-EICHBERG, LATOUR). 646 Tafel zur geschicht!. Entwicklung der elektro Maschinen und Transformatoren 1901 Ständergespeister kompensierter Induktionsmotor nach HEYLAND. 1902 Läufergespeister kompensierter Induktionsmotor nach ÜSNOS. 1900 ... 1904 Die heiden Österreicher F. EICHBERG und G. WINTER schaffen einen kompensierten Repulsionsmotor, den WINTER-EICHBERG-Motor. 1904 Einphasen-Repulsionsmotor mit DoppelbürBtensatz nach M. DER!. 1905 Maschine von LYDALL (SIEMENS-BROTHERS) und SCHERBIUS. 1910 Läufergespeister Drehstrom-Nehenschlußmotor nach SCHRAGE und R. RICHTER. Drehstrom-Reihenschlußmotor mit DoppelbürBtensatz nach M. SCHENKEL. 1925 Kompensierter Freqenzwandler von J. KOZISEK. Umformer. 1853 W. SIEMENS baut einen Gleichstrom-Gleichstrom-Umformer, die "Teller­ maschine" . 1874 Z. TH. GRAMMEl schafft einen Einankerumformer mit Ringanker und zwei Wicklungen. 1887 COERPER führt Einanker-Umformer mit einer Ankerwicklung aus. 1891 W. LAHlIIEYER baut Gleichstrom-Gleichstrom- und Drehstrom-Gleichstrom­ Umformer. Auf der elektrotechnischen Ausstellung in Frankfurt a. M. läuft ein Drehstrom­ Gleichstrom-Einankerumformer mit einer Wicklung (M. V. DOLIVo-DoBRo­ WOLSKY). TransforEnatoren 1831 FARADAY verwendet eine Anordnung bei seinen Versuchen, die sich grund­ sätzlich wenig von einem Transformator unterscheidet; ein geschlossener Eisenring mit zwei Wicklungen. 1851 Der Hannoveraner H. D. RÜHMKORFF verbessert den Funkeninduktor, dessen konstruktive Einzelheiten später heim Bau von Transformatoren als Grund­ lagen dienten. 1856 Der Engländer S. A. VARLEY stellt einen Transformator mit geschlossenem unterteiltem Eisenkreis und den ersten Manteltransformator her und erfindet die Scheibenspulenwicklung. 1877 JABLOCHKOFF schaltet die Primärwicklungen mehrerer Induktionsspulen in Reihe und betreibt von der Sekundärwicklung jeder Spule seine "Kerzen".
Recommended publications
  • Background Information
    Background information Nuremberg, November 3, 2016 A powerful driving force for 150 years The discovery of the dynamo-electric principle has brought about greater changes to the way our society lives than practically any other scientific breakthrough. By inventing the dynamo machine, not only did Werner von Siemens help bring about the advent of electrical machinery, he was also instrumental in accelerating and facilitating industrial processes. Seen from the perspective of society, this completely changed accepted concepts of time and mobility. Werner von Siemens was consequently justified in the confidence he expressed in concluding his report to the Berlin Academy of Sciences in 1867 with the words: “Technology now has the means to generate electrical current of unlimited strength in an inexpensive and convenient way wherever mechanical energy is available.” The first dynamo machines were then also used for the generation of electricity for “light and for galvanic metallurgy and for small electromagnetic machines that get their power from large ones” (Werner von Siemens). 18 years later, Nikola Tesla and Galileo Ferraris independently discovered that alternating currents displaced in time generated a rotating magnetic field with the ability to move an armature. Based on this work, in 1889 the head engineer at AEG, Michail von Dolivo-Dobrowolski, developed the first usable asynchronous motor, whose principle still forms the basis of 85 percent of all practical drive applications today, according to the ZVEI. Siemens AG Wittelsbacherplatz 2 Communications 80333 Munich Head: Clarissa Haller Germany Seite 1/11 Siemens AG Background information Fig. 1: Structure of the dynamo machine This discovery paved the way for mechanizing heavy work such as rolling, drilling, milling and grinding in factory halls.
    [Show full text]
  • Tesla Files His Patents for the Electric Motor
    NUMBERS DON’T LIE_BY VACLAV SMIL OPINION corresponding lecture at the American Institute of Electrical Engineers, one of IEEE’s predecessor societies. However, it was Tesla, helped with generous financ- ing from U.S. investors, who designed not only the AC induction motors but also the requisite AC transformers and dis- tribution system. The two basic patents for his polyphase motor were granted 130 years ago this month. He filed some three dozen more by 1891. In a polyphase motor, each electromag- netic pole in the stator—the stationary housing—has multiple windings, each of which carries alternating current that’s out of phase with current in the other windings. The differing phases induce a current flow that turns the rotor. George Westinghouse acquired Tesla’s AC patents in July 1888. A year later Westinghouse Co. began selling the world’s first small electrical appliance, a fan powered by a 125-watt AC motor. Tesla’s first patent was for a two-phase MAY 1888: motor; modern households now rely on many small, single-phase electric TESLA FILES HIS PATENTS motors. The larger, more efficient three- phase machines are common in indus- trial applications. Mikhail Osipovich FOR THE ELECTRIC MOTOR Dolivo-Dobrovolsky, a Russian engi- neer working as the chief electrician for Germany’s AEG, built the first three- ELECTRICAL DEVICES ADVANCED by leaps and bounds in the 1880s, phase induction motor in 1889. which saw the first commercial generation in centralized power plants, Today, some 12 billion small, non- the first durable lightbulbs, the first transformers, and the first (limited) industrial motors are sold every year, urban grids.
    [Show full text]
  • Induction Motor (Edited from Wikipedia)
    Induction Motor (Edited from Wikipedia) SUMMARY An induction motor or asynchronous motor is an AC electric motor in which the electric current in the rotor needed to make it spin is obtained by electromagnetic induction from the magnetic field of the stator [stationary] winding. An induction motor can therefore be made without electrical connections to the rotor. An induction motor's rotor can be either wound type or squirrel-cage type. Three-phase squirrel-cage induction motors are widely used as industrial drives because they are rugged, reliable and economical. Single-phase induction motors are used extensively for smaller loads, such as household appliances like fans. Although traditionally used in fixed-speed service, induction motors are increasingly being used with variable-frequency drives (VFDs) in variable-speed service. VFDs offer especially important energy savings opportunities. HISTORY In 1824, the French physicist François Arago formulated the existence of rotating magnetic fields, termed Arago's rotations. By manually turning switches on and off, Walter Baily demonstrated this in 1879, effectively the first primitive induction motor. The first commutator-free two phase AC induction motor was invented by Hungarian engineer Ottó Bláthy, he used the two phase motor to propel his invention, the Electricity meter. The first AC commutator-free three-phase induction motors were independently invented by Galileo Ferraris and Nikola Tesla, a working motor model having been demonstrated by the former in 1885 and by the latter in 1887. Tesla applied for US patents in October and November 1887 and was granted some of these patents in May 1888. In April 1888, the Royal Academy of Science of Turin published Ferraris's research on his AC polyphase motor detailing the foundations of motor operation.
    [Show full text]
  • From Volta's Pile to Ferraris' Motor
    S. D’Agostino, S. Leva, A.P. Morando From Volta’s Pile to Ferraris’ Motor: A History of Instruments and Theories Abstract3 The theory of Volta’s pile was initially included into Electrolysis and Chemistry. Only after Oersted’s discovery of the magnetic effect of electric currents, Ampére constructed a dynamical theory of their interactions. In the middle of nineteenth century, Faraday’s electromagnetic induction represented one of the main effects at the basis of Maxwell’s field theory, and, at the same time, the fundamental process for industrial production of electric power. The transmission at distance of this power became feasible only through Galileo Ferraris’ invention of the asyncronous motor and his Maxwellian theory of the transformer. The history of Electricicty is thus considered an emblematic example of a chain of tight connection between theories and instrumental operations, and Volta’s pile stands as the most important among the initial rings of this chain. 1. Introduction Volta’s discovery of a continuous source of electrical power represented the beginning of a process which, at the end of the Nineteenth Century, led to the social and industrial exploitation of electrical energy. At the middle of century, Faraday’s 1931 discovery of a mechanical production of electrical power and the inventions of new theories and of new technical innovations were fundamental aspects of this process. Following the examples of Heaviside, Hertz, Lodge, et alii, electricians would never have denied the merits of Maxwell’s theoretical approach; as mathematical physicists, they were so familiar with it that their only need was to re-read it, in order to adapt its theoretical content to the requirements of their projects, which increased day after day.
    [Show full text]
  • Chronologie De L'horlogerie Électrique
    Dossier réalisé par Jean-Pierre MOURAT, enseignant de sciences physiques, enseignant chargé de mission au musée du Temps, 2015. Chronologie des inventions relatives à l’horlogerie électrique 1790 Bologne Luigi Galvani, médecin à Bologne, constate que les muscles d’une grenouille récemment écorchée se convulsent lorsqu’on les met en contact convenable avec une pince formée par deux métaux, fer et cuivre. 1800 Côme Alexandre Volta, professeur à l’Université de Pavie, construit la première pile électrique. 1820 Copenhague Hans-Christian Œrsted ou Ørsted, constate qu’une aiguille aimantée est déviée par un courant électrique circulant dans un fil conducteur rectiligne. 1820 Paris François Arago observe que le fer doux s’aimante au voisinage d’un fil parcouru par un courant électrique. 1820 Paris André-Marie Ampère établit la théorie des phénomènes électromagnétiques. 1825 Angleterre L’anglais William Sturgeon construit le premier électro-aimant. 1827 Cologne Georg Ohm énonce la loi fondamentale de l’électrotechnique : I=E/R 1830 Vérone Le physicien Giuseppe Zamboni, construit la première horloge électrique dont le pendule est attiré, puis repoussé électro- statiquement, par les deux pôles d’une pile sèche, dérivée de celle de Volta (pile de Zamboni). Cette horloge fût présentée en 1832 à la société des Arts de Genève. 1831 Londres Michael Faraday découvre les phénomènes d’induction et en établit les lois. 1832 USA Le physicien Joseph Henry, en étudiant l’étincelle de rupture d’un circuit électrique bobiné, établit les lois de l’induction du courant électrique sur lui-même, ce que l’on appelle la self-induction. 1832 Paris Hippolyte Pixii construit le premier générateur de courant basé sur l’électromagnétisme.
    [Show full text]
  • Galileo Ferraris: a Life Dedicated to the Electrical Sciences
    Galileo Ferraris: A Life Dedicated to the Electrical Sciences M. Mitolo (°), M. Tartaglia(*) (°) ESI, Foothill Ranch, CA, USA (*) Politecnico di Torino (Italy), Dipartimento Energia This article illustrates the life and work of Prof. Galileo Ferraris (1847-1897), an Italian engineer and scientist who dedicated his life to the study of electricity and its applications in the 19th century. His contributions to different engineering disciplines were remarkable, as were his efforts to develop and disseminate electrical knowledge. In this article, we will briefly discuss his publications and formidable laboratory experiences from 1870 to 1897. All the original works of Galileo Ferraris, his numerous papers and books, are available for free download from the digital repository of the central library of the Politecnico di Torino, the university that he contributed in creating. His life Galileo Ferraris was born on 30 October 1847 in Livorno Piemonte (Kingdom of Sardinia). At the age of 22, he obtained the master’s degree in Civil Engineering, and decided to pursue an academic career. He became an assistant professor under the supervision of Prof. Codazza, within the Technical Physics Department of the Royal Industrial Museum of Turin, Italy. In 1877 he succeeded Prof. Codazza as a full professor of technical physics. Ferraris attended the International Conference in Paris, in 1882, as a delegate of the Italian Government. He was the vice-chair of the International Exposition in Vienna in 1883, and in 1884 he hosted the International Electrical Exhibition in Turin, Italy. During this event, he was also the chair of the award committee, which granted a prize to Gaulard and Gibbs for the invention of the transformer.
    [Show full text]
  • AC Motor INTRODUCTION
    AC motor INTRODUCTION An AC motor is an electric motor that is driven by an alternating current. It consists of two basic parts, an outside stationary stator having coils supplied with alternating current to produce a rotating magnetic field, and an inside rotor attached to the output shaft that is given a torque by the rotating field. There are two types of AC motors, depending on the type of rotor used. The first is the synchronous motor, which rotates exactly at the supply frequency or a submultiple of the supply frequency. The magnetic field on the rotor is either generated by current delivered through slip rings or by a permanent magnet. The second type is the induction motor, which turns slightly slower than the supply frequency. The magnetic field on the rotor of this motor is created by an induced current. History In 1882, Serbian inventor Nikola Tesla identified the rotating magnetic induction field principle[citation needed] and pioneered the use of this rotating and inducting electromagnetic field force to generate torque in rotating machines. He exploited this principle in the design of a poly-phase induction motor in 1883. In 1885, Galileo Ferraris independently researched the concept. In 1888, Ferraris published his research in a paper to the Royal Academy of Sciences in Turin. Introduction of Tesla's motor from 1888 onwards initiated what is sometimes referred to as the Second Industrial Revolution, making possible both the efficient generation and long distance distribution of electrical energy using the alternating current transmission system, also of Tesla's invention (1888).[1] Before widespread use of Tesla's principle of poly-phase induction for rotating machines, all motors operated by continually passing a conductor through a stationary magnetic field (as in homopolar motor).
    [Show full text]
  • Roma, Gen.-Ago. 2005
    RASSEGNA DEGLI ARCHIVI DI STATO nuova serie - anno I - n. 1-2 roma, gen.-ago. 2005 Ministero per i beni e le attività culturali, Dipartimento per i beni archivistici e librari, Direzione generale per gli archivi, Servizio I - Ufficio pubblicazioni, Roma. Direttore generale per gli archivi: Maurizio Fallace, direttore responsabile. Comitato scientifico: il direttore generale per gli archivi, presidente, Paola Carucci, Antonio Dentoni-Litta, Ferruccio Ferruzzi, Patrizia Ferrara, Cosimo Damiano Fonseca, Guido Melis, Claudio Pavone, Leopoldo Puncuh, Isabella Ricci, Antonio Romiti, Isidoro Soffietti, Giuseppe Talamo. Segretaria di redazione: Ludovica de Courten. Redazione: Antonella Mulè De Luigi, Giulia Barrera. La « Rassegna degli Archivi di Stato », rivista quadrimestrale dell’Amministrazione archivistica, è nata nel 1941 come « Notizie degli Archivi di Stato » ed ha assunto l’attuale denominazione nel 1955. I testi degli articoli, i volumi da segnalare e la richiesta di fascicoli in omaggio o scambio vanno indirizzati a « Rassegna degli Archivi di Stato », Ministero per i beni e le attività culturali, Dipartimento per i beni archivistici e librari, Direzione gene- rale per gli archivi, Servizio I - Ufficio pubblicazioni, via Gaeta 8/a 00185 Roma, tel. 06492251. Sito Internet: http://www.archivi.beniculturali.it/servizioI; e-mail: rasse- [email protected] I manoscritti, anche se non pubblicati, non si restituiscono. È vietata la riproduzione, totale o parziale, degli articoli pubblicati, senza citarne la fonte. Gli articoli firmati ri- specchiano le opinioni degli autori: la pubblicazione non implica adesione, da parte della rivista, alle tesi sostenute. VENDITE E ABBONAMENTI: Istituto Poligrafico e Zecca dello Stato s.p.a., Funzione arte/editoria, Libreria dello Stato, piazza G.
    [Show full text]
  • Electromagnetic Induction: Physics, Historical Breakthroughs
    Electromagnetic induction: physics, historical breakthroughs, epistemological issues and textbooks Giuseppe Giuliani Formerly, Dipartimento di Fisica, Universit`adegli Studi, via Bassi 6, 27100 Pavia, Italy. [email protected] Abstract. The discovery of Electromagnetism by Ørsted (1820) initiated an “extraordinary decennium” ended by the discovery of electromagnetic induction by Faraday (1831). During this decennium, in several experiments, the electromagnetic induction was there, but it was not seen or recognized. In 1873, James Clerk Maxwell, within a Lagrangian description of electric currents, wrote down a ‘general law of electromagnetic induction’ given by, in modern form and with standard symbols: ∂A~ = [E~ +(~v B~ )] dl~ ; E~ = ϕ E Il × · −∇ − ∂t In Maxwell’s derivation, the velocity appearing in this equation, is the velocity of the line element dl~ . A modern reformulation of Maxwell’s general law, starts with the definition of the induced emf as the = [E~ +(~vc B~ )] dl~ , where ~vc is the velocity E l × · of the charge. It is shown that, this apparentlyH minor difference, is fundamental. The general law is a local law: it correlates what happens in the line at the instant t to the values of quantities at the points of the line at the same instant t. For rigid circuits, it is Lorentz invariant. If expressed in terms of the magnetic field, it allows – in the approximation of low velocities – the derivation of the “flux rule”, for filiform circuits. The “flux rule” is a calculation tool and not a physical law because it not always yields the correct prediction, it does not say where the induced emf is localized, it requires ad hoc choices of the integration paths and – last but not least – because, if physically interpreted, it implies physical interactions with speeds higher than that of light.
    [Show full text]
  • The Invention of the Electric Dynamo
    The Invention of the Electromotive Engine B. J. G. van der Kooij This case study is part of the research work being completed in preparation for a doctorate-dissertation to be submitted to the University of Technology, Delft, The Netherlands (www.tudelft.nl). It is part of a series of case studies about “Innovation” under the title “The Invention Series.” About the text—This is a scholarly case study describing the historic developments that resulted in electromotive engines. It is based on a large number of historic and contemporary sources. As we did not conduct any research into primary sources, we made use of the efforts of numerous others by citing them quite extensively to preserve the original character of their contributions. Where possible we identified the individual authors of the citations. When an author is not identifiable, we identified the source of the text. Facts that are considered to be of a general character in the public domain are not cited. About the pictures—Many of the pictures used in this study were found on websites accessed through the Internet. Where possible they were traced to their origins, and the source is indicated. As most photos are past the age where copyright would apply, we feel that we make fair use of the pictures to illustrate the scholarly case, and this use is not an infringement of copyright. Copyright © 2015 B. J. G. van der Kooij Cover art is line drawing of Bush’ electric dynamo (US Patent № 189.997) and Dobrowolsky’s electric motor (US patent № 469.515). (courtesy USPTO) Version 1.1 (March 2015) All rights reserved.
    [Show full text]
  • Department of Commerce 2017-18
    GOVT. COLLEGE OF TEACHER EDUCATION, THYCAUD, THIRUVANANTHAPURAM INNOVATIVE PRACTICES BY DEPARTMENT OF COMMERCE GRAPHIC ORGANIZER BASED INSTRUCTIONAL PRACTICES 2017-18 TITLE OF THE PRACTICE: GRAPHIC ORGANIZER BASED INSTRUCTIONAL PRACTICES THE CONTEXT THAT REQUIRED INITIATION OF THE PRACTICE In this technological era, teachers will have to learn and practice new pedagogies capable of maintaining high standards in the face of India’s socio cultural diversity and economic disparity. If we expect students to learn appropriate competencies and skills, we must structure the learning environment so that these can be addressed and practiced. For this, appropriate pedagogic practices and episodes of teaching and learning need to be evolved besides keeping track of child’s interests and needs. Graphic organizers are shape-based diagrams that organize students’ thoughts. Graphic organizers help students sort, differentiate, show relationships, make meaning, and manage data quickly and easily before, during, and after reading and discussion. This method is can be adopted as an effective method of instruction. Our students use graphic organizer based instructional strategy during their teaching practice course. The prospective teachers know the effectiveness of this approach as they learnt through this method during their course of study. The Graphic Organizers, an instructional processing tool for: Modeling Learning experiences Assessment Graphic Organizer: An Instructional Special needs Processing Tool Variations Figure 2.6 Graphic Organizer: An Instructional Processing Tool Modeling: It is critical to model Graphic Organizer when you present it in to the class. Learning Experiences: Graphic Organizers can be effective used or individual and small group instruction through which they provide a structure for the students.
    [Show full text]
  • Winding Type Influence on Efficiency of an Induction Motor
    Miralem HADŽISELIMOVIĆ1,2, Tine MARČIČ3, Bojan ŠTUMBERGER1,2, Ivan ZAGRADIŠNIK2,1 University of Maribor, Faculty of Energy Technology (1) University of Maribor, Faculty of Electrical Engineering and Computer Science (2) TECES, Research and Development Centre for Electric Machines (3) Winding type influence on efficiency of an induction motor Abstract. The article presents an analysis of the winding type influence on the efficiency of an induction motor. The aim of this work is to choose such a type of stator winding that the induction motor will have the best efficiency by employing minimum winding (copper) mass. Three types of stator windings were considered in the analysis: concentric single layer winding, concentric double layer winding and fractional concentric winding. The complete procedure for the calculation of winding data is performed. The analytical calculations of electromagnetic characteristics were performed with the software package emLook in order to select the best suited winding type and consequently ensuring the best efficiency and performance of the induction motor in question. The presented results are applicable for the industry of electric machines. Streszczenie. Artykuł przedstawia analizę wpływu typu uzwojenia ja sprawność silnika indukcyjnego. Celem pracy jest wybór takiego typu uzwojenia stojana, które zapewni maksymalną sprawność przy minimalnej masie uzwojenia. Trzy typy uzwojeń stojana zostały rozpatrzone: uzwojenie koncentryczne jednowarstwowe, dwuwarstwowe oraz uzwojenie koncentryczne ułamkowe. Przedstawiono procedurę obliczania danych uzwojenia. Do wyznaczenia charakterystyki elektromagnetycznej wykorzystano obliczenia analityczne z pakietem emLook. Wyselekcjonowano najlepszy typ uzwojenia, zapewniający najlepszą sprawność działania rozważanego silnika indukcyjnego. Przedstawione wyniki zostały implementowane w rozwiązaniach przemysłowych. (Wpływ typu uzwojenia na sprawność silnika indukcyjnego) Keywords: induction motor, stator winding, characteristics, efficiency.
    [Show full text]