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During the 1820s Faraday sought to discover how to make electricity from magnetism. He achieved success with the device pictured above on 29 August 1831. When he passed an electric current through one coil he induced an electric current in the other coil, which flowed for a very brief period of time. When Michael Faraday made his discovery of electromagnetic induction in 1831, he hypothesized that a changing magnetic field is necessary to induce a current in a nearby circuit. To test his hypothesis he made a coil by wrapping a paper cylinder with wire. He connected the coil to a galvanometer, and then moved a magnet back and forth inside the cylinder. During the 1820s Faraday sought to discover how to make electricity from magnetism. He achieved success with the device pictured above on 29 August 1831. It's made from everyday materials such as wire made for bonnets, although the iron ring seems to have been specially made. Faraday’s magnetic induction experiment. Ampere's law applied to an infinitely-long wire predicts a magnetic field of strength B=m0I/(2pr) a radial distance r from the wire. The field B is tangential to a circle of radius r centered on the wire. We therefore have (B/I)=(m0/2p)(1/r). B/I is proportional to 1/r, and when plotted versus 1/r will yield a straight line with slope (m0/2p). Consider the magnetic field around an infinitely long wire due to a current I flowing through the wire. But B has the same value a distance a away from the rod, hence For the simple example, only one current linking the closed path C, therefore N = 1 (e Loo mat rat ma p. mf) kin erial ed teri Wh g isand by al ile is at iron so is wea use the but me me 2. Biotcan d infi ther ba asu Savart dev in nit e sic re Law elo ma e are cur of It is p gne wir othe re it's possible an tic e r nt ma to ana circ aga elem co gne determin lyti uits in ents nfi tic e the cal to we such gu 'str magneti sol det can as rat eng c field uti er app coba ion th'. generate on mi ly lt s Ma d by a for ne Am and usi gne current the the per nick ng tisa element axi flux e's el, thi tio using al den La as s n the Biotfiel siti w well la can Savart d, es as as w. be Law. it's in foll num Co inh not the ow erou nsi ere Eqn pos s 8.2 s: s var der nt sibl iou alloy an in e Fig s s 8.1 infi the to at the general electromagnetic principles which are widely employed in engineering. This is a very short introduction to a complex subject. Yo circ like If nit ma do and Forces uit The silic the ely teri this at the case of the pat tor on relcoilgun it will be beneficial to briefly examine the fundamentals of electromagnetic fields and lonforces. Whenever there is char al, for hs. us steel uct g suc the Mm . has an wir h fiel fas a Each ce e is d me mat ca caraeach system has different unit in there are three systems of units in popular use, namely the Sommerfield, Kennely and Gaussian systems. Since in asu an erial n ryi per gen red rad has be ng ma era in aius det a ne l. am of parti er curr nt In per and cular mi re ma ord ea prop ne nt gne er tur cro erty d ti. or to ns sswhic the We it fin or hsec n ca can d jus tio mak we n be the tgen nal es it ca us fiel Magnetisation n System of Units -1 weber Quantity tesla Am Unit M m H B I- (T) (W) Maxwell's Equations M a x w el l' s e q u at io n s c o n Faraday's Law of Induction The line integral of the electric field around a closed loop is equal to the negative of the rate of change of the magnetic flux through the area enclosed by the loop. This line integral is equal to the generated voltage or emf in the loop, so Faraday's law is the basis for electric generators. It also forms the basis for inductors and transformers. Application to voltage generation in a coil Gauss' law, electricity Gauss' law, magnetism Faraday's law Ampere's law Maxwell's Equations Index Maxwell's equations concepts HyperPhysics***** Electricity and Magnetism R NaveGo Back Ampere's Law In the case of static electric field, the line integral of the magnetic field around a closed loop is proportional to the electric current flowing through the loop. This is useful for the calculation of magnetic field for simple geometries. Gauss' law, electricity Gauss' law, magnetism Faraday's law Ampere's law Apply to charge conservation Maxwell's Equations Figure 6: Current i charging a capacitor as an illustration of Maxwell’s displacement current (see text).