Faraday’s Law, Alternating Current, and Maxwell’s Equations

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dc.AffiliationOctober University for modern sciences and Arts (MSA)
dc.contributor.authorA Radi, Hafez
dc.contributor.authorO Rasmussen, John
dc.date.accessioned2020-02-10T12:24:11Z
dc.date.available2020-02-10T12:24:11Z
dc.date.issued2012
dc.descriptionMSA Google Scholaren_US
dc.description.abstractExperimentally, M. Faraday and J. Henry show that a changing magnetic field can establish a current in a circuit that has no battery. When we move a magnet toward a stationary loop that is connected to a galvanometer, the galvanometer’s needle deflects in one direction. When the magnet stops, no deflection is observed. Now, when we move the magnet away from the loop, the needle deflects in the opposite direction.en_US
dc.identifier.doihttps://doi.org/10.1007/978-3-642-23026-4_27
dc.identifier.isbnOnline ISBN 978-3-642-23026-4
dc.identifier.issnPrint ISBN 978-3-642-23025-7
dc.identifier.otherhttps://doi.org/10.1007/978-3-642-23026-4_27
dc.identifier.urihttps://t.ly/w5gWM
dc.language.isoenen_US
dc.publisherSpringeren_US
dc.subjectMagnetic Fielden_US
dc.subjectMagnetic Fluxen_US
dc.subjectUniform Magnetic Fielden_US
dc.subjectInternal Magnetic Fielden_US
dc.subjectSecondary Coilen_US
dc.titleFaraday’s Law, Alternating Current, and Maxwell’s Equationsen_US
dc.typeBook chapteren_US

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