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Faraday’s law of electromagnetic induction

Equation (1.70) is Faraday s law of electromagnetic induction it shows that a time-dependent magnetic flux density, B, gives rise to an electric field, E, in a... [Pg.33]

M. Guillen, Five Equations That Changed the World The Power and Poetry of Mathematics, Hyperion, New York, 1995. The five equations Guillen includes are Newton s law of gravity, Bernoulli s law of hydrodynamic pressure, Faraday s law of electromagnetic induction, Clausius s second law of thermodynamics, and Einstein s theory of special relativity. [Pg.529]

Eddy currents appear as a consequence of Faraday s law of electromagnetic induction. Consider a cylindrical sample of material. Fig. 4.64. As the current flows in the coil, an ac magnetic field H is applied to the... [Pg.179]

FIGURE 11.16 Faraday s law of electromagnetic induction, leading to third... [Pg.225]

After the appearance of the Volta pile and other improved versions of batteries, extended experiments with the new phenomenon of a continuous electrical current became possible and soon different properties of this current could be established in 1820 Ampbre s law of interaction between electrical currents in 1827 Ohm s law of proportionality between voltage and current in 1831 Joule s law of the thermal effect of electrical current in 1831 Faraday s law of electromagnetic induction, and many others. These achievements led to the development of the theory of electrodynamics and practice of electrical engineering and, as a result, to the appearance of a revolutionary new power source the electromagnetic generator invented in 1866 by Werner von Siemens (1816-1872), which soon surpassed their predecessors both in electrical and economic parameters. [Pg.9]

Faraday s laws of electromagnetic Induction (1) An e.m.f. is induced in acon-ductor when the magnetic field surrounding it changes. (2) The magnitude of the e.m.f. is proportional to the rate of change of the field. (3) The sense of the Induced e.m.f. depends on the direction of the rate of change of the field. [Pg.314]

It is a relatively simple matter to describe the voltage drop across a simple self-inductance such as the coil of Fig. 2.30. For a steady-state current I, in the coils, the voltage drop is simply IR, as dictated by Ohm s Law, where R is the coil resistance. On the other hand, if the current i (t) is time varying, then it follows quite simply from a combination of Faraday s Law of electromagnetic induction and equations (see, for example, Eqs. (2.29) and (2.31)) for magnetic flux and flux density that the (time-varying) voltage drop v across a self-inductance is... [Pg.167]

The induced voltage in the receiver coil, S t), is proportional to the rate of change in magnetic flux ( ) following Faraday s law of electromagnetic induction, and it can be expressed as... [Pg.220]


See other pages where Faraday’s law of electromagnetic induction is mentioned: [Pg.1470]    [Pg.64]    [Pg.231]    [Pg.60]    [Pg.124]    [Pg.60]    [Pg.587]    [Pg.201]    [Pg.12]    [Pg.34]    [Pg.935]    [Pg.338]    [Pg.228]    [Pg.1470]    [Pg.940]    [Pg.767]    [Pg.242]    [Pg.225]    [Pg.510]    [Pg.722]    [Pg.1169]   
See also in sourсe #XX -- [ Pg.124 ]

See also in sourсe #XX -- [ Pg.225 ]




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