PHYC10007 Lecture Notes - Lecture 29: Galvanometer, Electric Field

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Induced currents fa(cid:396)ada(cid:455)(cid:859)s law: an electric field can produce a magnetic field, a changing magnetic field induces an electric current, cu(cid:396)(cid:396)e(cid:374)t i(cid:374)du(cid:272)ed i(cid:374) a (cid:272)losed loop of wi(cid:396)e that (cid:858)su(cid:396)(cid:396)ou(cid:374)ds(cid:859) the (cid:272)ha(cid:374)gi(cid:374)g magnetic field. I(cid:374) fa(cid:396)ada(cid:455)(cid:859)s o(cid:396)igi(cid:374)al e(cid:454)pe(cid:396)i(cid:373)e(cid:374)t, the (cid:374)o(cid:396)th pole of a pe(cid:396)(cid:373)a(cid:374)e(cid:374)t (cid:271)a(cid:396) (cid:373)ag(cid:374)et (a magnetized piece of iron) is moved through a conductor loop: as a result, the galvanometer displays a current peak. Induced electric field is larger if magnetic field is more intense: magnetic flux, depends on the angle between wire loop and magnetic field. Imagine a fan blowing air through a loop, more air through loop when loop is perpendicular to air flow. If two planes are parallel no induction. If there are n turns of wire enclosing the magnetic flux, the equation becomes: generators, pulling the loop of wire in a magnetic field to.

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