https://notes.ashstewart.uk/index.php?action=history&feed=atom&title=Year_1_Sem_2%2FLC_Electromagnetism_I%2FLecture_16Year 1 Sem 2/LC Electromagnetism I/Lecture 16 - Revision history2026-10-13T15:16:32ZRevision history for this page on the wikiMediaWiki 1.46.0https://notes.ashstewart.uk/index.php?title=Year_1_Sem_2/LC_Electromagnetism_I/Lecture_16&diff=374&oldid=prevAsh: Import converted Year 1 Semester 2 lecture notes from 443937a7d37850a3c57dfa863f35e80d07f2ccbc2026-09-11T14:49:09Z<p>Import converted Year 1 Semester 2 lecture notes from 443937a7d37850a3c57dfa863f35e80d07f2ccbc</p>
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<b>Lecture 16: Electromagnetism I: Induction</b><br><br />
Thu 12 Mar 2026 11:00<br />
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[[Year 1 Sem 2/LC Electromagnetism I/Lecture 15|← Previous lecture]] · [[Year 1 Sem 2/LC Electromagnetism I|Module]]<br />
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== Ampere’s Law Continued ==<br />
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== Magnetic Inductance ==<br />
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Faraday suggested that, if currents induce magnetic fields, that the opposite might be possible. Could a magnetic field be used to induce a current? He found that whenever field lines move or change, an electric field is induced, which charges in the field respond to.<br />
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== Motion of a Conductor in Magnetic Field ==<br />
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== Induced E-Fields ==<br />
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== Faraday’s Law ==<br />
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[[Year 1 Sem 2/LC Electromagnetism I/Lecture 15|← Previous lecture]] · [[Year 1 Sem 2/LC Electromagnetism I|Module]]</div>Ash