File:Faraday emf experiment.svg

Summary
Faraday's experiment to try to induce a current from a magnetic field, with a battery on the left, an iron ring in the centre, and a galvanometer on the right. This diagram is based on one found in page 263 of Physics: Principles with Applications, fifth edition, author Douglas C. Giancoli, illustrators Patrice Van Acker and Tamara Newnam Cavallo. The explanation in the book reads as follows, with the left coil being X and the right coil Y:
“In his attempt to produce an electric current from a magnetic field, Faraday used an apparatus like that shown in Fig. 21–1. A coil of wire, X, was connected to a battery. The current that flowed through X produced a magnetic field that was intensified by the iron core. Faraday hoped that by using a strong enough battery, a steady current in X would produce a great enough magnetic field to produce a current in a second coil Y. This second circuit, Y, contained a galvanometer to detect any current but contained no battery. He met no success with steady currents. But the long-sought effect was finally observed when Faraday saw the galvanometer in circuit Y deflect strongly at the moment he closed the switch in circuit X. And the galvanometer deflected strongly in the opposite direction when he opened the switch.[...] Faraday concluded that although a steady magnetic field produces no current, a [changing one can]. Such a current is called an induced current.”
For more information see <a href="https://en.wikipedia.org/wiki/Faraday%27s_law_of_induction" class="extiw" title="w:Faraday's law of induction">Faraday's law of induction</a> and <a href="https://en.wikipedia.org/wiki/Electromagnetic_induction" class="extiw" title="w:Electromagnetic induction">electromagnetic induction</a>.
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current | 19:30, 6 January 2017 | ![]() | 1,035 × 365 (41 KB) | 127.0.0.1 (talk) | Faraday's experiment to try to induce a current from a magnetic field, with a battery on the left, an iron ring in the centre, and a galvanometer on the right. This diagram is based on one found in page 263 of <i>Physics: Principles with Applications</i>, fifth edition, author Douglas C. Giancoli, illustrators Patrice Van Acker and Tamara Newnam Cavallo. The explanation in the book reads as follows, with the left coil being <i>X</i> and the right coil <i>Y</i>: <blockquote class="templatequote"><div class="Bug6200"><span class="language">“In his attempt to produce an electric current from a magnetic field, Faraday used an apparatus like that shown in Fig. 21–1. A coil of wire, <i>X</i>, was connected to a battery. The current that flowed through <i>X</i> produced a magnetic field that was intensified by the iron core. Faraday hoped that by using a strong enough battery, a steady current in <i>X</i> would produce a great enough magnetic field to produce a current in a second coil <i>Y</i>. This second circuit, <i>Y</i>, contained a galvanometer to detect any current but contained no battery. He met no success with steady currents. But the long-sought effect was finally observed when Faraday saw the galvanometer in circuit <i>Y</i> deflect strongly at the moment he closed the switch in circuit <i>X</i>. And the galvanometer deflected strongly in the opposite direction when he opened the switch.[...] Faraday concluded that although a steady magnetic field produces no current, a [changing one can]. Such a current is called an induced current.”</span></div></blockquote> For more information see <a href="https://en.wikipedia.org/wiki/Faraday%27s_law_of_induction" class="extiw" title="w:Faraday's law of induction">Faraday's law of induction</a> and <a href="https://en.wikipedia.org/wiki/Electromagnetic_induction" class="extiw" title="w:Electromagnetic induction">electromagnetic induction</a>. |
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