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The Dawn of Electro-Magnetism

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A Student's Guide Through the Great Physics Texts

Part of the book series: Undergraduate Lecture Notes in Physics ((ULNP))

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Abstract

So far, we have explored magnetism and electricity as separate phenomena. This is the legacy of William Gilbert, who recognized that while magnets and electrically charged bodies can exert forces, they do not exert forces on each other: electrically charged bodies attract or repel other electrically charged bodies; magnetic bodies attract or repel other magnetic bodies. This simple and pleasant demarcation was upset by the work of Hans Christian Oersted (1777–1851), who was born in Rudkøbing, Denmark.

Today, Oersted is best known for his discovery of the connection between electrical currents and magnetism. This work, described in the reading selection in this chapter, inspired later experiments on electromagnetic phenomena by both Faraday and Ampère and culminated in Maxwell’s electromagnetic theory of light. Originally written in Latin, Oersted’s Experiments on the Effect of a Current of Electricity on the Magnetic Needle was translated into English and published in 1820 in Thomson’s Annals of Philosophy.

It is sufficiently evident from the preceding facts that the electric conflict is not confined to the conductor, but dispersed pretty widely in the circumjacent space.

—Hans Christian Oersted

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Notes

  1. 1.

    See especially Chaps. 1, 4 and 6 of the present volume.

  2. 2.

    See Oersted, H. C., Selected Scientific Works of Hans Christian Oersted, Princeton University Press, 1998.

  3. 3.

    See Chaps. 8, 25 and 31 of the present volume.

  4. 4.

    For automated data acquisition, I have used the magnetic field sensor (Model MG-BTA) and a Lab Pro interface, both manufactured by Vernier Software & Technology, Beaverton, OR.

  5. 5.

    See Ampère’s theory of magnetism in Chap. 8 of the present volume.

  6. 6.

    See Chap. 6 of the present volume.

  7. 7.

    The concept of the magnetic field will be developed in more detail by Michael Faraday in Chaps. 28 and 29 of the present volume. See also the discussion of vector fields in Appendix A.

  8. 8.

    The magnetic field in the vicinity of arbitrarily shaped current-carrying wires can be computed using the Biot-Savart law; see Ex. 8.4 in the following chapter.

  9. 9.

    A system of units for measuring magnetic field strength was first developed in the 1830’s by the mathematician Carl Friedrich Gauss. Today, magnetic field strength is typically measured in either tesla (mks) or gauss (cgs); one gauss equals \(100 \times 10^{-6}\) T.

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Correspondence to Kerry Kuehn .

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Kuehn, K. (2016). The Dawn of Electro-Magnetism. In: A Student's Guide Through the Great Physics Texts. Undergraduate Lecture Notes in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-21816-8_7

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