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By Crowell B.

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8 The Story of the “Maxwell” Equations . . . . 9 Maxwell . . . . . . . . . . . . . . . . . . 10 Heaviside . . . . . . . . . . . . . . . . . 11 Zeeman, Hale, Gouy, and Larmor . . . . . . 13 Our story covers two and one half millennia. It starts with Thales of Miletus who wrote in −600 about the mineral magnetite. It ends with Gouy and Larmor who proposed at the beginning of the 20th century the concept of self-excited dynamo to explain the existence of magnetic fields on the Sun.

194 × 106 ρ volts/meter .

31 33 34 34 35 36 36 37 37 37 41 44 Our objective in Chapters 2 to 5 is to set the stage for our study of magneto-fluid-dynamic phenomena. Here we think about electric fields in simple cases: for the moment there are no magnetic fields, and no moving conductors. We present an Example and a Case Study: the first concerns a proton beam, and the second the electrostatic potential at the surface of the Sun. In this chapter we study the electric fields that result from accumulations of electric charge.

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