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The notion that the phenomena of electricity and magnetism are interconnected was rst proposed in the early 1800s by H C Oersted, a Danish physicist Oersted showed that an electric current produces magnetic effects (more speci cally, a magnetic eld) Soon after, the French scientist Andr Marie Amp` re expressed e e this relationship by means of a precise formulation, known as Amp` re s law A few e years later, the English scientist Faraday illustrated how the converse of Amp` re s e law also holds true, that is, that a magnetic eld can generate an electric eld; in short, Faraday s law states that a changing magnetic eld gives rise to a voltage We shall undertake a more careful examination of both Amp` re s and Faraday s e laws in the course of this chapter As will be explained in the next few sections, the magnetic eld forms a necessary connection between electrical and mechanical energy Amp` re s and e Faraday s laws will formally illustrate the relationship between electric and magnetic elds, but it should already be evident from your own individual experience that the magnetic eld can also convert magnetic energy to mechanical energy (for example, by lifting a piece of iron with a magnet) In effect, the devices we commonly refer to as electromechanical should more properly be referred to as electromagnetomechanical, since they almost invariably operate through a conversion from electrical to mechanical energy (or vice versa) by means of a magnetic eld s 16 through 18 are concerned with the use of electricity and magnetic materials for the purpose of converting electrical energy to mechanical, and back The Magnetic Field and Faraday s Law The quantities used to quantify the strength of a magnetic eld are the magnetic ux, , in units of webers (Wb); and the magnetic ux density, B, in units of webers per square meter (Wb/m2 ), or teslas (T) The latter quantity, as well as the associated magnetic eld intensity, H (in units of amperes per meter, or A/m) are vectors1 Thus, the density of the magnetic ux and its intensity are in general described in vector form, in terms of the components present in each spatial direction (eg, on the x, y, and z axes) In discussing magnetic ux density and eld intensity in this chapter and the next, we shall almost always assume that the eld is a scalar eld, that is, that it lies in a single spatial direction This will simplify many explanations It is customary to represent the magnetic eld by means of the familiar lines of force (a concept also due to Faraday); we visualize the strength of a magnetic eld by observing the density of these lines in space You probably know from a previous course in physics that such lines are closed in a magnetic eld, that is, that they form continuous loops exiting at a magnetic north pole (by de nition).

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will use the boldface symbols B and H to denote the vector forms of B and H ; the standard typeface will represent the scalar ux density or eld intensity in a given direction

where the symbol denotes the (vector) cross product If the charge is moving at a velocity u in a direction that makes an angle with the magnetic eld, then the magnitude of the force is given by f = quB sin (162)

(You ll notice that the View Report button is not enabled; it won t be until the test has been run at least once do you understand how the code works to make this happen ) You should see the Calculator appear and the Addition test will take a few seconds to run..

(161)

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and entering at a magnetic south pole The relative strengths of the magnetic elds generated by two magnets could be depicted as shown in Figure 161 Magnetic elds are generated by electric charge in motion, and their effect is measured by the force they exert on a moving charge As you may recall from previous physics courses, the vector force f exerted on a charge of q moving at velocity u in the presence of a magnetic eld with ux density B is given by the equation

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