Instructors_Guide_Ch26 - 26 The Electric Field Recommended...

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26 The Electric Field Recommended class days: 3 minimum, 4 preferred Background Information Chapter 25 introduced the field model, and Chapter 26 will now develop the quantitative analysis of electric fields and of the motion of charged particles in the field. The goal is not for students to become experts at calculating fields, although they should be able to do calculations for simple charge distributions, but for them to recognize standard electric fields such as those of dipoles and of lines and planes of charge. Field calculations are based directly upon the principle of superposition. Superposition is a straightforward and readily understood procedure, whereas, as will be discussed more in Chapter 27, research has found that only a very small fraction of students are able to understand Gauss’s law. Further, superposition helps students with their conceptual difficulties by explicitly linking field calculations to Coulomb’s law. With one exception, all the standard fields can easily be found using superposition. The exception is the field of a sphere of charge, for which the integrations—although doable—are too complex for an introductory class. However, it is quite believable, without a rigorous proof, that the exterior field of a sphere of charge is the same as that of a point charge. We routinely make this same assertion, without proof, for Newton’s law of gravity. At this point in the course, students have been doing calculus long enough that nearly all can carry out an integration. However, students are still very inexperienced at using calculus to analyze a problem. Their difficulty with this chapter—and it is a major difficulty for most—is not with doing integrals but with knowing what to integrate . Students are completely unfamiliar with the procedure of dividing a charge distribution into small pieces, writing the superposition of fields as a sum, and then converting the sum to an integral by using the charge density. The emphasis in this chapter needs to be on the analysis and the procedures that lead to an integration. Students also have a hard time visualizing fields in three dimensions. The fields of interest in this course usually have an axis of symmetry, so you need to encourage students to imagine the two-dimensional drawings of the textbook, or that you draw on the board, as being rotated about that axis. Several software packages can provide useful classroom demonstrations giving three- dimensional renderings of fields. It is important to explain clearly what the standard two-dimensional drawings are meant to represent. For example, a parallel-plate capacitor is usually drawn as shown in the figure. Many students don’t recognize, unless you point it out, that the drawing shown here represents two planes of charge extending above and below the plane of the drawing. These students interpret the drawing literally as a two-dimensional field of two short line segments of charge. The parallel-plate capacitor encounters another common student misconception: that one layer
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This note was uploaded on 01/14/2011 for the course CD 254 taught by Professor Kant during the Spring '10 term at Central Oregon Community College.

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Instructors_Guide_Ch26 - 26 The Electric Field Recommended...

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