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You can probably see intuitively that the rst of these assumptions might not hold true near the ends of the coil, but that it might be more reasonable if the coil is tightly wound The second assumption is equivalent to stating that the relative permeability of the core is in nitely higher than that of air (presuming that this is the medium surrounding the core): if this were the case, the ux would indeed be con ned within the core It is worthwhile to note that we make a similar assumption when we treat wires in electric circuits as perfect conductors: the conductivity of copper is substantially greater than that of free space, by a factor of approximately 1015 In the case of magnetic materials, however, even for the best alloys, we have a relative permeability only on the order of 103 to 104 Thus, an approximation that is quite appropriate for electric circuits is not nearly as good in the case of magnetic circuits Some of the ux in a structure such as those of Figures 1612 and 1613 would thus not be con ned within the core (this is usually referred to as leakage ux) Finally, the assumption that the ux is uniform across the core cannot hold for a nite-permeability medium, but it is very helpful in giving an approximate mean behavior of the magnetic circuit The magnetic circuit analogy is therefore far from being exact However, short of employing the tools of electromagnetic eld theory and of vector calculus, or advanced numerical simulation software, it is the most convenient tool at the engineer s disposal for the analysis of magnetic structures In the remainder of this chapter, the approximate analysis based on the electric circuit analogy will be used to obtain approximate solutions to problems involving a variety of useful magnetic circuits, many of which you are already familiar with Among these will be the loudspeaker, solenoids, automotive fuel injectors, sensors for the measurement of linear and angular velocity and position, and other interesting applications.

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16

Find: ; B; H Schematics, Diagrams, Circuits, and Given Data: r = 1,000; N = 500 turns; i = 01 A The magnetic circuit geometry is de ned in Figures 1614 and 1615 Assumptions: All magnetic ux is linked by the coil; the ux is con ned to the magnetic core; the ux density is uniform Analysis:

Calculation of magnetomotive force From equation 1628, we calculate the magnetomotive force: F = mmf = N i = (500 turns)(01 A) = 50 A t

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Findings ASP projects range from 2 to 14 hours per function point Median and mean are both 6 hours per function point Oracle projects are spread fairly evenly from 1 to 33 hours per function point The median is 9 and the mean is 10 hours per function point SQL ranges from 3 to 12 hours per function point, with an average of 5 hours per function point and a median of 4 Again, C projects appear to have better PDR rates than C++ projects, but the sample of C projects is small, so this conclusion is risky Treating them as a single combined group, nearly all are between 3 and 15 hours per function point The median is 10 hours per function point, and the mean is 14 hours per function point COBOL ranges widely, from 3 to over 30 hours per function point Almost half are below 6 hours per function point The rest are scattered from 9 to 35 hours per function point The median is 10 hours per function point, and the mean is 13 hours per function point Visual Basic projects range from 1 to 24 hours per function point, but nearly all are below 12 hours per function point The mean and median are both 7 hours per function point Nearly all Java projects are between 2 and 12 hours per function point The median is 8 hours per function point, and the mean is 9 hours per function point

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Calculation of mean path Next, we estimate the mean path of the magnetic ux On the basis of the assumptions, we can calculate a mean path that runs through the geometric center of the magnetic structure, as shown in Figure 1615 The path length is: lc = 4 009 m = 036 m

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