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the chapter) simplify the problem and make its approximate numerical solution possible in a few simple steps In reality, ux leakage, fringing, and uneven distribution of ux across the structure would require the solution of three-dimensional equations using nite-element methods These methods are not discussed in this book, but are necessary for practical engineering designs The usefulness of these approximate methods is that you can, for example, quickly calculate the approximate magnitude of the current required to generate a given magnetic ux or ux density You shall soon see how these calculations can be used to determine electromagnetic energy and magnetic forces in practical structures The methodology described in this example is summarized in the following methodology box

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For a fraction to be zero, the numerator must equal zero. ^ Thus, q2 0, and q 0. At equilibrium, the a allele should be entirely removed from the population. If the aa homozygotes are being removed, and if there is no mutation to return a alleles to the population, then eventually the a allele disappears from the population.

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Magnetic Structures and Equivalent Magnetic Circuits Direct Problem: Given The structure geometry and the coil parameters (number of turns, current) Calculate The magnetic ux in the structure 1 Compute the mmf 2 Determine the length and cross section of the magnetic path for each continuous leg or section of the path 3 Calculate the equivalent reluctance of the leg 4 Generate the equivalent magnetic circuit diagram and calculate the total equivalent reluctance 5 Calculate the ux, ux density, and magnetic eld intensity, as needed Inverse Problem: Given The desired ux or ux density and structure geometry Calculate The necessary coil current and number of turns 1 Calculate the total equivalent reluctance of the structure from the desired ux 2 Generate the equivalent magnetic circuit diagram 3 Determine the mmf required to establish the required ux 4 Choose the coil current and number of turns required to establish the desired mmf

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Consider the analysis of the same simple magnetic structure when an air gap is present Air gaps are very common in magnetic structures; in rotating machines, for example, air gaps are necessary to allow for free rotation of the inner core of the machine The magnetic circuit of Figure 1617(a) differs from

q(1 q) q)(1 q) q q)

r 0

l5 (a)

(20.17)

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the circuit analyzed in Example 162 simply because of the presence of an air gap; the effect of the gap is to break the continuity of the high-permeability path for the ux, adding a high-reluctance component to the equivalent circuit The situation is analogous to adding a very large series resistance to a series electrical circuit It should be evident from Figure 1617(a) that the basic concept of reluctance still applies, although now two different permeabilities must be taken into account The equivalent circuit for the structure of Figure 1617(a) may be drawn as shown in Figure 1617(b), where Rn is the reluctance of path ln , for n = 1, 2, , 5, and Rg is the reluctance of the air gap The reluctances can be expressed as follows, if we assume that the magnetic structure has a uniform cross-sectional area, A: R1 = l1 r 0 A R2 = l2 r 0 A R3 = l3 r 0 A

One shortcoming of this selection model is that it is not immediately apparent how many generations will be required to remove the a allele.The de ciency can be compensated for by using a computer simulation or by introducing a calculus differential into the model. Either method would produce the frequency-time graph of gure 20.11. This gure clearly shows that the a allele is removed more quickly when selection is stronger (when s is larger) and that the curves appear to be asymptotic the a allele is not immediately eliminated and would not be entirely removed until an in nitely large number of generations had passed. There is a reason for the asymptotic behavior of the graph: As the a allele becomes rarer and rarer, it tends to be found in heterozygotes (table 20.3). Since selection can remove only aa homozygotes, an a allele hidden in an Aa heterozygote will not be selected against.When q 0.5, there are two heterozygotes for every aa homozygote. When

(1631)

Figure 1617 (a) Magnetic circuit with air gap; (b) Equivalent representation of magnetic circuit with an air gap

To solve this equation, q is multiplied by (1 q)/(1 q) so that both parts of the expression are over a common denominator: q q q(1 q) 1 q

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