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In summary, when an N -turn coil carrying a current i is wound around a magnetic core such as the one indicated in Figure 1612, the mmf, F, generated by the coil produces a ux, , that is mostly concentrated within the core and is assumed to be uniform across the cross section Within this simpli ed picture, then, the analysis of a magnetic circuit is analogous to that of resistive electrical circuits This analogy is illustrated in Table 163 and in the examples in this section

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Table 163 Analogy between electric and magnetic circuits Electrical quantity Electrical eld intensity, E, V/m Voltage, v, V Current, i, A Current density, J , A/m2 Resistance, R, Conductivity, , 1/ m Magnetic quantity Magnetic eld intensity, H , A t/m Magnetomotive force, F , A t Magnetic ux, , Wb Magnetic ux density, B, Wb/m2 Reluctance, R = l/ A, A t/Wb Permeability, , Wb/A m

Directional, stabilizing, and disruptive selection. Colored areas show the groups being selected against. At the top is the original distribution of individuals. The nal distributions after selection appear in the bottom row.

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The usefulness of the magnetic circuit analogy can be emphasized by analyzing a magnetic core similar to that of Figure 1612, but with a slightly modi ed geometry Figure 1613 depicts the magnetic structure and its equivalent circuit analogy In the gure, we see that the mmf, F = N i, excites the magnetic circuit, which is composed of four legs: two of mean path length l1 and cross-sectional area A1 = d1 w, and the other two of mean length l2 and cross section A2 = d2 w Thus, the reluctance encountered by the ux in its path around the magnetic core is given by the quantity Rseries , with Rseries = 2R1 + 2R2 and R1 = l1 A1 R2 = l2 A2

It is instructive to verify (at least the rst time the method is applied) that it is not necessary to apply KCL at the reference node The equation obtained at node c, i1 i3 iS = 0 (34)

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the other end of the phenotypic distribution; in our example, the mean shifts toward long-necked giraffes. The evolution of neck length in giraffes, presumably by directional selection, has been documented from the geologic record. Stabilizing selection ( g. 20.9) works by constantly removing individuals from both ends of a phenotypic distribution, thus maintaining the same mean over time. Stabilizing selection now works on giraffe neck length it is neither increasing nor decreasing. Disruptive selection works by favoring individuals at both ends of a phenotypic distribution at the expense of individuals in the middle. It, like stabilizing selection, should maintain the same mean value for the phenotypic distribution. Disruptive selection has been carried out successfully in the laboratory for bristle number in Drosophila. Starting with a population with a mean number of sternopleural chaeta (bristles on one of the body plates) of about eighteen, investigators succeeded after twelve generations of getting a y population with one peak of bristle numbers at about sixteen and another at about twenty-three ( g. 20.10).

is not independent of equations 32 and 33; in fact, it may be obtained by adding the equations obtained at nodes a and b (verify this, as an exercise) This observation con rms the statement made earlier: In a circuit containing n nodes, we can write at most n 1 independent equations

Now, in applying the node voltage method, the currents i1 , i2 , and i3 are expressed as functions of va , vb , and vc , the independent variables Ohm s law requires that i1 , for example, be given by va vc (35) i1 = R1 since it is the potential difference, va vc , across R1 that causes the current i1 to ow from node a to node c Similarly, va vb i2 = R2 (36) vb vc i3 = R3

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