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In practical electromagnetic circuits, the self-inductance of a circuit is not necessarily constant; in particular, the inductance parameter, L, is not constant, in general, but depends on the strength of the magnetic eld intensity, so that it will not be possible to use such a simple relationship as v = L di/dt, with L constant If we revisit the de nition of the transformer voltage, e=N d dt (1613)

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Figure 20.7 Continued genetic drift in the one thousand populations, each numbering one hundred in size, shown in gures 20.5 and 20.6. After approximately 2N generations, the distribution is at, and populations are going to loss or xation of the a allele at a rate of 1/2N populations per generation. (From

we see that in an inductor coil, the inductance is given by L= N = i i (1614)

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This expression implies that the relationship between current and ux in a magnetic structure is linear (the inductance being the slope of the line) In fact, the properties of ferromagnetic materials are such that the ux-current relationship is nonlinear, as we shall see in Section 163, so that the simple linear inductance parameter used in electric circuit analysis is not adequate to represent the behavior of the magnetic circuits of the present chapter In any practical situation, the relationship between the ux linkage, , and the current is nonlinear, and might be described by a curve similar to that shown in Figure 168 Whenever the i- curve is not a straight line, it is more convenient to analyze the magnetic system in terms of energy calculations, since the corresponding circuit equation would be nonlinear In a magnetic system, the energy stored in the magnetic eld is equal to the integral of the instantaneous power, which is the product of voltage and current, just as in a conventional electrical circuit: Wm = ei dt (1615)

i (A)

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However, in this case, the voltage corresponds to the induced emf, according to Faraday s law: e= d d =N dt dt (1616)

back into the gene pool, these populations maintain a constant allelic frequency of zero or 1.0. At a point between N (one hundred) and 2N (two hundred) generations, the distribution of allelic frequencies attens out and begins to lose populations to the edges ( xation or loss) at a constant rate, as shown in gure 20.7. The rate of loss is about 1/2N (1/200), or 0.5% of the populations per generation. If the initial allelic frequency was not 0.5, everything is shifted in the distribution ( g. 20.8), but the basic process is the same in all populations, sampling error causes allelic frequencies to drift toward xation or elimination. If no other factor counteracts this drift, every population is destined to eventually be either xed for or de cient in any given allele. The amount of time the process takes depends on population size. The example used here was based on small populations of one hundred. If we substitute one million for one hundred in gure 20.6, a at distribution of populations would not be reached for two million generations, rather than two hundred generations. Thus, a population experiences the effect of random genetic drift in inverse proportion to its size: Small populations rapidly x or lose a given allele, whereas large populations take longer to show the same effects. Genetic drift also shows itself in several other ways.

Random genetic drift in small populations with q 0.1. Compare this gure with gure 20.6. In this case, the probability of xation of the a allele is 0.1, and the probability of its loss is 0.9. (From M. Kimura, Solution of a process of random

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and is therefore related to the rate of change of the magnetic ux The energy stored in the magnetic eld could therefore be expressed in terms of the current by the integral Wm = ei dt = d i dt = dt i d (1617)

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