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The rst two sections of this chapter introduced energy-storage elements and timedependent signal sources The logical next task is to analyze the behavior of circuits containing such elements The major difference between the analysis of the resistive circuits studied in s 2 and 3 and the circuits we will explore in the remainder of this chapter is that now the equations that result from applying Kirchhoff s laws are differential equations, as opposed to the algebraic equations obtained in solving resistive circuits Consider, for example, the circuit of Figure 425, which consists of the series connection of a voltage source, a resistor, and a capacitor Applying KVL around the loop, we may obtain the following equation: vS (t) = vR (t) + vC (t) (425)

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majority accept to explain the abundance of molecular variation found in natural populations. Another controversial theory concerns the rate of evolutionary change. It is suggested that most evolutionary change is not gradual, as the fossil record seems to indicate, but occurs in short, rapid bursts, followed by long periods of very little change. This theory is called punctuated equilibrium. A nal area of evolutionary biology that has generated much controversy is the theory of sociobiology. Sociobiologists suggest that social behavior is under genetic control and is acted upon by natural selection, as is any morphological or physiological trait. This idea is controversial mainly as it applies to human beings; it calls altruism into question and suggests that to some extent we are genetically programmed to act in certain ways. People have criticized the theory because they feel it justi es racism and sexism.

iC C + vC (t) _

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The purpose of this chapter has been to provide a brief history of genetics and a brief overview of the following twenty chapters. We hope it serves to introduce the material and to provide a basis for early synthesis of some of the material that, of necessity, is presented in the discrete units called chapters. This chapter also differs from all the others because it lacks some of the end materials that

Observing that iR = iC , equation 425 may be combined with the de ning equation for the capacitor (equation 45) to obtain vS (t) = RiC (t) + 1 C

10 m

Suggested Readings for chapter 1 are on page B-1.

(426)

Equation 426 is an integral equation, which may be converted to the more familiar form of a differential equation by differentiating both sides of the equation, and recalling that d dt

should be of value to you as you proceed: solved problems, and exercises and problems.These features are presented chapter by chapter throughout the remainder of the book. At the end of the book, we provide answers to exercises and problems and a glossary of all boldface words throughout the book.

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Fig 234: Morphologies of films grown in a hot filament CVD reactor: (a) triangular {111} morphology, (b) {110}

8.4 (2) 13.0 4.6

= iC (t)

(427)

Figure 6.24 Two possible arrangements of the a and b loci and their centromere. Distances are in map units.

to obtain the following differential equation: diC 1 1 dvS + iC = dt RC R dt (428)

The McGraw Hill Companies, 2001

morphology, (c) {100} morphology and (d) cauliflower morphology [39]

where the argument (t) has been dropped for ease of notation Observe that in equation 428, the independent variable is the series current owing in the circuit, and that this is not the only equation that describes the series RC circuit If, instead of applying KVL, for example, we had applied KCL at the node connecting the resistor to the capacitor, we would have obtained the following relationship: iR = or dvC 1 1 + vC = vS dt RC RC (430) vS vC dvC = iC = C R dt (429)

tetratypes plus the number of nonparental ditypes, all divided by the total number of asci, expressed as a percentage. For ordered spores (Neurospora), the distance from a locus to its centromere is one-half the percentage of second-division segregants. Mapping the distance between two loci is similar to the process in unordered spores.

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