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From the material developed thus far, it should be apparent that electromagnetomechanical devices are capable of converting mechanical forces and displacements to electromagnetic energy, and that the converse is also possible The objective of this section is to formalize the basic principles of energy conversion in electromagnetomechanical systems, and to illustrate its usefulness and potential for application by presenting several examples of energy transducers A transducer is a device that can convert electrical to mechanical energy (in this case, it is often called an actuator), or vice versa (in which case it is called a sensor) Several physical mechanisms permit conversion of electrical to mechanical energy and back, the principal phenomena being the piezoelectric effect,3 consisting of the generation of a change in electric eld in the presence of strain in

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PROBLEM 2: Given a population of about one million cicadas with a frequency of the a allele at the A locus of 0.75, what is the probability that the a allele will be lost due to random genetic drift How much longer will the possible loss of the allele take than the loss of the allele would take in a population of one thousand

Answer: Regardless of the size of a nite population, random genetic drift takes place. The probability of the loss of an allele with a frequency of 0.75 is 0.25; the prob-

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certain crystals (eg, quartz), and electrostriction and magnetostriction, in which changes in the dimension of certain materials lead to a change in their electrical (or magnetic) properties Although these effects lead to many interesting applications, this chapter is concerned only with transducers in which electrical energy is converted to mechanical energy through the coupling of a magnetic eld It is important to note that all rotating machines (motors and generators) t the basic de nition of electromechanical transducers we have just given Forces in Magnetic Structures Mechanical forces can be converted to electrical signals, and vice versa, by means of the coupling provided by energy stored in the magnetic eld In this subsection, we discuss the computation of mechanical forces and of the corresponding electromagnetic quantities of interest; these calculations are of great practical importance in the design and application of electromechanical actuators For example, a problem of interest is the computation of the current required to generate a given force in an electromechanical structure This is the kind of application that is likely to be encountered by the engineer in the selection of an electromechanical device for a given task As already seen in this chapter, an electromechanical system includes an electrical system and a mechanical system, in addition to means through which the two can interact The principal focus of this chapter has been the coupling that occurs through an electromagnetic eld common to both the electrical and the mechanical system; to understand electromechanical energy conversion, it will be important to understand the various energy storage and loss mechanisms in the electromagnetic eld Figure 1637 illustrates the coupling between the electrical and mechanical systems In the mechanical system, energy loss can occur because of the heat developed as a consequence of friction, while in the electrical system, analogous losses are incurred because of resistance Loss mechanisms are also present in the magnetic coupling medium, since eddy current losses and hysteresis losses are unavoidable in ferromagnetic materials Either system can supply energy, and either system can store energy Thus, the gure depicts the ow of energy from the electrical to the mechanical system, accounting for these various losses The same ow could be reversed if mechanical energy were converted to electrical form.

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nesses of the genotypes of an electrophoretic locus (malate dehydrogenase) are determined. Three genotypes, FF, FS, and SS, have tnesses of 0.85, 1.0, and 0.6, respectively. What is the equilibrium frequency of the slow allele (S) Answer: If the tnesses of the three genotypes FF, FS, and SS are as given, then the locus is exhibiting heterozygote advantage with selection coef cients of the two homozygotes of s1 0.15 (1 0.85) and s2 0.4 (1 0.6). If q is the frequency of the slow allele, then, using equation 20.24,

Known Quantities: Source currents, resistor values Find: All node voltages and branch currents Figure 36

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