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The derivative of the reluctance with respect to the displacement of the plunger can then be computed to be: dRgap (x) 2 = dx 0 Agap Knowing the reluctance, we can calculate the magnetic ux in the structure as a function of the coil current: N i 0 Agap Ni = = 2 R(x) and the force in the air gap is given by the expression fgap = (Ni 0 Agap )2 2 0 Agap (Ni)2 2 dR(x) = = 2 dx 0 Agap 8 4 0 Agap (Ni)2 = frestore = 5 N 4 1 4frestore = 0 Agap 10,000 20 = 399 A 4 10 7 00001

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hold the relay closed, because the reluctance of the structure is much smaller once the gap is reduced to zero

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In Search of the Genetic Material 205 Required Properties of a Genetic Material 205 Evidence for DNA as the Genetic Material 209 Chemistry of Nucleic Acids 211 Biologically Active Structure 214 Requirements of Genetic Material 218 Alternative Forms of DNA 219 DNA Replication_The Process 220 The Meselson and Stahl Experiment 220 Autoradiographic Demonstration of DNA Replication 222 DNA Replication_The Enzymology 225 Continuous and Discontinuous DNA Replication 225 The Origin of DNA Replication 229 Events at the Y-Junction 232 Supercoiling 234 Termination of Replication 236 DNA Partitioning in E. coli 238 Replication Structures 238 Rolling-Circle Model 238 D-Loop Model 238 Eukaryotic DNA Replication 238 Summary 240 Solved Problems 240 Exercises and Problems 241 Critical Thinking Questions 242 Box 9.1 Molecular Structure of Nucleic Acids: A Structure for Deoxyribose Nucleic Acid 206 Box 9.2 Prions: The Biological Equivalent of Ice-Nine 213 Box 9.3 Multiple-Stranded DNA 221

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This chapter gives a state-of-the-art review of many books and papers to help the readers understand the basics of the performance and application of microelectromechanical systems The authors considered in the review are 1 Michalicek, MA, Introduction to Microelectromechanical Systems, Air Force Research Laboratory, New Mexico, 2000 2 Hsu, TR, MEMS and Microsystems Design and Manufacture, McGraw Hill, 2002 3 MacDonald, NC, Microelectromechanical Systems (MEMS) Paradigms, Cornell University MEMS is the acronym for Micro Electro Mechanical Systems In Europe, MEMS are more commonly known as microsystems [1] MEMS can generally be defined as highly miniaturized devices or arrays of devices combining electrical and mechanical components, such as sensors, valves, actuators or complete systems, which are fabricated by using integrated circuit (IC) batch-processing techniques [2] Typically, MEMS contain components of sizes ranging from 1 micrometre ( m) to 1 millimetre (mm) For comparison purposes, Figure 81 shows a MEMS device (gear) alongside a human hair which is of a size of about 100 m [3] From the name itself, it can be understood that MEMS is able to achieve engineering functions through electromechanical means The current MEMS technology also incorporates thermal, magnetic, electrochemical, fluidic and optical devices Basically, the first effort to spur innovative miniature fabrication techniques for micromechanics was made by Richard Feynman in 1959 [4] However, his efforts failed to generate a fundamentally new fabrication technique In 1969, Westinghouse created the resonant gate Field-Effect Transistor (FET) based on new microelectronics fabrication techniques [2] Bulk-etched silicon wafers were used as pressure sensors in the 1970s, while the early experiments on surface-micromachined polysilicon were started in the 1980s The microelectronics industry enjoyed a great progress in the

Moving-Coil Transducers Another important class of electromagnetomechanical transducers is that of moving-coil transducers This class of transducers includes a number of common devices, such as microphones, loudspeakers, and all electric motors and generators The aim of this section is to explain the relationship between a xed magnetic eld, the emf across the moving coil, and the forces and motions of the moving element of the transducer The basic principle of operation of electromechanical transducers was presented in Section 161, where we stated that a magnetic eld exerts a force on a charge moving through it The equation describing this effect is f = qu B (1651)

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which is a vector equation, as explained earlier In order to correctly interpret equation 1651, we must recall the right-hand rule and apply it to the transducer, illustrated in Figure 1647, depicting a structure consisting of a sliding bar which makes contact with a xed conducting frame Although this structure does not represent a practical actuator, it will be a useful aid in explaining the operation of moving-coil transducers such as motors and generators In Figure 1647, and in all similar gures in this section, a small cross represents the tail of an arrow pointing into the page, while a dot represents an arrow pointing out of the page; this convention will be useful in visualizing three-dimensional pictures

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