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You can probably see intuitively that the rst of these assumptions might not hold true near the ends of the coil, but that it might be more reasonable if the coil is tightly wound The second assumption is equivalent to stating that the relative permeability of the core is in nitely higher than that of air (presuming that this is the medium surrounding the core): if this were the case, the ux would indeed be con ned within the core It is worthwhile to note that we make a similar assumption when we treat wires in electric circuits as perfect conductors: the conductivity of copper is substantially greater than that of free space, by a factor of approximately 1015 In the case of magnetic materials, however, even for the best alloys, we have a relative permeability only on the order of 103 to 104 Thus, an approximation that is quite appropriate for electric circuits is not nearly as good in the case of magnetic circuits Some of the ux in a structure such as those of Figures 1612 and 1613 would thus not be con ned within the core (this is usually referred to as leakage ux) Finally, the assumption that the ux is uniform across the core cannot hold for a nite-permeability medium, but it is very helpful in giving an approximate mean behavior of the magnetic circuit The magnetic circuit analogy is therefore far from being exact However, short of employing the tools of electromagnetic eld theory and of vector calculus, or advanced numerical simulation software, it is the most convenient tool at the engineer s disposal for the analysis of magnetic structures In the remainder of this chapter, the approximate analysis based on the electric circuit analogy will be used to obtain approximate solutions to problems involving a variety of useful magnetic circuits, many of which you are already familiar with Among these will be the loudspeaker, solenoids, automotive fuel injectors, sensors for the measurement of linear and angular velocity and position, and other interesting applications.

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q(q sq p) 1 sq2 q(1 sq) 1 sq2 (20.15)

Find: ; B; H Schematics, Diagrams, Circuits, and Given Data: r = 1,000; N = 500 turns; i = 01 A The magnetic circuit geometry is de ned in Figures 1614 and 1615 Assumptions: All magnetic ux is linked by the coil; the ux is con ned to the magnetic core; the ux density is uniform Analysis:

This model can be simpli ed somewhat if we assume that the aa genotype is lethal. Its tness would be zero,

Therefore, it is possible to produce a hydrostatic bearing for a required load capacity and stiffness with a lower friction power loss However, it is not economical to produce a hydrostatic bearing of a

Calculation of magnetomotive force From equation 1628, we calculate the magnetomotive force: F = mmf = N i = (500 turns)(01 A) = 50 A t

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Calculation of mean path Next, we estimate the mean path of the magnetic ux On the basis of the assumptions, we can calculate a mean path that runs through the geometric center of the magnetic structure, as shown in Figure 1615 The path length is: lc = 4 009 m = 036 m

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The cross sectional area is A = w 2 = (001)2 = 00001 m2 Calculation of reluctance Knowing the magnetic path length and cross sectional area we can calculate the reluctance of the circuit: lc lc 036 R= = = = 2865 106 A t/Wb A r 0 A 1,000 4 10 7 00001 The corresponding equivalent magnetic circuit is shown in Figure 1616 Calculation of magnetic ux, ux density and eld intensity On the basis of the assumptions, we can now calculate the magnetic ux: = 50 A t F = = 175 10 5 Wb R 2865 106 A t/Wb

q(1 q) 1 q2 q)(1

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small diameter since the cost of the pump remains the same although the requirement changes The reduction in size also reduces the rigidity of the shaft Being of a non-contact nature, air bearings avoid the traditional bearing-related problems of friction, wear, and lubricant handling, and offer distinct advantages in precision positioning and high-speed applications The choice of liquid and gas lubrication mainly depends on the type of application Moderate loads and moderate stiffness at a high speed will favour gas bearings, whereas the requirement for a high load and a high stiffness at a moderate speed favours hydrostatic bearings Figure 772 from the work of Weck [37] indicates the suitability of bearing systems for application in various precision machines The demand for a high precision, which comes with rigidity and stiffness, requires the use of aerostatic bearings, which are dominant in precision machines Processes such as hard turning results in high cutting forces, which limits the use of aerostatic bearings Due to the presence of a backlash and friction resulting from a surface-to-surface contact, rolling element bearings are seldom used in precision tools For guideways, hydrostatic bearings are the most suitable option to design machine tools due to their unique load carrying properties

the ux density:

(20.16)

175 10 5 Wb = 0175 Wb/m2 = 2 = A w 00001 m2 and the magnetic eld intensity: B= H = 0175 Wb/m2 B B = = = 139 A t/m r 0 1,000 4 10 7 H/m

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