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Figure 1610 illustrates the magnetic ux lines in the vicinity of a coil The magnetic eld generated by the coil can be made to generate a much greater ux density if the coil encloses a magnetic material The most common ferromagnetic materials are steel and iron; in addition to these, many alloys and oxides of iron as well as nickel and some arti cial ceramic materials called ferrites also exhibit magnetic properties Winding a coil around a ferromagnetic material accomplishes two useful tasks at once: it forces the magnetic ux to be concentrated near the coil and if the shape of the magnetic material is appropriate completely con nes the ux within the magnetic material, thus forcing the closed path for the ux lines to be almost entirely enclosed within the ferromagnetic material Typical arrangements are the iron-core inductor and the toroid of Figure 1611 The ux densities for these inductors are given by the expressions B= Ni l N i B= 2 r2 Flux density for tightly wound circular coil Flux density for toroidal coil (1624) (1625)

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When performing code reviews, look for the following in a well-written .NET application: Does the project Use Shared or static classes to contain logically related reusable routines Properly manage forms and their display Does the code Use understandable names for functions and procedures Create functions and procedures that are single-purpose (Large, cumbersome procedures are less reusable and intelligible. Routines should have a single, clear purpose.) Correctly distinguish between synchronous and asynchronous timing Consistently document all files

Intuitively, the presence of a high-permeability material near a source of magnetic ux causes the ux to preferentially concentrate in the high- material, rather than in air, much as a conducting path concentrates the current produced by an electric eld in an electric circuit In the course of this chapter, we shall

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continue to develop this analogy between electric circuits and magnetic circuits Figure 1612 depicts an example of a simple electromagnetic structure, which, as we shall see shortly, forms the basis of the practical transformer Table 162 summarizes the variables introduced thus far in the discussion of electricity and magnetism

Mean path of magnetic flux lines (note how the path of the flux is enclosed within the magnetic structure)

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s you know, testing jobs are becoming more demanding every day Employers demand that their testers be more productive, which often translates into having to know not only testing and documenting, but also how to automate testing procedures and programs in general In the last chapter, you saw how to create simple automations Automation is a very important tool for testers, but creating good automation tools, or testware, takes time When you do write these testware applications, it is vital that you get the most benefit for your efforts This means first identifying tasks that can be automated and then creating code that can be reused It also means designing your code to be simple enough that it can be modified for other projects without a great deal of time and expense To create efficient testing utilities, you need to learn to break your tasks into small, reusable components.

Table 162 Magnetic variables and units Variable Current Magnetic ux density Magnetic ux Magnetic eld intensity Electromotive force Magnetomotive force Flux linkage Symbol I B H e F Units A Wb/m2 = T Wb A/m V A t Wb t

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161 A coil having 100 turns is immersed in a magnetic eld that is varying uniformly from 80 mWb to 30 mWb in 2 seconds Find the induced voltage in the coil 162 The magnitude of H at a radius of 05 m from a long linear conductor is 1 A m 1 Find the current in the wire 163 The relation between the ux linkages and the current for a magnetic material is given by = 6i/(2i + 1) Wb t Determine the energy stored in the magnetic eld for = 2 Wb t 164 Verify that for the linear case, where the ux is proportional to the mmf, the energy stored in the magnetic eld is 1 Li 2 2

It is possible to analyze the operation of electromagnetic devices such as the one depicted in Figure 1612 by means of magnetic equivalent circuits, similar in many respects to the equivalent electrical circuits of the earlier chapters Before we can present this technique, however, we need to make a few simplifying approximations The rst of these approximations assumes that there exists a mean path for the magnetic ux, and that the corresponding mean ux density is approximately constant over the cross-sectional area of the magnetic structure Thus, a coil wound around a core with cross-sectional area A will have ux density (1626) A where A is assumed to be perpendicular to the direction of the ux lines Figure 1612 illustrates such a mean path and the cross-sectional area, A Knowing the ux density, we obtain the eld intensity: B= H = B = A (1627)

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