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permeability of free space, 0 = 4 10 7 H/m, times the relative permeability, r , which varies greatly according to the medium For example, for air and for most electrical conductors and insulators, r is equal to 1 For ferromagnetic materials, the value of r can take values in the hundreds or thousands The size of r represents a measure of the magnetic properties of the material A consequence of Amp` re s law is that, the larger the value of , the smaller the current required to e produce a large ux density in an electromagnetic structure Consequently, many electromechanical devices make use of ferromagnetic materials, called iron cores, to enhance their magnetic properties Table 161 gives approximate values of r for some common materials Conversely, the reason for introducing the magnetic eld intensity is that it is independent of the properties of the materials employed in the construction of magnetic circuits Thus, a given magnetic eld intensity, H, will give rise to different ux densities in different materials It will therefore be useful to de ne sources of magnetic energy in terms of the magnetic eld intensity, so that different magnetic structures and materials can then be evaluated or compared for a given source In analogy with electromotive force, this source will be termed magnetomotive force (mmf) As stated earlier, both the magnetic ux density and eld intensity are vector quantities; however, for ease of analysis, scalar elds will be chosen by appropriately selecting the orientation of the elds, wherever possible Amp` re s law states that the integral of the vector magnetic eld intensity, e H, around a closed path is equal to the total current linked by the closed path, i: H dl = i (1620)

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where dl is an increment in the direction of the closed path If the path is in the same direction as the direction of the magnetic eld, we can use scalar quantities to state that H dl = i (1621)

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forms and classes, as well as existing items. And you ve learned some important ways to use timing in your tests, including using the DateTime and TimeSpan classes, as well as the Timer control. You also looked at two ways to launch applications synchronously and asynchronously using the Shell() and Process.Start() methods, respectively. What we hope you will take away from this chapter is that every time you create, or run across, a useful procedure for testing, you ll throw it into a library for your future use and that of your test team. Having a code repository that you can use to quickly get yourself ready to run actual tests is one of the most important things you can create for yourself. You don t have time to write every line of code from scratch, so you ll find that you ll often leverage the code from other projects to get your automated tests written quickly. So, in other words, not only should your test project have a test framework, in the form of prewritten code libraries of common and useful routines, but also so should you! You can take these libraries from project-to-project and job-to-job to add your own value to any automated test project. The kind of class you focused on in this chapter is the static/Shared class that can simply function as a code repository. In the next chapter, you ll learn how to make and test fully objectoriented applications using standard classes and the object-oriented concepts of encapsulation, inheritance, and polymorphism.

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Figure 169 illustrates the case of a wire carrying a current i, and of a circular path of radius r surrounding the wire In this simple case, you can see that the magnetic eld intensity, H, is determined by the familiar right-hand rule This rule states that if the direction of the current i points in the direction of the thumb of one s right hand, the resulting magnetic eld encircles the conductor in the direction in which the other four ngers would encircle it Thus, in the case of Figure 169, the closed-path integral becomes equal to H (2 r), since the path and the magnetic eld are in the same direction, and therefore the magnitude of the magnetic eld intensity is given by H = i 2 r (1622)

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