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But then, knowing the eld intensity, we can relate the mmf of the coil, F, to the product of the magnetic eld intensity, H , and the length of the magnetic (mean) path, l, for one leg of the structure: F =N i =H l (1628)

16

The term components can mean a number of things, but it all comes down to creating small, reusable sections of code You can accomplish this by creating sets of programming statements and saving them in one or more files With the proper use of components, the individual parts of your applications can be created and tested before they are combined into a whole application This is just what is done in the applications you may be asked to unit test In fact, unit testing is such an important part of testing nowadays because the use of components is so prevalent In this chapter, you will examine some important principals of how modern applications are programmed into components, and how you can use these same principals to create your own reusable testware components.

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In summary, the mmf is equal to the magnetic ux times the length of the magnetic path, divided by the permeability of the material times the cross-sectional area: F = l A (1629)

.

A review of this formula reveals that the magnetomotive force, F, may be viewed as being analogous to the voltage source in a series electrical circuit, and that the ux, , is then equivalent to the electrical current in a series circuit and the term l/ A to the magnetic resistance of one leg of the magnetic circuit You will note that the term l/ A is very similar to the term describing the resistance of a cylindrical conductor of length l and cross-sectional area A, where the permeability, , is analogous to the conductivity, The term l/ A occurs frequently enough to be assigned the name of reluctance, and the symbol R It is also important to recognize the relationship between the reluctance of a magnetic structure and its inductance This can be derived easily starting from equation 1614: N N Ni N2 = = = i i i R R

(1630)

In summary, when an N -turn coil carrying a current i is wound around a magnetic core such as the one indicated in Figure 1612, the mmf, F, generated by the coil produces a ux, , that is mostly concentrated within the core and is assumed to be uniform across the cross section Within this simpli ed picture, then, the analysis of a magnetic circuit is analogous to that of resistive electrical circuits This analogy is illustrated in Table 163 and in the examples in this section

Table 163 Analogy between electric and magnetic circuits Electrical quantity Electrical eld intensity, E, V/m Voltage, v, V Current, i, A Current density, J , A/m2 Resistance, R, Conductivity, , 1/ m Magnetic quantity Magnetic eld intensity, H , A t/m Magnetomotive force, F , A t Magnetic ux, , Wb Magnetic ux density, B, Wb/m2 Reluctance, R = l/ A, A t/Wb Permeability, , Wb/A m

You will see how your components can use the principals of OOP to allow your future projects to take advantage of your earlier work To do this, you will first build a simple bug-reporting application with all the programming statements in one code file You will then separate these statements into sets of reusable statements, called methods These methods will be reorganized again into a set of methods and placed into classes Later, these classes themselves will be divided into different code files at first and then into different component files (exes and dlls) after that Finally, you will see how you can reuse these methods and classes in these component files for other projects by changing (or morphing ) them into slightly different versions of your original design..

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