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Another experiment involves passing a current-carrying wire through the paper at a right angle, as shown in Fig. 8-3. The iron filings will be grouped along circles centered at the point where the wire passes through the paper. Physicists consider magnetic fields to be comprised of flux lines. The intensity of the field is determined according to the number of flux lines passing through a certain cross section, such as a square centimeter or a square meter. The lines don t really exist as geometric threads in space, or as anything solid, but it is intuitively appealing to imagine them, and the iron filings on the paper really do bunch themselves into lines when there is a magnetic field of sufficient strength to make them move.

Of course, g.lite is not without its detractors. A number of vendors have pointed out that if g.lite requires the installation of microfilters at the premises on a regular basis, then true splitterless DSL is a myth, because microfilters are in effect a form of splitter. They contend that if the filters are required anyway, then they might as well be used in fullservice ADSL deployments to guarantee a high-quality service delivery. Unfortunately, this flies in the face of one of the key tenets of g.lite, which is to simplify and reduce the cost of DSL deployment by eliminating the need for an installation dispatch (a truck roll in the industry s parlance). The key to g.lite s success in the eyes of the implementers is to eliminate the dispatch, minimize the impact on traditional POTS telephones, reduce costs, and extend the achievable drop length. Unfortunately, customers still have to be burdened with the installation of microfilters, and coupled noise on POTS is higher than expected. Many vendors argue that these problems largely disappear with full-feature ADSL using splitters; a truck dispatch is still required, but again, it is often required to install the microfilters anyway, so there is no net loss. Furthermore, a number of major semiconductor manufacturers support both g.lite and ADSL on the same chipset, so the decision to migrate from one to the other is a simple one that does not necessarily involve a major replacement of internal electronics.

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A magnetic field has a direction at any given point in space near a current-carrying wire or a permanent magnet. The flux lines run parallel with the direction of the field. A magnetic field is considered to begin at the north magnetic pole, and to terminate at the south magnetic pole. In the case of a permanent magnet, it is obvious where these poles are.

when the current stops flowing in the coil. Retentivity, also sometimes called remanence, is a measure of how well the substance memorizes the magnetism and thereby becomes a permanent magnet. Retentivity is expressed as a percentage, and is symbolized Br. If the flux density in the material is x tesla or gauss when it is subjected to the greatest possible magnetomotive force, and then goes down to y tesla or gauss when the current is removed, the retentivity is equal to 100( y/x)%. Suppose that a metal rod can be magnetized to 135 G when it is enclosed by a coil carrying an electric current. Imagine that this is the maximum possible flux density that the rod can be forced to have. (For any substance, there is always such a maximum.) Now suppose that the current is shut off, and 19 G remain in the rod. Then the retentivity, Br, is calculated as follows: Br = 100(19/135)% = (100 0.14)% = 14% Some ferromagnetic substances have high retentivity. These materials are excellent for making permanent magnets. Other substances have low retentivity. They work well as electromagnets, but not as permanent magnets. If a ferromagnetic substance has poor retentivity, it is especially well-suited for use as the core material for an ac electromagnet, because the polarity of the magnetic flux can reverse within the material at a rapid rate. Materials with high retentivity do not work well for ac electromagnets, because they resist the polarity reversal that takes place with ac.

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With a current-carrying wire, the magnetic field just goes around and around endlessly, like a dog chasing its own tail. A charged electric particle, such as a proton, hovering in space, is a monopole, and the electric flux lines around it aren t closed (Fig. 8-4). A positive charge does not have to be mated with a negative charge. The electric flux lines around any stationary, charged particle run outward in all directions for a theoretically infinite distance.

Magnetism has numerous applications in common consumer devices and systems. Here are some of the more common ways in which magnetic phenomena can be put to use.

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