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HDSL2 offers the same service that HDSL offers, with one added (and significant) advantage: it does so over a single pair of wire, rather than two. It also provides other advantages. First, it was designed to improve vendor interoperability by requiring less equipment at either end of the span (transceivers or repeaters). Second, it was designed to work within the confines of standard telephone company carrier serving area (CSA) guidelines by offering a 12,000-foot wire-run capability that matches the requirements of CSA deployment strategies. (See the discussion on CSA guidelines later in this section.) A number of companies have deployed T-1 access over HDSL2 at rates 40 percent lower than typical T-Carrier prices. Furthermore, a number of vendors including 3Com, Lucent, Nortel Networks, and Alcatel have announced their intent to work together to achieve interoperability among DSL modems.

The overall magnitude of a magnetic field is measured in units called webers (Wb). A smaller unit, the maxwell (Mx), is sometimes used if a magnetic field is weak. One weber is equivalent to 100,000,000 (108) maxwells. Conversely, 1 Mx = 0.00000001 Wb = 10 8 Wb.

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4. The voltage in a battery is: A. Less than the voltage in a cell of the same kind. B. The same as the voltage in a cell of the same kind. C. More than the voltage in a cell of the same kind. D. Always a multiple of 1.018 V. 5. A direct short-circuit of a battery can cause: A. An increase in its voltage. B. No harm other than a rapid discharge of its energy. C. The current to drop to zero. D. An explosion. 6. A cell of 1.5 V supplies 100 mA for seven hours and twenty minutes, and then it is replaced. It has supplied: A. 7.33 Ah. B. 733 mAh. C. 7.33 Wh. D. 733 mWh.

The Tesla and the Gauss If you have access to a permanent magnet or electromagnet, you might see its strength expressed in terms of webers or maxwells. But usually you ll hear units called teslas (T) or gauss (G). These units are expressions of the concentration, or intensity, of the magnetic field within a certain cross section. The flux density, or number of lines per square meter or per square centimeter, is a more useful expression for magnetic effects than the overall quantity of magnetism. A flux density of 1 tesla (1 T) is equal to 1 weber per square meter (1 Wb/m2). A flux density of 1 gauss (1 G) is equal to 1 maxwell per square centimeter (1 Mx/cm2). It turns out that the gauss is equal to 0.0001 tesla (10 4 T). Conversely, the tesla is equivalent to 10,000 gauss (104 G). The Ampere-Turn and the Gilbert With electromagnets, another unit is employed: the ampere-turn (At). This is technically a unit of magnetomotive force, which is the magnetic counterpart of electromotive force. A wire, bent into a circle and carrying 1 A of current, produces 1 At of magnetomotive force. If the wire is bent into a loop having 50 turns, and the current stays the same, the resulting magnetomotive force is 50 At. If the current is then reduced to 1/50 A or 20 mA, the magnetomotive force will go back down to 1 At. The gilbert (Gb) is also used to express magnetomotive force, but it is less common than the ampere-turn. One gilbert (1 Gb) is equal to 0.796 At. Conversely, 1 At = 1.26 Gb.

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3. A Weston cell is generally used: A. As a current reference source. B. As a voltage reference source. C. As a power reference source. D. As an energy reference source.

Any electric current, or movement of charge carriers, produces a magnetic field. This field can become intense in a tightly coiled wire that has many turns and carries a large current. When a ferromagnetic core is placed inside the coil, the magnetic lines of flux are concentrated in the core, and the field strength in and near the core can become tremendous. This is the principle of an electromagnet (Fig. 8-5). Electromagnets are almost always cylindrical in shape. Sometimes the cylinder is long and thin; in other cases it is short and fat. But whatever the ratio of diameter to length for the core, the principle is the same: the magnetic field produced by the current results in magnetization of the core.

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