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In 1968, the FCC convened the Cellular Docket, a contentious and highly visible collection of lawmakers who eventually ruled that mobile telephony s concerns could only be solved by giving them spectrum In 1970, the FCC reallocated UHF channels 70 to 83 from television to mobile services From the resulting 115-MHz electromagnetic chunk, 75 MHz was allocated to mobile telephony, with 40 MHz available immediately and 35 MHz held in reserve Once the spectrum was allocated, the political games began It was roundly assumed that AT&T would design, install, and operate the wireless network as an extension of its own universal wireline network After all, the spectrum allocation was deeded to the wireline telephone companies, and because AT&T provided service to roughly 85 percent of the market, this assumption was somewhat natural.

10-6 Illustration for Problem 10-6.

Problem 10-6 Imagine two coils with inductances of L1 = 835 H and L 2 = 2.44 mH. Suppose they are connected in series so that their coefficient of coupling is 0.922, acting so that the coils oppose each other, as shown in Fig. 10-6. What is the net inductance of the pair

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Their Advanced Mobile Phone System (AMPS) architecture, based on the same design philosophy as the wireline network, relied on a massively expensive switching infrastructure, hundreds of cells, and centralized control of all functions AT&T s only competitors in this market were the RCCs, mentioned earlier Among them were Motorola, even then a large player in the industry Initially, Motorola sided with AT&T, but when AT&T chose other vendors to manufacture the equipment required to establish the network, Motorola changed its spots and sided with the other 500 and some-odd RCCs in the country to sue the FCC for unfair treatment Their suit called for the Commission to deny AT&T s application for the development of AMPS and to re-examine the spectrum allocation In 1970, Motorola, in partnership with another large RCC, applied for permission to offer wireless service in Washington, DC.

First, calculate M. Notice that the coil inductances are specified in different units. Convert them both to microhenrys, so that L2 becomes 2440 H. Then M 0.922(835 2440)1/ 2 1316 H. The total inductance is therefore L L1 L2 2M 835 2440 2632 643 H. It is possible for mutual inductance to increase the total series inductance of a pair of coils by as much as a factor of 2, if the coupling is total and if the flux reinforces. Conversely, it is possible for the inductances of two coils to cancel each other. If two equal-valued inductors are connected in series so that their fluxes oppose, the result will be theoretically zero inductance.

Problem 10-6.

The simplest inductors (besides plain, straight lengths of wire) are coils. A coil can be wound on a plastic, wooden or other nonferromagnetic material, and it will work very well, although no air-core inductor can have very much inductance. In practice, the maximum attainable inductance for such coils is about 1 mH. Air-core coils are used mostly at radio frequencies, in transmitters, receivers, and antenna networks. In general, the higher the frequency of an alternating current, the less inductance is needed to produce significant effects. Air-core coils can be made to have

After examining the petition, the courts decided that the answer to the industry s woes lay in a competitive market In 1980, they began another cellular rulemaking.

190 Inductance almost unlimited current-carrying capacity, just by using heavy-gauge wire and making the radius of the coil large. Air does not dissipate much energy in the form of heat; it is almost lossless. For these reasons, air-core coils can be made highly efficient.

First, calculate M from k. The coil inductances are specified in different units. Let s use microhenrys for our calculations, so L 2 = 2440 H. Then M = 0.922(835 2440)1/2 = 1316 H. Then figure the total inductance. It is L = L1 + L 2 2M = 835 + 2440 2632 = 643 H.

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