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One of the biggest challenges in acoustical design is the avoidance of significant antinodes and nodes In a home hi-fi system, this can be as simple as minimizing the extent to which sound waves reflect from the ceiling, the walls, the floor, and the furniture Acoustical tile can be used on the ceiling, the walls can be papered or covered with cork tile, the floor can be carpeted, and the furniture can be upholstered with cloth In large auditoriums and music halls, the problem becomes more complex because of the larger sound propagation distances involved, and also because of the fact that sound waves reflect from the bodies of the people in the audience!.

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Then calculate jBC j(6.28fC). Convert picofarads to microfarads, and use megahertz for the frequency. Therefore jBC j(6.28 1.592 0.001000) j0.0100

Regardless of its size, a good hi-fi sound system must have certain characteristics. Here are two of the most important technical considerations.

Let the conductance and inductive susceptance go together as one vector, 0.100 j0.0100. (Remember that conductance is the reciprocal of resistance; here G

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Linearity Linearity is the extent to which the output waveform of an amplifier is a faithful reproduction of the input waveform In hi-fi equipment, all the amplifiers must be as linear as the state of the art allows If you connect a dual-trace oscilloscope (one that lets you observe two waveforms at the same time) to the input and output terminals of a hi-fi audio amplifier with good linearity, the output waveform is a vertically magnified duplicate of the input waveform When the input signal is applied to the horizontal scope input and the output signal is applied to the vertical scope input, the display is a straight line In an amplifier with poor linearity, the instantaneous output-versus-input function is not a straight line The output waveform is not a faithful reproduction of the input, and distortion occurs In some RF amplifiers this is all right.

294 RLC circuit analysis 1/R 1/10.0 0.100.) Let the capacitance alone be the other vector, 0 j0.0100. Then the sum is 0.100 j0.0100 j0.0100 0. 100 j0. This is a pure conductance of 0.100 siemens.

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Communication, which is now universally accepted as the framework for modern communications. We won t delve into the complex (but fascinating) mathematics that underlie Shannon s Theorem, but suffice it to say that his conclusions are seminal: the higher the noise level in a circuit, the lower the achievable bandwidth. The bottom line Noise matters. It matters so much, in fact, that network designers and engineers make its elimination the first order of business in their overall strategies for creating high-bandwidth networks. This is one of the reasons that optical fiber-based networks have become so critically important in modern transport systems they are far less subject to noise and absolutely immune to the electromagnetic interference that plagues copper-based networks. Cable companies that now offer data services have the same issues and concerns. Every time a customer decides to play installer by adding a cable spur for a new television set in their home and crimping the connector on the end of the cable with a pair of pliers instead of a tool specifically designed for the purpose, they create a point where noise can leak into the system, causing problems for everyone. It gets even more melodramatic than that: According to John Judson, a cable systems maintenance manager in the Midwest, unauthorized connection to the cable network can cause problems that go way beyond unauthorized access to service. Cable networks are high-frequency systems, he observes. Some of the harmonics created in cable networks just happen to fall within the range of frequencies used in avionics, and therefore have the potential to affect aviation communications and nav-

The GB plane is, as you have seen, similar in appearance to the RX plane, although mathematically the two are worlds apart. Once you ve found a complex admittance for a parallel RLC circuit, how do you transform this back to a complex impedance Generally, it is the impedance, not the admittance, that technicians and engineers work with. The transformation from complex admittance, or a vector G jB, to a complex impedance, or a vector R jX, requires the use of the following formulas: R X G/(G2 B2) B/(G2 B 2)

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