vb.net ean 13

vb.net ean 13

vb.net ean 13

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The unit of capacitance 201 Energy will be stored in this electric field. The ability of the plates, and of the space between them, to store this energy is the property of capacitance. It is denoted by the letter C.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

It s out of the question to make a capacitor of the above dimensions. But two sheets, or strips, of foil can be placed one on top of the other, separated by a thin, nonconducting sheet such as paper, and then the whole assembly can be rolled up to get a large effective surface area. When this is done, the electric flux becomes great enough so that the device exhibits significant capacitance. In fact, two sets of several plates each can be meshed together, with air in between them, and the resulting capacitance will be significant at high ac frequencies. In a capacitor, the electric flux concentration is multiplied when a dielectric of a certain type is placed between the plates. Plastics work very well for this purpose. This increases the effective surface area of the plates, so that a physically small component can be made to have a large capacitance. The voltage that a capacitor can handle depends on the thickness of the metal sheets or strips, on the spacing between them, and on the type of dielectric used. In general, capacitance is directly proportional to the surface area of the conducting plates or sheets. Capacitance is inversely proportional to the separation between conducting sheets; in other words, the closer the sheets are to each other, the greater the capacitance. The capacitance also depends on the dielectric constant of the material between the plates. A vacuum has a dielectric constant of 1; some substances have dielectric constants that multiply the effective capacitance many times.

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When electrical energy must be sent over long distances, extremely high voltages are used. This is because, for a given amount of power ultimately dissipated by the loads, the current is lower when the voltage is higher. Lower current translates into reduced loss in the transmission line. Recall the formula P = EI, where P is the power (in watts), E is the voltage (in volts), and I is the current (in amperes). If you can make the voltage 10 times larger, for a given power level, then the current is reduced to 1 10 as much. The ohmic losses in the wires are proportional to the square of the current. Remember that P = I 2R, where P is the power (in watts), I is the current (in amperes), and R is the resistance (in ohms). Engineers can t do much about the wire resistance or the power consumed by the loads, but they can adjust the voltage, and thereby the current. Suppose the voltage in a power transmission line is increased by a factor of 10, and the load at the end of the line draws constant power. This increase in the voltage reduces the current to 1 10 of its previous value. As a result, the ohmic loss is cut to (1 10)2, or 1 100, of its previous amount. That s a major improvement in the efficiency of the transmission line, at least in terms of the loss caused by the resistance in the wires and it is the reason why regional power plants have massive transformers capable of generating hundreds of thousands of volts.

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