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Home Fundamentals Capacitance and Inductance Introduction | ||||
See also: Effective Input Capacitance, Capacitance and Condensers | ||||
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Capacitance and InductanceAuthor: J.B. Hoag Suppose we rub a glass rod with a piece of silk. The glass rod will become positively charged and the silk negatively charged. We have not created electricity. Nor can it be destroyed. It can only be transferred from one body to another. A neutral body contains equal amounts of positive and negative electricity, and when electrons are added to it, it is negatively charged; when they are removed, it is positively charged.
The directions of the lines of force are very important, for they represent the paths along which free electrical charges tend to move. We can control the motion of the electrons in radio and cathode-ray tubes by sending them through properly designed electrical fields. Figure 3 A shows some electrical fields around metal balls and plates connected to batteries of various potentials, together with the apparatus used to measure the fields (an electrolytic trough). Also in this figure, there are some lines everywhere at right angles to the lines of force. These correspond to the contour lines of a map and are called equipotential lines, for the voltage or potential is everywhere equal along a given line. We shall return to the discussion and use of lines of force and equipotential lines in a later chapter.
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