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Tab Electronics Guide to Understanding Electricity ... - Sciences Club

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Capacitance<br />

151<br />

Many of the more expensive DVMs are specified as measuring true<br />

rms. If you are using this type of DVM <strong>to</strong> measure the ripple content,<br />

the indication you’ll obtain will be the true rms value. The majority<br />

of DVMs, however, will give an accurate rms voltage measurement of<br />

sine-wave AC only. Referring back <strong>to</strong> Fig. 5-5, note that the ripple waveshape<br />

is not a sine wave; it is more like a “saw<strong>to</strong>oth” (you’ll learn more<br />

about differing waveshapes in succeeding chapters). The point here is<br />

that there can be some error in the ripple measurement you just performed.<br />

High accuracy is not important in this case, but you can<br />

experience circumstances in the future, where you must consider the<br />

type of AC waveshape that you are measuring with a DVM, and compensate<br />

accordingly.<br />

As an additional test, I used a 100-ohm, 25-watt resis<strong>to</strong>r <strong>to</strong> apply a load<br />

<strong>to</strong> the circuit. If you have a comparable resis<strong>to</strong>r, you might want <strong>to</strong> try<br />

this also, but be careful with the resis<strong>to</strong>r; it gets hot.<br />

The resis<strong>to</strong>r is connected across each capaci<strong>to</strong>r, and the subsequent AC<br />

and DC voltage measurements are taken. The loading effect was practically<br />

identical between the positive and negative supplies, which is <strong>to</strong> be<br />

expected. The DC voltage dropped by about 3.1 volts, and the ripple voltage<br />

increased <strong>to</strong> about 135 mV. These effects are typical.<br />

Food for Thought<br />

Throughout this chapter, I have followed a more traditional, and commonly<br />

accepted, method of teaching and analyzing capaci<strong>to</strong>r theory.<br />

I suggest that you continue <strong>to</strong> comprehend capaci<strong>to</strong>r operation from<br />

this perspective. However, in the interest of accuracy, you will find the<br />

following s<strong>to</strong>ry <strong>to</strong> be of interest.<br />

Michael Faraday, the great English chemist and physicist, had a theory<br />

that more closely approaches the way a capaci<strong>to</strong>r really works. His<br />

theory stated that the charge is actually contained in the dielectric<br />

material—not the capaci<strong>to</strong>r’s plates. Inside the dielectric material are<br />

tiny molecular dipoles arranged in a random fashion. Applying a voltage<br />

<strong>to</strong> the plates of a capaci<strong>to</strong>r stresses these dipoles causing them <strong>to</strong> line up<br />

in rows, s<strong>to</strong>ring the energy by their alignment. In many ways, this is<br />

similar <strong>to</strong> the physical change occurring in iron, when it becomes<br />

a temporary magnet by being exposed <strong>to</strong> magnetic flux lines. When a<br />

capaci<strong>to</strong>r is discharged, the dipoles flex back like a spring, and their<br />

energy is released.

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