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

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206 Chapter Seven<br />

“starving” the zener diode from its holding current when the current<br />

flow through R L<br />

was maximum. The nearest standard value below 3.98<br />

ohms is 3.9 ohms, which is the best choice. By using any of the familiar<br />

power equations, the power dissipated by R1 comes out <strong>to</strong> be about<br />

1 watt. A 2-watt resis<strong>to</strong>r should be used <strong>to</strong> provide a good safety margin.<br />

The worst-case power dissipation condition for ZD occurs when there<br />

is no current flow through R L<br />

. If all current flow through R L<br />

ceases, the<br />

full 502 milliamps must flow through ZD. Actually, the maximum current<br />

flow through ZD could be as high as 513 milliamps because you<br />

chose a 3.9-ohm resis<strong>to</strong>r for R1 instead of the calculated 3.98 ohms. The<br />

power dissipated by ZD is the voltage across it (12 volts), multiplied by<br />

the current flow through it (the worst case is 513 milliamps). This is the<br />

familiar power equation P IE. The answer is 6.15 watts. Therefore, ZD<br />

would need <strong>to</strong> be a 12-volt, 10-watt zener with an appropriate heatsink.<br />

Another option would be <strong>to</strong> use two 5-watt, 6-volt zeners in series. The<br />

latter option eliminates the need for a heatsink, but care must be exercised<br />

<strong>to</strong> assure plenty of “air space” around the zener diodes for adequate<br />

convection cooling.<br />

As the previous design example illustrates, zener-regulated power<br />

supplies are not extremely efficient because the zener diode wastes a<br />

significant amount of power when the current flow through the load<br />

is small. For this reason, zener-regulated power supplies are typically<br />

restricted <strong>to</strong> low-power applications. However, zener diodes are commonly<br />

used as voltage references in high-power circuits, as is illustrated<br />

later in this chapter.<br />

Varac<strong>to</strong>r Diodes<br />

Going back <strong>to</strong> diode fundamentals, you might recall that when a diode is<br />

reverse-biased, a “depletion region” of current carriers is formed around<br />

the junction area. This depletion region acts as an insula<strong>to</strong>r resulting<br />

in the restriction of any appreciable current flow. A side effect of this<br />

depletion region is <strong>to</strong> look like the dielectric of a capaci<strong>to</strong>r, with<br />

the anode and cathode ends of the diode acting like capaci<strong>to</strong>r plates. As the<br />

reverse-bias voltage across a capaci<strong>to</strong>r is varied, the depletion region will<br />

also vary in size. This gives the effect of varying the distance between the<br />

plates of a capaci<strong>to</strong>r, which varies the capacitance value. A diode that is<br />

specifically designed <strong>to</strong> take advantage of this capacitive effect is called a<br />

varac<strong>to</strong>r diode. In essence, a varac<strong>to</strong>r is a voltage-controlled capaci<strong>to</strong>r.

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