09.02.2015 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

Special-Purpose Diodes and Op<strong>to</strong>electronic Devices<br />

219<br />

Figure 7-6<br />

A triple-LED<br />

flasher circuit.<br />

6 <strong>to</strong> 12 V<br />

R1 R2 R3 R4 R5 R6<br />

C1<br />

C2<br />

R1 = R3 = R5 =33 k<br />

R2 = R4 = R6 =560 <br />

C1 = C2 = C3 =100 F<br />

C3<br />

Q1 LED1<br />

LED2<br />

Q2 Q3<br />

LED3<br />

All capaci<strong>to</strong>rs rated at 16 WVdc or higher<br />

base resis<strong>to</strong>r. When the voltage across C1 reaches a high enough potential,<br />

it turns on Q2 and causes LED2 <strong>to</strong> become dark (the saturation of<br />

Q2 effectively short-circuits the voltage drop across LED2).<br />

Here is where the circuit operation becomes a little tricky. Going back<br />

<strong>to</strong> the prior condition when Q2 was in cu<strong>to</strong>ff, the voltage on the negative<br />

side of C2 was actually a little more positive than the voltage on the<br />

positive side. This is because the voltage drop across LED2 was a little<br />

higher than the base-<strong>to</strong>-emitter voltage drop of Q3. Therefore, C2 actually<br />

takes on a slight reverse voltage charge. When Q2 saturates, this has the<br />

effect of forcing Q3 in<strong>to</strong> “hard” cu<strong>to</strong>ff, because a slight negative voltage is<br />

applied <strong>to</strong> its base, before C2 has the chance <strong>to</strong> start charging in the positive<br />

direction through Q3’s 33k base resis<strong>to</strong>r. With Q3 in the cu<strong>to</strong>ff<br />

state, C3 begins <strong>to</strong> take on a small reverse charge, while C2 begins <strong>to</strong><br />

charge <strong>to</strong>ward the point where it will drive Q3 back in<strong>to</strong> saturation. The<br />

cycle continues <strong>to</strong> progress in a sequential manner, with LED1 lighting<br />

next, and so on. Even though C1, C2, and C3 are electrolytic capaci<strong>to</strong>rs,<br />

the small reverse charge is not damaging because the charging current<br />

and voltage are very low.<br />

The frequency of operation is a function of the time constant of the<br />

capaci<strong>to</strong>rs and base resis<strong>to</strong>rs. Increasing the value of either component<br />

will slow down the sequence. Any general purpose NPN transis<strong>to</strong>r<br />

should operate satisfac<strong>to</strong>rily in this circuit. The LED type is not critical,<br />

either, although you would have <strong>to</strong> adjust the resis<strong>to</strong>r values somewhat <strong>to</strong><br />

accommodate the newer “high brightness” LEDs.<br />

Many of the applications that applied <strong>to</strong> Fig. 7-5 will also apply <strong>to</strong> this<br />

circuit. One of the advantages of this circuit design is that additional<br />

transis<strong>to</strong>r stages can be added on for a longer sequential flashing string.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!