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528 ⏐⏐⏐ SINUSOIDAL ALTERNATING WAVEFORMS<br />

i<br />

t<br />

Sine wave<br />

R, L, or C<br />

FIG. 13.11<br />

The sine wave is the only alternating<br />

waveform whose shape is not altered by the<br />

response characteristics of a pure resistor,<br />

inductor, or capacitor.<br />

E m<br />

0° 90° 180° 270° 360°<br />

Cosine wave<br />

E m<br />

0° 90° 180° 270° 360°<br />

FIG. 13.12<br />

Sine wave and cosine wave with the<br />

horizontal axis in degrees.<br />

57.296°<br />

r<br />

v<br />

+<br />

–<br />

r<br />

FIG. 13.13<br />

Defining the radian.<br />

1 radian<br />

t<br />

α<br />

α<br />

The need for defining polarities and current direction will become quite<br />

obvious when we consider multisource ac networks. Note in the last<br />

sentence the absence of the term sinusoidal before the phrase ac networks.<br />

This phrase will be used to an increasing degree as we progress;<br />

sinusoidal is to be understood unless otherwise indicated.<br />

13.3 THE SINE WAVE<br />

The terms defined in the previous section can be applied to any type of<br />

periodic waveform, whether smooth or discontinuous. The sinusoidal<br />

waveform is of particular importance, however, since it lends itself<br />

readily to the mathematics and the physical phenomena associated with<br />

electric circuits. Consider the power of the following statement:<br />

The sinusoidal waveform is the only alternating waveform whose<br />

shape is unaffected by the response characteristics of R, L, and C<br />

elements.<br />

In other words, if the voltage across (or current through) a resistor,<br />

coil, or capacitor is sinusoidal in nature, the resulting current (or voltage,<br />

respectively) for each will also have sinusoidal characteristics, as<br />

shown in Fig. 13.11. If a square wave or a triangular wave were<br />

applied, such would not be the case.<br />

The unit of measurement for the horizontal axis of Fig. 13.12 is the<br />

degree. A second unit of measurement frequently used is the radian<br />

(rad). It is defined by a quadrant of a circle such as in Fig. 13.13 where<br />

the distance subtended on the circumference equals the radius of the<br />

circle.<br />

If we define x as the number of intervals of r (the radius) around the<br />

circumference of the circle, then<br />

and we find<br />

π radians<br />

(3.14 radians)<br />

C � 2pr � x ⋅ r<br />

x � 2p<br />

Therefore, there are 2p rad around a 360° circle, as shown in Fig.<br />

13.14, and<br />

2p rad � 360°<br />

3<br />

2<br />

1 radian<br />

4<br />

5 6<br />

0.28<br />

2π π radians<br />

(6.28 radians)<br />

FIG. 13.14<br />

There are 2p radians in one full circle of 360°.<br />

(13.4)

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