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680 ⏐⏐⏐ SERIES AND PARALLEL ac CIRCUITS<br />

+<br />

e<br />

–<br />

R<br />

L<br />

+<br />

vL –<br />

Oscilloscope<br />

FIG. 15.97<br />

Determining the phase relationship between e and v L.<br />

θ<br />

1.6 div.<br />

e<br />

T = 8 div.<br />

FIG. 15.98<br />

Determining the phase angle between e and v L.<br />

For the chosen horizontal sensitivity, each waveform of Fig. 15.98<br />

has a period T defined by eight horizontal divisions, and the phase angle<br />

between the two waveforms is defined by 1 �1<br />

2 � divisions. Using the fact<br />

that each period of a sinusoidal waveform encompasses 360°, the following<br />

ratios can be set up to determine the phase angle v:<br />

v<br />

� 8 div.<br />

� � �<br />

360°<br />

1.6 div.<br />

�<br />

v<br />

and v � � � 360° � 72°<br />

In general,<br />

1.6<br />

�<br />

8<br />

( div.<br />

for<br />

v)<br />

v � � � � 360°<br />

( div.<br />

for<br />

T)<br />

1<br />

2<br />

a c<br />

(15.43)<br />

If the phase relationship between e and v R is required, the oscilloscope<br />

must not be hooked up as shown in Fig. 15.99. Points a and b<br />

have a common ground that will establish a zero-volt drop between the<br />

two points; this drop will have the same effect as a short-circuit connection<br />

between a and b. The resulting short circuit will “short out” the<br />

inductive element, and the current will increase due to the drop in<br />

impedance for the circuit. A dangerous situation can arise if the inductive<br />

element has a high impedance and the resistor has a relatively low

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