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Z i, from which the resistive and reactive components can be determined<br />

using a few basic geometric relationships. The reactive nature (inductive<br />

or capacitive) of the input impedance can be determined when the<br />

angle between E i and I i is computed. For a dual-trace oscilloscope, if<br />

E g leads V Rs (E i leads I i), the network is inductive; if the reverse is true,<br />

the network is capacitive.<br />

Red<br />

E g<br />

Black<br />

+<br />

––<br />

Black<br />

FIG. 26.7<br />

Determining Z i using an oscilloscope.<br />

To determine the angle associated with Z o, the sensing resistor must<br />

again be moved to the bottom to form a common ground with the supply<br />

E g. Then, using the approximation E g � E o, the magnitude and<br />

angle of Z o can be determined.<br />

EXAMPLE 26.1 Given the DMM measurements appearing in Fig.<br />

26.8, determine the input impedance Zi for the system if the input<br />

impedance is known to be purely resistive.<br />

Solution:<br />

VRs � Eg � Ei � 100 mV � 96 mV � 4 mV<br />

Ii � IRs � � �40 mA<br />

Zi � Ri � � Ei<br />

� � � 9<br />

VRs 4 mV<br />

� �<br />

Rs 100 �<br />

6 mV<br />

� � 2.4 k�<br />

40<br />

mA<br />

I i<br />

R s<br />

I i<br />

Red<br />

I i<br />

+<br />

EXAMPLE 26.2 Using the provided DMM measurements of Fig.<br />

26.9, determine the output impedance Z o for the system if the output<br />

impedance is known to be purely resistive.<br />

E i = 0 V<br />

Two-port<br />

system<br />

+<br />

E i<br />

–<br />

FIG. 26.9<br />

Example 26.2.<br />

Two-port<br />

system<br />

Channel 2: V Rs<br />

Channel 1: E s<br />

Share common<br />

ground<br />

+<br />

Rs 2 k�<br />

+<br />

Eo = 1.92 V Eg 2 V<br />

–<br />

Z o<br />

THE IMPEDANCE PARAMETERS Z i AND Z o ⏐⏐⏐ 1153<br />

–<br />

E g<br />

+<br />

–<br />

R s<br />

100 �<br />

100 mV<br />

+<br />

E i = 96 mV<br />

Z i<br />

–<br />

FIG. 26.8<br />

Example 26.1.<br />

Two-port<br />

system

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