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32 CHAPTER ONE the circuit abstraction<br />

i<br />

0<br />

Slope =<br />

v<br />

1<br />

---<br />

R<br />

FIGURE 1.28 Plot <strong>of</strong> the v–i<br />

relationship for a resistor.<br />

i<br />

0<br />

+<br />

V<br />

-<br />

(a)<br />

i<br />

(b)<br />

FIGURE 1.29 (a) Independent<br />

voltage source with assigned<br />

terminal variables, (b) v–i relationship<br />

for the voltage source.<br />

+<br />

v<br />

-<br />

V<br />

v<br />

Most <strong>of</strong>ten, resistances <strong>and</strong> conductances are thought <strong>of</strong> as time-invariant<br />

parameters. But if the temperature <strong>of</strong> a resistor changes, then so too can<br />

its resistance <strong>and</strong> conductance. Thus, a linear resistor can be a time-varying<br />

element.<br />

1.6.2 ELEMENT LAWS<br />

From the viewpoint <strong>of</strong> circuit analysis, the most important characteristic <strong>of</strong> a<br />

two-terminal element is the relation between the voltage across <strong>and</strong> the current<br />

through its terminals, or the v i relationship for short. This relation, called<br />

the element law, represents the lumped-parameter summary <strong>of</strong> the electronic<br />

behavior <strong>of</strong> the element. for example, as seen in Equation 1.15,<br />

v = iR<br />

is the element law for the resistor. The element law is also referred to as the<br />

constituent relation, or the element relation. In order to st<strong>and</strong>ardize the manner<br />

in which element laws are expressed, the current <strong>and</strong> voltage for all two-terminal<br />

elements are defined according to the associated variables convention shown in<br />

Figure 1.19. Figure 1.28 shows a plot <strong>of</strong> the v i relationship for a resistor when<br />

v <strong>and</strong> i are defined according to the associated variables convention.<br />

The constituent relation for the independent voltage source in Figure 1.26b<br />

supplying a voltage V is given by<br />

v = V (1.18)<br />

when its terminal variables are defined as in Figure 1.29a. A plot <strong>of</strong> the v i<br />

relationship is shown in Figure 1.29b. Observe the clear distinction between<br />

the element parameter V <strong>and</strong> its terminal variables v <strong>and</strong> i.<br />

Similarly, the element law for the ideal wire (or a short circuit) is given by<br />

v = 0. (1.19)<br />

Figure 1.30a shows the assignment <strong>of</strong> terminal variables <strong>and</strong> Figure 1.30b<br />

plots the v i relationship.<br />

Finally, the element law for an open circuit is given by<br />

i = 0. (1.20)<br />

Figure 1.31a shows the assignment <strong>of</strong> terminal variables <strong>and</strong> Figure 1.31b<br />

plots the v − i relationship.<br />

Comparing the v i relationship for the resistor in Figure 1.28 to those for a<br />

short circuit in Figure 1.30 <strong>and</strong> an open circuit in Figure 1.31, it is evident that<br />

the short circuit <strong>and</strong> open circuit are limiting cases for a resistor. The resistor<br />

approaches the short circuit case as its resistance approaches zero. The resistor<br />

approaches the open circuit case as its resistance approaches infinity.

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