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IN DC CIRCUITS, RESISTANCE IS A SIMPLE THING. IT CAN BE EXPRESSED AS A number, from zero (a perfect conductor) to extremely large values, increasing without limit through the millions, billions, and even trillions of ohms. Physicists call resistance a scalar quantity, because it can be expressed on a one-dimensional scale. In fact, dc resistance can be represented along a half line, or ray, as shown in Fig. 13-1.

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Given a certain dc voltage, the current decreases as the resistance increases, in accordance with Ohm s Law, as you already know. The same law holds for ac through a resistance, if the ac voltage and current are both specified as peak, pk-pk, or rms values.

Inductive reactance can be plotted along a half line, just as can resistance. In a circuit containing both resistance and inductance, the characteristics become two-dimensional. You can orient the resistance and reactance half lines perpendicular to each other to make a quarter-plane coordinate system, as shown in Fig. 13-5. Resistance is plotted horizontally, and inductive reactance is plotted vertically upward.

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Suppose that you have some wire that conducts electricity very well. What will happen if you wind a length of the wire into a coil and connect it to a source of dc, as shown in Fig. 13-2 The wire will draw a large amount of current, possibly blowing a fuse or overstressing a battery. It won t matter whether the wire is a single-turn loop, or whether it s lying haphazardly on the floor, or whether it s wrapped around a stick. The current will be large. In amperes, it will be equal to I E/R, where I is the current, E is the dc voltage, and R is the resistance of the wire (a low resistance).

inductive reactance (XL ) and resistance (R). This is also known as the RL quarter-plane, or simply as the RL plane.

You can make an electromagnet, as you ve already seen, by passing dc through a coil wound around an iron rod. But there will still be a large, constant current in the coil. The coil will probably get more or less hot, as energy is dissipated in the resistance of the wire. The battery, too, or power supply components, will become warm or hot. If the voltage of the battery or power supply is increased, the wire in the coil, iron core or not, will get hotter. Ultimately, if the supply can deliver the necessary current, the wire will melt.

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In this scheme, resistance-inductance (RL) combinations form complex impedances (The term impedance comes from the root impede, and fully describes how electrical components impede, or inhibit, the flow of ac You ll learn all about this in Chap 15) Each point on the RL plane corresponds to one unique complex impedance value Conversely, each complex impedance value corresponds to one unique point on the RL plane You might ask, What s the little j doing in Fig 13-5 For reasons that will be made clear in Chap 15, impedances on the RL plane are written in the form R + jXL, where R is the resistance in ohms, and XL is the inductive reactance in ohms The little j is called a j operator and is a mathematical way of expressing the fact that reactance is denoted at right angles to resistance in compleximpedance graphs.

Suppose you change the voltage source, connected across the coil, from dc to ac (Fig. 13-3). Imagine that you can vary the frequency of the ac, from a few hertz to hundreds of hertz, then kilohertz, then megahertz.

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