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C h a p t e r 3 : A n t e n n a B a s i c s 83<br />

area.) Similarly, the application of a constant voltage across the resistor terminals<br />

will result in a steady current flow through the resistor until the voltage is<br />

removed. The power dissipated in a resistor is given by<br />

2<br />

P V I P V 2<br />

= × or, alternatively, = or P = I × R<br />

(3.2)<br />

R<br />

Note that all three forms of Eq. (3.2) are equivalent and lead to the same answer.<br />

The resistance of an ideal resistor (i.e., one with no capacitance or inductance)<br />

does not depend on frequency.<br />

• Capacitors. A capacitor is a two-terminal component capable of storing electrical<br />

energy in the form of stored electric charges. The fundamental unit of capacitance<br />

is the farad, and the Capacitor total energy stored in a capacitor is ½ CV 2 , where C is the<br />

capacitance of the specific capacitor in question, and V is the voltage (in volts)<br />

across its terminals. Another useful relationship for capacitors is<br />

= × ∆ V<br />

I C<br />

∆t<br />

(3.3)<br />

where I (in amperes) is the current through a capacitor of value C when the<br />

voltage across the capacitor terminals changes by some amount DV (in volts)<br />

over a short time interval Dt (in seconds). A simple capacitor you can make at<br />

home consists of two identical sheets of aluminum foil insulated from each<br />

other by a sheet of waxed paper of the same size.<br />

Note The only time current flows on the leads of a capacitor is when the voltage across its<br />

terminals is changing: I = C DV/Dt.<br />

A capacitor is said to exhibit capacitive reactance. Reactance works much like<br />

resistance to impede the flow of current in a circuit but the two are very different:<br />

44<br />

The reactance of an ideal capacitor does not dissipate any power.<br />

44<br />

The reactance of a capacitor is frequency dependent.<br />

The magnitude of capacitive reactance is defined in Eq. (3.4):<br />

1<br />

X = − (3.4)<br />

C<br />

2 π fC<br />

where f is the frequency in hertz and C is the capacitance in farads. Alternatively,<br />

f can be in megahertz (MHz) and C in microfarads (µF). The minus sign is<br />

important in distinguishing the effect of capacitors from that of inductors.<br />

• Inductors. An inductor is a two-terminal component capable of storing magnetic<br />

energy in the form of current, or moving electric charges. The fundamental unit<br />

of inductance is Inductor the henry (abbreviated H), and the total energy stored in an<br />

inductor is ½ LI 2 , where L is the inductance of the device in question and I is<br />

the current (in amperes) going through it. Another useful relationship for<br />

inductors is

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