Capacitores

6.1 INTRODUCTION

So far we have limited our study to resistive circuits. In this chapter, we

shall introduce two new and important passive linear circuit elements:

the capacitor and the inductor. Unlike resistors, which dissipate energy,

capacitors and inductors do not dissipate but store energy, which can be

retrieved at a later time. For this reason, capacitors and inductors are

In contrast to a resistor, which spends or dis- called storage elements.

sipates energy irreversibly, an inductor or capacitor

stores or releases energy (i.e., has a

memory).

The application of resistive circuits is quite limited. With the introduction

of capacitors and inductors in this chapter, we will be able to

analyze more important and practical circuits. Be assured that the circuit

analysis techniques covered in Chapters 3 and 4 are equally applicable to

circuits with capacitors and inductors.

We begin by introducing capacitors and describing how to combine

them in series or in parallel. Later, we do the same for inductors. As

typical applications, we explore how capacitors are combined with op

amps to form integrators, differentiators, and analog computers.

6.2 CAPACITORS

A capacitor is a passive element designed to store energy in its electric

field. Besides resistors, capacitors are the most common electrical components.

Capacitors are used extensively in electronics, communications,

computers, and power systems. For example, they are used in the tuning

circuits of radio receivers and as dynamic memory elements in computer

systems.

A capacitor is typically constructed as depicted in Fig. 6.1.

Metal plates,

each with area A

d

Dielectric with permittivity e

Figure 6.1 A typical capacitor.

A capacitor consists of two conducting plates separated

by an insulator (or dielectric).

In many practical applications, the plates may be aluminum foil while the

dielectric may be air, ceramic, paper, or mica.

When a voltage source v is connected to the capacitor, as in Fig.

6.2, the source deposits a positive charge q on one plate and a negative

charge −q on the other. The capacitor is said to store the electric charge.

The amount of charge stored, represented by q, is directly proportional

to the applied voltage v so that

q = Cv (6.1)

where C, the constant of proportionality, is known as the capacitance

of the capacitor. The unit of capacitance is the farad (F), in honor of

the English physicist Michael Faraday (1791–1867). From Eq. (6.1), we

Alternatively, capacitance is the amount of charge may derive the following definition.

storedper plate for a unit voltage difference in a

capacitor.

−

−

−

+q −q

+

+

+

+

+

+

+ −

v

Figure 6.2 A capacitor

with applied voltage v.

Capacitance is the ratio of the charge on one plate of a capacitor to the voltage

difference between the two plates, measured in farads (F).

Note from Eq. (6.1) that 1 farad = 1 coulomb/volt.

CHAPTER 6 Capacitors andInd uctors 203

Although the capacitance C of a capacitor is the ratio of the charge

q per plate to the applied voltage v, it does not depend on q or v. It

depends on the physical dimensions of the capacitor. For example, for

the parallel-plate capacitor shown in Fig. 6.1, the capacitance is given by

C = A

d

(6.2)

where A is the surface area of each plate, d is the distance between the

plates, and  is the permittivity of the dielectric material between the

plates. Although Eq. (6.2) applies to only parallel-plate capacitors, we

may infer from it that, in general, three factors determine the value of the

capacitance:

Capacitor voltage rating andca pacitance are typically

inversely ratedd ue to the relationships in

Eqs. (6.1) and(6.2). Arcing occurs if d is small

and V is high.

1. The surface area of the plates—the larger the area, the greater

the capacitance.

2. The spacing between the plates—the smaller the spacing, the

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