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Alternating Current Analysis 247


and

 2 2


2
2

1


2


1


2


1


2


114


R   


RC RC C R R


C


L















 


The BW is then given by

BW


RC Q


R
P

  








21

1


2


^1









R.3.54 A parallel RLC circuit presents the following characteristics at resonance:
a. ZT is at a maximum.
b. ZT = R, since the angle between I and V is zero.
c. Current is at a minimum.
d. The effective power is at its minimum.
R.3.55 Practical resonant circuits are constructed by placing a capacitor and an inductor
in parallel as shown in Figure 3.20, where R 1 and R 2 are the internal resistances
of L and C, respectively. Recall that the condition at resonance is that the complex
admittance Y is a real number, then

X
RX

X


RX


C
C

L
2 L

2 2
1

 ^22 


and the resonant frequency is given by

R


LC


RLC


RLC











1 12


2

2

()


()


Since ωR is real, R^21 > L/C and R^22 > L/C.
R.3.56 Recall that the process used in the mesh or loop equations techniques was presented
and discussed in Chapter 2, for the purely resistive DC case. The theory developed

L C

R 1 R 2

Y

FIGURE 3.20
Network of R.3.55.
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