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.