Application of complex numbers to series a.c. circuits 433
Figure 24.8 (a) Circuit
diagram (b) Phasor diagram
(c) Argand diagram
it may be seen that in complex form the supply voltage V is given by:
V
= V
R
Y j.V
L
− V
C
/
From the voltage triangle the impedance triangle is derived and superim-
posing this on the Argand diagram gives, in complex form,
impedance Z
= R Y j.X
L
− X
C
/ or Z = jZj
66
f
where, jZjD
[R
2
C X
L
X
C
2
]and D arctanX
L
X
C
/R
When V
L
D V
C
, X
L
D X
C
and the applied voltage V and the current
I are in phase. This effect is called series resonance and is discussed
separately in Chapter 28.
(g) General series circuit
In an a.c. circuit containing several impedances connected in series, say,
Z
1
,Z
2
,Z
3
,...,Z
n
, then the total equivalent impedance Z
T
is given by
Z
T
= Z
1
Y Z
2
Y Z
3
Y ...Y Z
n
Problem 1. Determine the values of the resistance and the
series-connected inductance or capacitance for each of the
following impedances: (a) 12 C j5 (b) j40 (c) 30
6
60
°
(d) 2.20 ð 10
6
6
30
°
. Assume for each a frequency of 50 Hz.
(a) From Section 24.2(d), for an R –L series circuit, impedance
Z D R C jX
L
.
Thus Z D 12 C j5 represents a resistance of 12 and an induc-
tive reactance of 5 in series.
Since inductive reactance X
L
D 2fL,
inductance L D
X
L
2f
D
5
250
D 0.0159 H
i.e., the inductance is 15.9 mH.
Thus an impedance .12 Y j5/Z represents a resistance of 12 Z
in series with an inductance of 15.9 mH.
(b) From Section 24.2(c), for a purely capacitive circuit, impedance
Z DjX
c
.
Thus Z Dj40 represents zero resistance and a capacitive reac-
tance of 40 .
Since capacitive reactance X
C
D 1/2fC,
capacitance C D
1
2fX
C
D
1
25040
F D
10
6
25040
µF
D 79.6
µF