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CHAPTER 8 THE IMPEDANCE MODEL AND NETWORK CALCULATIONS
of the adm;ttance directly connected between buses
and
@
, as we would
expect since mutually coupled branches are absent.
We have made this detailed examination of the bus admittances in order
to dierentiate them clearly from the impedances of the bus impedance matrix.
Conceptually, we solve Eq. (8.3) by premultiplying both sides of the
e
quatio
n
by
YI� =
Z
hus
to yield
(B.B)
and
we must remember when dealing with
Z
hus
that V and I are column vectors
of the bus voltages and the currents entering the buses from current sources,
respectively. Expanding Eq. (8.8) for a network of three in
d
ependent nodes
yields
(
8.9)
(8.10)
(8.11)
From Eq. (8.10) we see that the driving-point impedance 22
2
is deter
mined by open-circuiting the current sources at buses
and and by
injecting the source current
12
at bus
W
. Then,
V
2
222
=
--
12
(8.12)
Figure 8.2 shows the circuit described. Since 2
2
2 IS dened by openmg the
+
®