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Solution 19.86
(a) By definition, g11 =
, g21 =
.
We let V1 = 1 V and open-circuit the output port. The schematic is shown below. After
simulation, we obtain
g11 = I1 = 2.7
(b) Similarly,
g12 =
, g22 =
We let I2 = 1 A and short-circuit the input port. The schematic is shown below. After
simulation,
Solution 19.87
(a) Since a =
and c =
,
we open–circuit the input port and let V2 = 1 V. The schematic is shown below. In the
AC Sweep box, set Total Pts = 1, Start Freq = 0.1592, and End Freq = 0.1592. After
simulation, we obtain an output file which includes
From this,
(b) Similarly,
b =
and d =
We short-circuit the input port and let V2 = 1 V. The schematic is shown below. After
simulation, we obtain an output file which includes
From this, we get
Solution 19.88
To get
, consider the network in Fig. (a).
But
222121
L
2
2
R
–VyVy
V
I+==
Substituting (3) into (1) yields
+
⋅+=
L22
121
121111 R1
–
y
Vy
yVyI
,
or
From (3),
To get
, consider the circuit in Fig. (b).
Substituting this into (1) yields
Substituting this into (4) gives
Solution 19.89
Lfereoeieie
Lfe
vR)hhhh(h
Rh–
A−+
=
Solution 19.90
(a)
Loe
Lfere
iein Rh1
Rhh
hZ +
−=
(b)
Lfereoeieie
Lfe
vR)hhhh(h
Rh–
A−+
=
Solution 19.91
,
(a)
Lfereoeieie
Lfe
t
R)hhhh(h
Rh–
A−+
=
Solution 19.92
Due to the resistor
, we cannot use the formulas in section 18.9.1. We will
need to derive our own. Consider the circuit in Fig. (a).
(1)
Substituting (4) into (3),
c
oe
E
L
bfec
h
1
R
R
hIII +
−=
From (3) and (5),
Substituting (4) and (6) into (2),
EccrebEiebRh)Rh( IVIV +++=
From (5),
We substitute this with (4) into (2) to get
To obtain out
, which is the same as the Thevenin impedance at the output, we introduce
a 1-V source as shown in Fig. (b).
From the input loop,
From the output loop,
Substituting (10) into (9) gives
out
re
oeE
ieEs
feoe
h
hR1
hRR
)hh(
−
+
++