3.4 FREQUENCY RESPONSE 165They-parameter equivalent circuit that satisfies these equations is shown in Figure E3.4.3(a).
V 1 V 2−y 12y 11 + y 12 y 22 + y 12 (y 21 − y 12 )V 1I 1 I 211 ′
(a)
22 ′+−+−Figure E3.4.3(a)y-para-
meter equivalent circuit.
(b)z-parameter equivalent
circuit.(c)h-parameter
equivalent circuit.V 1 z 12 V 2z 11 − z 12 z 22 − z 12
(z 21 − z 12 )I 1I 1 I 211 ′
(b)
22 ′+
− +−+−V 1 h 12 V 2 h 21 I 1 h 22 V 2I 1 h 11 I 211 ′
(c)
22 ′+
+−
−+−Equations (3.4.13) and (3.4.14) can be arranged as
V 1 =(z 11 −z 12 )I 1 +z 12 (I 1 +I 2 )V 2 =(z 21 −z 12 )I 1 +(z 22 −z 12 )I 2 +z 12 (I 1 +I 2 )Thez-parameter equivalent circuit that satisfies these equations is shown in Figure E3.4.3(b).
Theh-parameter equivalent circuit satisfying Equations (3.4.15) and (3.4.16) is shown in Figure
E3.4.3(c).
Equations (3.4.11) and (3.4.12) can be solved simultaneously to yield
V 1 =y 22
y 11 y 22 −y 12 y 21I 1 +−y 12
y 11 y 22 −y 12 y 21I 2V 2 =−y 21
y 11 y 22 −y 12 y 21I 1 +y 11
y 11 y 22 −y 12 y 21I 2By comparing these with Equations (3.4.13) and (3.4.14), one gets
z 11 =y 22
y 11 y 22 −y 12 y 21; z 12 =−y 12
y 11 y 22 −y 12 y 21z 21 =−y 21
y 11 y 22 −y 12 y 21; z 22 =y 11
y 11 y 22 −y 12 y 21