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Impedance parameters
1.
I
P M A P E I1 I2 A z11 z12 M D + Input Output + V1 _ Port z 21 z 22 Port V2 _ E A T E C E S Copyright © 2012 Ahmad Nauman. All Rights Reserved
2.
A two-port network
may be voltage-driven as I1 I2 V1 Linear V2 Network or current-driven as + + I1 V1 Linear I2 _ V2 Network _ Copyright © 2012 Ahmad Nauman. All Rights Reserved
3.
From previous Figures
V1 z11I1 z12 I 2 (a) V2 z 21I1 z 22 I 2 Only two of the four variables (V1, V2, I1 and I2) are independent/known. The other two can be found using equation (a) And in matrix form as V1 z11 z12 I1 V V2 z 21 z 22 I2 Copyright © 2012 Ahmad Nauman. All Rights Reserved
4.
or
V1 I1 z V2 I2 Where z terms are called impedance parameters or simply z-parameters z11 z12 z z 21 z 22 Copyright © 2012 Ahmad Nauman. All Rights Reserved
5.
I1
I2=0 + V1 Linear V2 Network _ The values of the parameters can be evaluated by setting I2 = 0 (output port open-circuited). V1 V2 z11 z 21 I1 I2 0 I1 I2 0 Copyright © 2012 Ahmad Nauman. All Rights Reserved
6.
I1=0
I2 + V1 Linear V2 _ Network The values of the parameters can be evaluated by setting I1 = 0 (output port open-circuited). V1 V2 z12 z 22 I2 I1 0 I2 I1 0 Copyright © 2012 Ahmad Nauman. All Rights Reserved
7.
z11
Open - circuit input impedance. z12 Open Circuit Transfer impedance from port 1 to port 2. z 21 Open Circuit Transfer impedance from port 2 to port 1. z 22 Open - circuit output impedance. Copyright © 2012 Ahmad Nauman. All Rights Reserved
8.
• Since the
z-parameters are obtained by open- circuiting the input or output port, they are also called the open-circuit impedance parameters. • Since they are obtained as a ratio of voltage and current. • And the parameters are obtained by open- circuiting port 2 ( I2 = 0) or port1 ( I1 = 0). • Units of z-parameter are in ohms’ (Ω) Copyright © 2012 Ahmad Nauman. All Rights Reserved
9.
Impedance parameters are
commonly used; • In the synthesis of filter. • They are also useful in the design and analysis of impedance-matching networks. • And power distribution networks. Copyright © 2012 Ahmad Nauman. All Rights Reserved
10.
I1
z1 z2 I2 + + z3 V1 V2 _ _ General form is V1 z11 z12 I1 V2 z 21 z 22 I2 Copyright © 2012 Ahmad Nauman. All Rights Reserved
11.
z1
z2 + + I1 z3 I2 V2 V1 _ _ Find the z-parameters. Copyright © 2012 Ahmad Nauman. All Rights Reserved
12.
z1
+ V1 I1 z3 I2 _ Applying KVL in loop 1 V1 z1I1 z 3 (I1 I2 ) (z 1 z 3 )I1 z 3I 2 But we also know that V1 z11I1 z12 I 2 Copyright © 2012 Ahmad Nauman. All Rights Reserved
13.
z2
+ I1 z3 I2 V2 _ Applying KVL in loop 2 V2 z2I2 z 3 (I1 I2 ) (z 3 )I1 (z 2 z 3 )I 2 But we also know that V2 z 21I1 z 22 I 2
14.
I1
z1 z2 I2 + + z3 V1 V2 _ _ V1 z1 z 3 z3 I1 V2 z3 z 2 z3 I2 And the z-parameters are z1 z 3 z3 z z3 z 2 z3 Copyright © 2012 Ahmad Nauman. All Rights Reserved
15.
20
50 + + V1 25 V2 _ _ Figure 17.19 (a) Find the z-parameters. Copyright © 2012 Ahmad Nauman. All Rights Reserved
16.
20
50 + + V1 25 V2 _ _ Solution: As we know that z-parameters in T Network are z1 z 3 z3 z z3 z 2 z3 So from above figure 20 25 25 z 25 50 25 Copyright © 2012 Ahmad Nauman. All Rights Reserved
17.
20
50 + + V1 25 V2 _ _ Solution: 45 25 z 25 75 Copyright © 2012 Ahmad Nauman. All Rights Reserved
18.
If each two-port
has common reference node for its input and output, and if the references are connected together as indicated in Figure. I1=I1A I2=I2A + + + V1A _ Network A _ V2A + V1 I1 I2 V2 _ V1B + Network B + V2B _ _ _ I1=I1B I2=I2B Copyright © 2012 Ahmad Nauman. All Rights Reserved
19.
I1 flows through
the input ports of the two networks in series. A similar statement holds for I2. Thus, ports remain ports after the interconnection. It follows that I = IA = IB. And V VA VB zA IA z BIB So (z A z B )I zI Where z zA zB Copyright © 2012 Ahmad Nauman. All Rights Reserved
20.
Zg
Z out I2 + V1 V2 _ From this circuit Vs V1 I1Z g (a) Copyright © 2012 Ahmad Nauman. All Rights Reserved
21.
z in
As we know that V1 z11 I1 z12 I 2 From eq. (a) Vs z11I1 z12 I 2 I1Z g Vs (z 11 Z g )I1 z12 I 2 Vs z12 I 2 I1 (b) (z 11 Z g ) (z 11 Z g ) zout We also know that V2 z 21I1 z 22 I 2 (c) Copyright © 2012 Ahmad Nauman. All Rights Reserved
22.
z 21Vs
z12 z 21I 2 V2 z 22 I 2 (z 11 Z g ) (z 11 Z g ) z 21 z12 z 21 V2 Vs z 22 I2 (z11 Z g ) (z11 Z g ) Thus output impedance in terms of z-parameters z12 z 21 Z out z 22 - (z 11 Z g ) Copyright © 2012 Ahmad Nauman. All Rights Reserved
23.
Z out
I2 z21 zth + z11 z g Vs V2 z12z 21 _ Zout z22 z11 z g If the generator impedance z 0 is zero, the simpler expression g z12z 21 Zout z22 z11 z11z 22 z12z 21 z z11 11 Copyright © 2012 Ahmad Nauman. All Rights Reserved
24.
20
50 + + 25 I1 I2 V1 V2 0.5V2 _ _ Figure 17.19 (c) Copyright © 2012 Ahmad Nauman. All Rights Reserved
25.
20
+ 25 I1 I2 V1 0.5V2 _ Solution: Applying KVL in loop 1 V1 20I1 25 (I1 I 2 ) 0.5V2 V1 45I1 25I2 0.5V2 (a) Copyright © 2012 Ahmad Nauman. All Rights Reserved
26.
50
+ 25 I1 I2 V2 0.5V2 _ Solution: Applying KVL in loop 2 V2 50I2 25 (I1 I 2 ) 0.5V2 V2 0.5V2 25I1 75I2 V2 50I1 150I2 (b) Copyright © 2012 Ahmad Nauman. All Rights Reserved
27.
Solution:
Substituting equation (b) into (a), we get; V1 45I1 25I2 0.5(50I1 150I 2 ) V1 (45 25)I1 (25 75)I 2 V1 70I1 100I 2 (c) As we know that V1 z11 z12 I1 V2 z 21 z 22 I2 From equation (c) and (b), we get; V1 70 100 I1 V2 50 150 I 2 Copyright © 2012 Ahmad Nauman. All Rights Reserved
28.
Solution:
We know z-parameters are z11 z12 z z 21 z 22 So [z] will be 70 100 z 50 150 Copyright © 2012 Ahmad Nauman. All Rights Reserved
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