1. NETWORK FILTERS
AND
TRANSMISSION LINE

2. TWO PORT NETWORKS

3. SUB - TOPICS Z – PARAMETER Y – PARAMETER T (ABCD) – PARAMETER
TERMINATED TWO PORT NETWORKS

4. OBJECTIVES TO UNDERSTAND ABOUT TWO – PORT NETWORKS AND ITS FUNTIONS.
TO UNDERSTAND THE DIFFERENT BETWEEN Z – PARAMETER, Y – PARAMETER, T – PARAMETER AND TERMINATED TWO PORT NETWORKS.
TO INVERTIGATE AND ANALYSIS THE BEHAVIOUR OF TWO – PORT NETWORKS.

5. TWO – PORT NETWORKS
A pair of terminals through which a current may enter or leave a network is known as a port.
Two terminal devices or elements (such as resistors, capacitors, and inductors) results in one – port network.
Most of the circuits we have dealt with so far are two – terminal or one – port circuits.

6. A two – port network is an electrical network with two separate ports for input and output.
It has two terminal pairs acting as access points. The current entering one terminal of a pair leaves the other terminal in the pair.

7. One – port network Two – port network I + V Linear network - I1 + V2

8. Two (2) reason why to study two port – network:
Such networks are useful in communication, control system, power systems and electronics.
Knowing the parameters of a two – port network enables us to treat it as a “black box” when embedded within a larger network.

9. From the network, we can observe that there are 4 variables that is I1, I2, V1and V2, which two are independent.
The various term that relate these voltages and currents are called parameters.

10. Z – PARAMETER
Z – parameter also called as impedance parameter and the units is ohm (Ω)
Impedance parameters is commonly used in the synthesis of filters and also useful in the design and analysis of impedance matching networks and power distribution networks.
The two – port network may be voltage – driven or current – driven.

11. Two – port network driven by voltage source.
Two – port network driven by current sources.
Linear network I1 I2 +  V1 V2 I1 I2 + V1 -
Linear network V2

12. The “black box” is replace with Z-parameter is as shown below.
The terminal voltage can be related to the terminal current as: + V1 - I1 I2 V2
Z11
Z21
Z12
Z22
(1)
(2)

13. In matrix form as:
The Z-parameter that we want to determine are z11, z12, z21, z22.
The value of the parameters can be evaluated by setting:
1. I1= 0 (input port open – circuited)
2. I2= 0 (output port open – circuited)

14. Thus,

15. Where;
z11 = open – circuit input impedance.
z12 = open – circuit transfer impedance from port 1 to port 2.
z21 = open – circuit transfer impedance from port 2 to port 1.
z22 = open – circuit output impedance.

16. Example 1 Find the Z – parameter of the circuit below. 40Ω 240Ω 120Ω +V1 _ V2 I1 I2

17. Solution I2 = 0(open circuit port 2). Redraw the circuit. 40Ω 240Ω
120Ω + V1 _ V2 I1 Ia Ib

19. ii) I1 = 0 (open circuit port 1). Redraw the circuit.
40Ω
240Ω
120Ω + V1 _ V2 Iy I2 Ix

20. In matrix form:

21. Example 2 Find the Z – parameter of the circuit below + _ V1 V2 -j20Ω
10Ω
j4Ω 2Ω
10I2 I2 I1

22. Solution i) I2 = 0 (open circuit port 2). Redraw the circuit. + V1 _
j4Ω 2Ω I1 V2
I2 = 0

23. ii) I1 = 0 (open circuit port 1). Redraw the circuit.+ _ V1 V2
-j20Ω
10Ω
10I2 I2
I1 = 0

24. Y - PARAMETER
Y – parameter also called admittance parameter and the units is siemens (S).
The “black box” that we want to replace with the Y-parameter is shown below. + V1 - I1 I2 V2
Y11
Y21
Y12
Y22

25. The terminal current can be expressed in term of terminal voltage as:
In matrix form:
(1)
(2)

26. The y-parameter that we want to determine are Y11, Y12, Y21, Y22
The y-parameter that we want to determine are Y11, Y12, Y21, Y22. The values of the parameters can be evaluate by setting:
i) V1 = 0 (input port short – circuited).
ii) V2 = 0 (output port short – circuited).
Thus;

27. Example 1 Find the Y – parameter of the circuit shown below. 5Ω 15Ω
20Ω + V1 _ V2 I1 I2

28. Solution
V2 = 0 5Ω
20Ω + V1 _ I1 I2 Ia

29. ii) V1 = 0
In matrix form; 5Ω
15Ω + V2 _ I1 I2 Ix

30. Example 2 (circuit with dependent source)
Find the Y – parameters of the circuit
shown. + _ V1 V2
-j20Ω
10Ω
j4Ω 2Ω
10I2 I2 I1

31. Solution i) V2 = 0 (short – circuit port 2). Redraw the circuit. + _
10Ω
j4Ω 2Ω
10I2 I2 I1

32. ii) V1 = 0 (short – circuit port 1). Redraw the circuit.+ _ V2
-j20Ω
10Ω
j4Ω 2Ω
10I2 I2 I1

33. T (ABCD) PARAMETER
T – parameter or ABCD – parameter is a another set of parameters relates the variables at the input port to those at the output port.
T – parameter also called transmission parameters because this parameter are useful in the analysis of transmission lines because they express sending – end variables (V1 and I1) in terms of the receiving – end variables (V2 and -I2).

34. The “black box” that we want to replace with T – parameter is as shown below.
The equation is: + V1 - I1 I2 V2
A11
C21
B12
D22

35. In matrix form is:
The T – parameter that we want determine are A, B, C and D where A and D are dimensionless, B is in ohm (Ω) and C is in siemens (S).
The values can be evaluated by setting
i) I2 = 0 (input port open – circuit)
ii) V2 = 0 (output port short circuit)

36. Thus;
In term of the transmission parameter, a network is reciprocal if;

37. Example Find the ABCD – parameter of the circuit shown below. 2Ω 10Ω +V2 _ I1 I2 V1 4Ω

38. Solution
i) I2 = 0, 2Ω
10Ω + V2 _ I1 V1

39. ii) V2 = 0, 2Ω
10Ω I1 I2 + V1 _ 4Ω
I1 + I2

40. TERMINATED TWO – PORT NETWORKS
In typical application of two port network, the circuit is driven at port 1 and loaded at port 2.
Figure below shows the typical terminated 2 port model. + V1 - I1 I2 V2  Zg ZL Vg
Two – port network

41. Zg represents the internal impedance of the source and Vg is the internal voltage of the source and ZL is the load impedance.
There are a few characteristics of the terminated two-port network and some of them are;

42. The derivation of any one of the desired expression involves the algebraic manipulation of the two – port equation. The equation are:
1) the two-port parameter equation either Z or Y or ABCD.
For example, Z-parameter,

43. 2) KVL at input,
3) KVL at the output,
From these equations, all the characteristic can be obtained.

44. ATTENUATORS

45. Attenuators are simple but very important instruments
Attenuators are simple but very important instruments. Unlike an amplifier, which is ordinarily used to increase a signal level by a given amount, the attenuator is used to reduce the signal level by a given amount

46. The use of attenuators has become so widespread that a study of their design and use is important in the study of electronic instruments. Attenuators may be constructed in many ways. We will confine our discussion to lumped-resistance attenuators.

47. The L-type Attenuator
One of the simplest types of attenuators is the L type or the ordinary voltage divider. The voltage gain of this network is the out­put voltage divided by the input voltage.

48. The Characteristic Resistance of Symmetrical Attenuators
Usually, the term attenuator refers to a device that not only introduces a precise amount of attenuation but also provides an impedance match on the input and output terminals.