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An Introduction To Two – Port Networks The University of Tennessee Electrical and Computer Engineering Knoxville, TN wlg
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Page 1: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

An Introduction ToTwo – Port Networks

The University of TennesseeElectrical and Computer Engineering

Knoxville, TNwlg

Page 2: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Generalities: The standard configuration of a two port:

The NetworkInputPort

OutputPort

+

_ _

+V1 V2

I1 I2

The network ?

The voltage and current convention ?

* notes

Presenter
Presentation Notes
The two port network configuration shown with this slide is practically used universally in all text books. The same goes for the voltage and current assumed polarity and direction at the input and output ports. I think this is done because of how we define parameters with respect the voltages and currents at the input and out ports. With respect to the network, it may be configured with passive R, L, C, op-amps, transformers, dependent sources but not independent sources.
Page 3: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Network Equations:

V1 = z11 I1 + z12 I2

V2 = z21 I1 + z22 I2

I1 = y11 V1 + y12 V2

I2 = y21 V1 + y22 V2

V1 = AV2 - BI2

I1 = CV2 - DI2

V2 = b11 V1 - b12 I1

I2 = b21 V1 – b22 I1

V1 = h11 I1 + h12 V2

I2 = h21 I1 + h22 V2

I1 = g11 V1 + g12 I2

V2 = g21 V1 + g22 I2

ImpedanceZ parameters

AdmittanceY parameters

TransmissionA, B, C, D

parameters

HybridH parameters

* notes

Presenter
Presentation Notes
The equations in light orange are the ones we will consider here. The other equations are also presented and consider in Nilsson & Riedel, 6th ed. The parameters are defined in terms of open and short circuit conditions of the two ports. This will be illustrated and some examples presented.
Page 4: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters:

11

11 IV

z =02=I

21

12 IV

z =01=I

12

21 IV

z =02=I

22

22 IV

z =01=I

z11 is the impedance seen looking into port 1when port 2 is open.

z12 is a transfer impedance. It is the ratio of thevoltage at port 1 to the current at port 2 whenport 1 is open.

z21 is a transfer impedance. It is the ratio of the voltage at port 2 to the current at port 1 whenport 2 is open.

z22 is the impedance seen looking into port 2when port 1 is open.

* notes

Page 5: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Y parameters:

11

11 VI

y =02=V

21

12 VI

y =01=V

12

21 VI

y =02=V

22

22 VI

y =01=V

y11 is the admittance seen looking into port 1when port 2 is shorted.

y12 is a transfer admittance. It is the ratio of thecurrent at port 1 to the voltage at port 2 whenport 1 is shorted.

y21 is a transfer impedance. It is the ratio of the current at port 2 to the voltage at port 1 whenport 2 is shorted.

y22 is the admittance seen looking into port 2when port 1 is shorted.

* notes

Presenter
Presentation Notes
Similar to input and output impedance, y11 and y22 are determined by looking into the input and output ports with the opposite ports short circuited. When we look for y12 and y21 we adhere to the above equations with respect to shorting the output terminals. If the circuit is not passive, we need to be careful and do exactly as the equations tell us to do.
Page 6: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters: Example 1

Given the following circuit. Determine the Z parameters.

8

20 20 Ω

ΩΩ

Ω

10

+

_

+

_

V1 V2

I1 I2

Find the Z parameters for the above network.

Page 7: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters: Example 1 (cont 1)

For z11 :

Z11 = 8 + 20||30 = 20 Ω

For z22 :

For z12 :

Z22 = 20||30 = 12 Ω

21

12 IV

z = 01=I

8

20 20 Ω

ΩΩ

Ω

10

+

_

+

_

V1 V2

I1 I2

22

1 83020

2020xI

xxIV =

+=

Therefore:88

2

212 ==

IxIz Ω = 21z

Page 8: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters: Example 1 (cont 2)

The Z parameter equations can be expressed inmatrix form as follows.

⎥⎦

⎤⎢⎣

⎡⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

2

1

128820

II

VV

⎥⎦

⎤⎢⎣

⎡⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

2221

1211

2

1

II

zzzz

VV

Page 9: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters: Example 2 (problem 18.7 Alexander & Sadiku)

You are given the following circuit. Find the Z parameters.

4 Ω

2 Ω

2Vx

+

-Vx

+ +

_ _

V1 V2

I1 I2

Page 10: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Z parameters: Example 2 (continue p2)

11

11 IV

z =02=I

4 Ω

2 Ω

2Vx

+

-Vx

+ +

_ _

V1 V2

I1 I2

626

62

11xxxxxx VVVVVV

I++

=+

+=

23

1xV

I = ; but 11 IVVx −=

Substituting gives;

( )2

3 111

I VI −= or Ω==

35

111

1 zIV

Z21 = -0.667 Ω

Z12 = 0.222 Ω

Z22 = 1.111 Ω

Other Answers

Page 11: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Transmission parameters (A,B,C,D):

The defining equations are:

⎥⎦

⎤⎢⎣

⎡−⎥

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

2

1

1

IV

DCBA

IV

2

1

VVA=

I2 = 0 2

1

IVB−

= V2 = 0

2

1

VI

C =I2 = 0 2

1

IID−

= V2 = 0

Page 12: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Transmission parameters (A,B,C,D):

Example Given the network below with assumed voltage polarities andCurrent directions compatible with the A,B,C,D parameters.

+

_

+

_

R1

R2V1 V2

I1 -I2

We can write the following equations.

V1 = (R1 + R2 )I1 + R2 I2

V2 = R2 I1 + R2 I2

It is not always possible to write 2 equations in terms of the V’s and I’s Of the parameter set.

Page 13: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

1

1R

2

1R

2

21

RRR +

Two Port Networks

Transmission parameters (A,B,C,D):

Example (cont.)

V1 = (R1 + R2 )I1 + R2 I2

V2 = R2 I1 + R2 I2

From these equations we can directly evaluate the A,B,C,D parameters.

2

1

VVA=

I2 = 02

1

IVB−

= V2 = 0

2

1

VI

C =I2 = 0 2

1

IID−

= V2 = 0

=

=

=

=

Later we will see how to interconnect two of these networks together for a final answer* notes

Presenter
Presentation Notes
The answers to the above are underneath the gray boxes. The A,B,C,D parameters are best used when we want to cascade two networks together such as follows
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Two Port Networks

Hybrid Parameters: The equations for the hybrid parameters are:

⎥⎦

⎤⎢⎣

⎡⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

2221

1211

2

1

VI

hhhh

IV

1

111 I

Vh =V2 = 0

2

112 V

Vh =I1 = 0

1

221 I

Ih =V2 = 0 2

222 V

Ih =I1 = 0

* notes

Presenter
Presentation Notes
The H parameters are used almost solely in electronics. These parameters are used in the equivalent circuit Of a transistor. As you will see, the H parameter equations directly set-up so as to describe the device in terms Of the hij parameters which are given by the manufacturer. You will use this material in junior electronics.
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Two Port Networks

Hybrid Parameters: The following is a popular model used to representa particular variety of transistors.

+ +

_ _

V1 V2

+

_

K1

K4K3V1K2V2

I1 I2

We can write the following equations:

DVCII

BVAIV

212

211

+=

+=

* notes

Presenter
Presentation Notes
In this example we consider a very popular model of a transistor. We first assign some identifier, such as K1, K2, K3, K4, to the model. Next we write the equations at the input port and output port. In this case they are extremely simple to write. Then it turns out that we can use these equations to directly identify what will be called the H parameters. Note that one of the parameters is a voltage gain, one is a current gain, one is an resistance and one is a conductance. You will go into a fair amount of detail on this model later in the curriculum
Page 16: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

4

1K

K2

K3

K1

Two Port Networks

Hybrid Parameters:

DVCII

BVAIV

212

211

+=

+=

We want to evaluate the H parameters from the above set of equations.

1

111 I

Vh =V2 = 0 2

112 V

Vh =I1 = 0

1

221 I

Ih =V2 = 0

2

222 V

Ih =I1 = 0

=

=

=

=

Page 17: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

2

1R

1

- 1

1R

Two Port Networks

Hybrid Parameters: Another example with hybrid parameters.

Given the circuit below.

+

_

+

_

R1

R2V1 V2

I1 -I2The equations for the circuit are:

V1 = (R1 + R2 )I1 + R2 I2

V2 = R2 I1 + R2 I2

The H parameters are as follows.

1

111 I

Vh =2

112 V

Vh =

1

221 I

Ih =2

222 V

Ih =

V2 =0

V2 =0

I1 =0

I1 =0

=

=

=

=

Page 18: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Modifying the two port network:

Earlier we found the z parameters of the following network.

8

20 20 Ω

ΩΩ

Ω

10

+

_

+

_

V1 V2

I1 I2

⎥⎦

⎤⎢⎣

⎡⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

2

1

128820

II

VV

* notes

Presenter
Presentation Notes
Equations from two port networks are not considered to be the end of the problem. We will practically always add components to the input and output. When we do this we must start with the two port parameter, in a certain form, and modify the equations to incorporate the changes at the two ports. For example, we may place a voltage source in series with a resistor at the input port and maybe a load resistor at the output port. The example here illustrates how to handle this problem.
Page 19: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Modifying the two port network:

We modify the network as shown be adding elements outside the two ports

8

20 20 Ω

ΩΩ

Ω

10

+

_

+

_

V1 V2

I1 I2

+

_10 v

4 Ω

We now have:

V1 = 10 - 6I1

V2 = - 4I2

Page 20: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Modifying the two port network:We take a look at the original equations and the equations describingthe new port conditions.

⎥⎦

⎤⎢⎣

⎡⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

2

1

128820

II

VV V1 = 10 - 6I1

V2 = - 4I2

So we have,

10 – 6I1 = 20I1 + 8I2

-4I2 = 8I1 + 12I2

* notes

Presenter
Presentation Notes
Remember that we are trying to solve for I1 and I2 after changing the port conditions. This involves doing some algebra but at a low level. We recombine terms and arrange the original equation in matrix form and we can easily take the inverse to find the solution or else we can use simultaneous equations with our hand calculators.
Page 21: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

-0.2273

0.4545

0

10

168

826

Two Port Networks

Modifying the two port network:

Rearranging the equations gives,

⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

2

1

II

⎥⎦⎤

⎢⎣⎡

⎥⎦

⎤⎢⎣

⎡=⎥

⎤⎢⎣

⎡−1

2

1

II

Page 22: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Y Parameters and Beyond:

Given the following network.

+

_

+

_V1 V2

I1I2

s1

1 Ω

1 Ω

s

(a) Find the Y parameters for the network.

(b) From the Y parameters find the z parameters

Page 23: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

11

11 VI

y =02=V

21

12 VI

y =01=V

12

21 VI

y =02=V 2

222 V

Iy =

01=V

I1 = y11 V1 + y12 V2

I2 = y21 V1 + y22 V2

+

_

+

_V1 V2

I1I2

s1

1 Ω

1 Ω

s

To find y11

⎥⎦⎤

⎢⎣⎡

+=

+=

122)

12

2( 111 s

Is

sIV so = s + 0.5

11

11 VI

y =02=V

We use the above equations toevaluate the parameters from thenetwork.

Y Parameter Example

short

Page 24: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port NetworksY Parameter Example

12

21 VI

y =

02=V +

_

+

_V1 V2

I1

s1

1 Ω

1 Ω

s

I2

21 2IV −=

We see

= 0.5 S

12

21 VI

y =

Page 25: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port NetworksY Parameter Example

+

_

+

_V1 V2

I1

s1

1 Ω

1 Ω

s

I2

21

12 VI

y =01=V

21

12 VI

y =

12 2IV −=

We have

= 0.5 S

short

22

22 VI

y =01=V

We have

)2(2

22 +=

ssIV s

y 15.022 +=

To find y12 and y21 we reversethings and short V1

Page 26: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port NetworksY Parameter Example

Summary:

Y = ⎥⎦

⎤⎢⎣

⎡+−

−+=⎥

⎤⎢⎣

⎡s

syyyy

15.05.05.05.0

2221

1211

Now suppose you want the Z parameters for the same network.

Page 27: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Networks

Going From Y to Z Parameters

For the Y parameters we have:

VYI =

For the Z parameters we have:

IZV =

From above; IZIYV == −1

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

⎥⎥⎦

⎢⎢⎣

⎡=

ΔΔ

Δ

Δ− ==

Y

y

Y

yY

y

Y

y

zz

zzYZ

1121

1222

2221

12111 YY det=Δ

Therefore

where

Page 28: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Parameter Conversions:

Page 29: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Two Port Parameter Conversions:

To go from one set of parameters to another, locate the set of parametersyou are in, move along the vertical until you are in the row that containsthe parameters you want to convert to – then compare element for element

22

11 hz HΔ

=

Page 30: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Interconnection Of Two Port Networks

Three ways that two ports are interconnected:

* Parallel

* Series

* Cascade

[ ] [ ] [ ]ba

yyy +=

[ ] [ ] [ ]ba

zzz +=

[ ] [ ] [ ]ba

TTT =

ya

yb

za

zb

Ta Tb

parametersY

parametersZ

parametersABCD

Page 31: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

Interconnection Of Two Port Networks

Consider the following network:

R1

R2

R1

R2T1 T2

Referring to slide 13 we have;

+

_

+

_

V1 V2

I1 I2

1

2VV

Find

⎥⎦

⎤⎢⎣

⎡−

⎥⎥⎥⎥

⎢⎢⎢⎢

⎡ +

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

⎡ +

=⎥⎦

⎤⎢⎣

2

2

2

121

2

12

21

1

1

1111

2

IV

R

RR

RR

R

RR

RR

IV

Page 32: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

⎥⎦

⎤⎢⎣

⎡−

⎥⎥⎥⎥

⎢⎢⎢⎢

⎡ +

⎥⎥⎥⎥⎥

⎢⎢⎢⎢⎢

⎡ +

=⎥⎦

⎤⎢⎣

2

2

2

121

2

12

21

1

1

1111

2

IV

R

RR

RR

R

RR

RR

IV

Interconnection Of Two Port Networks

Multiply out the first row:

⎥⎥⎥

⎢⎢⎢

⎡−

⎥⎥⎦

⎢⎢⎣

⎡+

⎟⎟⎠

⎞⎜⎜⎝

⎛ ++

⎥⎥

⎢⎢

⎡+

⎟⎟⎠

⎞⎜⎜⎝

⎛ += )( 211

2

212

2

12

2

211

IRRR

RRV

RR

RRR

V

Set I2 = 0 ( as in the diagram)

22211

22

1

2

32 RRRR

RVV

+= Can be verified directly

by solving the circuit

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Page 34: An Introduction To Two – Port Networks · The two port network configuration shown with this slide is practically used universally in all text books. The same go 攀猀 昀漀爀

End of Lesson

Basic Laws of Circuits

Two-Port Networks


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