the admittance matrix

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A R D B  O  O  F  E  D  U   Adopted by the of Education for California Public Schools California State Board December, 1997 English–Language Arts Content Standards Kindergarten Through Grade Twelve California Department of Education Reposted June 9, 2009

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Page 1: The Admittance Matrix

8/6/2019 The Admittance Matrix

http://slidepdf.com/reader/full/the-admittance-matrix 1/5

Page 2: The Admittance Matrix

8/6/2019 The Admittance Matrix

http://slidepdf.com/reader/full/the-admittance-matrix 2/5

03/01/05 The Admittance Matrix.doc 2/5

Jim Stiles The Univ. of Kansas Dept. of EECS

(given that 0 for all )m mn  k 

I Y V k n

V = = ≠  

Note here that the voltage at all but one port must be equal to

zero. We can ensure that by simply placing a short circuit at

these zero voltage ports!

Note that 1mn mn  Y Z ≠ !

1I 

2 0V  =

1V +

2I 

4-port 

microwave 

device  

Z 0   Z 0  

Z 0  

Z 0  

3I 

4I 

3 0V  =

4 0V  =

 

Page 3: The Admittance Matrix

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03/01/05 The Admittance Matrix.doc 3/5

Jim Stiles The Univ. of Kansas Dept. of EECS

Now, we can thus equivalently state the definition of trans-

admittance as:

(given that all ports are )m mn 

V Y k n I 

= ≠ short-circuited  

Just as with the trans-impedance values, we can use the trans-

admittance values to evaluate general circuit problems, where

none of the ports have zero voltage.

Since the device is linear, the current at any one port due to all

the port currents is simply the coherent sum of the currents at

that port due to each of the port voltages!

For example, the current at port 3 can be determined by:

3 33 3 32 2 31 134 4I Y V Y V Y V Y V  = + + +  

More generally, the current at port m of an N -port device is:

1

m mn n  n 

I Y V =

= ∑  

This expression can be written in matrix form as:

Page 4: The Admittance Matrix

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Jim Stiles The Univ. of Kansas Dept. of EECS

=I Y V  

Where I is the vector:

[ ]1 2 3

N I ,I ,I , ,I  =I  

and V is the vector:

1 2 3

N V ,V ,V , ,V  ⎡ ⎤= ⎣ ⎦V …  

And the matrix Y is called the admittance matrix:

11 1

1

m mn 

Y Y 

Y Y 

⎡ ⎤⎢ ⎥= ⎢ ⎥⎢ ⎥⎣ ⎦

 Y

 

The admittance matrix is a N  by N  matrix that completelycharacterizes a linear, N -port device. Effectively, the

admittance matrix describes a multi-port device the way that L Y  

describes a single-port device (e.g., a load)!

But beware! The values of the admittance matrix for a

particular device or network, just like L Y , are frequency

dependent! Thus, it may be more instructive to explicitly write:

( )

( ) ( )

( ) ( )

11 1

1

m mn 

Y Y 

Y Y 

⎡ ⎤⎢ ⎥= ⎢ ⎥⎢ ⎥⎣ ⎦

 Y

ω ω 

ω 

ω ω 

 

Page 5: The Admittance Matrix

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Jim Stiles The Univ. of Kansas Dept. of EECS

Q: You said earlier that 1mn mn  Y Z ≠ . Is there any relationship

between the admittance and impedance matrix of a given

device?

A: I don’t know! Let’s see if we can figure it out.

Recall that we can determine the inverse of a matrix. Denoting

the matrix inverse of the admittance matrix as1−

 Y , we find:

( )1 1

1 1

1

− −

− −

=

=

⎛ ⎞= ⎜ ⎟⎝ ⎠

=

I Y V

 Y I Y Y V

 Y I Y Y V

 Y I V

 

Meaning that: 1−=V Y I  

But, we likewise know that:

=V Z I  

By comparing the two previous expressions, we can conclude:

1 1and− −= =Z Y Y Z