Lattice and Lattice-Ladder Structures for IIR Systems

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Lattice and Lattice-Ladder

Structures for IIR Systems

Lattice IIR Structure

Consider a system with finite poles and all its zeros at z

=

0 whose transfer function is of the form

H

=

Α

N

1

( ) where

Α

N k

N

=

1 a

N

[ ] − k

N z

=

0.

Lattice IIR Structure

A Direct Form II system with

N finite poles and N zeros at z = 0.

Lattice IIR Structure

Compare the Direct Form II structures for FIR and IIR systems.

If, in the FIR system, we exchange the roles of X

( )

and Y

( )

, b

− a 's (with b

0

=

1) and let N

=

M

1, we get the

IIR system.

FIR IIR

Lattice-Ladder IIR Structure

Modify the FIR lattice structure as illustrated below. Reverse the arrows on all the "f" signals. Reverse the lattice and apply x

[ ] to the previous output and take y

[ ]

from the previous input.

Also re verse the signs of the signals arriving from the bottom. This is now a recursive or feedback structure which can implement an

IIR filter.

Lattice-Ladder IIR Structure

Take the case N

=

1. x

[ ] = f

1

[ ]

, f

0

[ ] = f

1

[ ] −

K g

1 0

[ n

− ]

1

[ ] =

K f

1 0 n

+ g

0

[ n

1

] and y

[ ] = f

0

[ ] = g

0

[ ] = f n

K g

1 0

[ n

1

]

= x

[ ]

= y

[ ] z transforming

Y

( ) +

K z

1

1

Y

( ) =

X

( ) ⇒

H

1

( ) =

1

+

1

1 z K

1

= z

+ z

K

1

Single pole at z

= −

K

1

and a zero at z

=

0.

Lattice-Ladder IIR Structure z

Also, for the N

=

1 case

g

1

G

1

[ ] =

K

1 y

[ ] [ n

1

]

( ) =

K

1

Y

( ) + z

1 Y

G

Y

1

( )

( )

G

1

Y

( )

( )

=

K z 1 K

1

+ − =

1

is the transfer function of a system with a single zero at z

+

1/ K

1 z

= −

1/ K

1

and a pole at zero.

Lattice-Ladder IIR Structure

For the N

=

2 case, it can be shown that

H

2

=

Y

X

( )

( )

=

1

+

K K

1 2

+

1

1

) z

1 +

K z

2

2

= z

2 +

1

( z

2

2

+

1

) z

+

K

2 and

G

Y

2

( )

( )

=

K

2

+

1

(

2

+

1

) z

1 + z

2 =

K

2 z

2 +

K

1

( z

2

K

2

) z

+

1/ K

2

Notice that the coefficients for the FIR and IIR systems occur in rever se order as before.

Lattice-Ladder IIR Structure

H m

=

Y

X

( )

( )

=

Α m

1

( ) and

G

Y m

( )

( )

= Β m

( ) = z

− m Α m and the previous relations for FIR lattices still hold.

Α

0

( ) = Β

0

( ) =

1 ,

Α m

= Α m

1

( ) +

K z m

1 Β m

1

Β m

( ) = z

− m Α m

Α m

1

=

( )

, K m

Α m

( ) −

K

Β m m

1

K m

2

= α m

Lattice-Ladder IIR Structure

If we want to add finite zeros to H m

we can add a ladder network to the lattice. Then the transfer function will be of the form

H

=

1

+

γ

α

N

N

( )

( ) z

+

1

γ

+

N

α

( )

N z

1

( ) z

2

γ

N

( )

α

N

( )

N

N

=

Γ

N

Α

N

( )

( )

y

=

N

m

=

0 v g m m

[ ] ⇒

Y

( ) = m

N

=

0 v G m m

Lattice-Ladder Example

Synthesize the transfer function

H

=

1

− z

1 +

0.5

z

+ z

1 −

0.15

2

2

= z z

2 z

2 − +

0.5

+

0.2

z

0.15

using a lattice-ladder network.

Α

2

( ) = + z

1 −

0.15

z

2

K

2

= −

0.15 and

Β

2

( ) = − + z

1 + z

2

Γ

2

( ) = m

2

=

0 v

Β m m z

1 +

0.5

z

2

Γ

1

( ) = Γ

2

( ) v

2 2

( ) = − z

1 +

0.5

⇒ v

2

= z

2 −

0.5

0.5

(

− +

Γ

1

( ) = − z

1 ⇒ = −

1

1.1

Γ

0

( ) = Γ

1

( ) v

1 1

( ) z

1 + z

2

)

Using

Α m

Α

1

( ) =

1

Lattice-Ladder Example

Α m

( ) −

K m

Β m =

1

K

2 m

+ z

1 −

0.15

z

2

(

0.15

) (

− + z

1 + z

2

)

1

(

0.15

)

2

K

1

1

Α

1

( ) =

= z

0.9775

0.23529 and

Β

1

( ) =

Γ

0

( ) = − z

1

0.23529

( ) (

+ z

1 z

1

+ z

1

)

=

1.3382

⇒ v

0

=

1.3382

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