Hankel norm approximation, Hankel norm approximation -6 – National Instruments NI MATRIXx Xmath User Manual

Page 29

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Chapter 2

Additive Error Reduction

Xmath Model Reduction Module

2-6

ni.com

with controllability and observability grammians given by,

in which the diagonal entries of

Σ are in decreasing order, that is,

σ

1

≥ σ

2

≥ ···, and such that the last diagonal entry of Σ

1

exceeds

the first diagonal entry of

Σ

2

. It turns out that Re

λ

i

(

)<0 and

Re

λ

i

(A

11

A

12

A

21

)< 0, and a reduced order model G

r

(s) can be

defined by:

The attractive feature [LiA89] is that the same error bound holds as for
balanced truncation. For example,

Although the error bounds are the same, the actual frequency pattern of
the errors, and the actual maximum modulus, need not be the same for
reduction to the same order. One crucial difference is that balanced
truncation provides exact matching at

ω = ∞, but does not match at DC,

while singular perturbation is exactly the other way round. Perfect
matching at DC can be a substantial advantage, especially if input signals
are known to be band-limited.

Singular perturbation can be achieved with

mreduce( )

. Figure 2-1 shows

the two alternative approaches. For both continuous-time and discrete-time
reductions, the end result is a balanced realization.

Hankel Norm Approximation

In Hankel norm approximation, one relies on the fact that if one chooses an
approximation to exactly minimize one norm (the Hankel norm) then the
infinity norm will be approximately minimized. The Hankel norm is
defined in the following way. Let G(s) be a (rational) stable transfer

P

Q

Σ

Σ

1

0

0

Σ

2

=

=

=

A

22

1

A

22

1

x·

A

11

A

12

A

22

1

A

21

(

)x

B

1

A

12

A

22

1

B

2

+

(

)u

+

=

y

C

1

C

2

A

22

1

A

21

(

)x

D C

2

A

22

1

B

2

(

)u

+

=

G j

ω

( ) G

r

j

ω

( )

2tr

Σ

2

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