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204 CHAPTER 11. H 2 MODEL-ORDER REDUCTION FROM ORDER N TO N-3<br />
with z 0 (ρ 2 ),z 1 (ρ 2 ),...,z η1 (ρ 2 ) all polynomial in ρ 2 with a maximal degree of η 2 .The<br />
idea is <strong>to</strong> substitute this expression for z(ρ 1 ,ρ 2 ) in<strong>to</strong> (11.22), which leads <strong>to</strong>:<br />
(<br />
) (z0<br />
P (ρ 2 ) T + ρ 1 Q(ρ 2 ) T (ρ 2 ) − ρ 1 z 1 (ρ 2 )+ρ 2 1z 2 (ρ 2 )+...+(−1) η1 ρ η1<br />
1 z η 1<br />
(ρ 2 ) ) =<br />
1<br />
(<br />
·<br />
(<br />
+P (ρ 2 ) T z 0 (ρ 2 )<br />
)<br />
)<br />
+<br />
ρ 1 ·<br />
(<br />
−P (ρ 2 ) T z 1 (ρ 2 ) +Q(ρ 2 ) T z 0 (ρ 2 )<br />
)<br />
+<br />
ρ 2 1 · +P (ρ 2 ) T z 2 (ρ 2 ) −Q(ρ 2 ) T z 1 (ρ 2 ) +<br />
.<br />
.<br />
.<br />
(<br />
)<br />
.<br />
ρ η1<br />
1 ·<br />
(<br />
(−1) η1 P (ρ 2 ) T z η1 (ρ 2 ) (−1) η1−1 Q(ρ 2 ) T z η1−1(ρ 2 )<br />
)<br />
+<br />
ρ η1+1<br />
1 ·<br />
(−1) η1 Q(ρ 2 ) T z η1 (ρ 2 ) =0<br />
(11.24)<br />
When the relationships for the coefficients are worked out, this generates a system<br />
of equations which can be expressed in matrix-vec<strong>to</strong>r form as follows:<br />
⎛<br />
P (ρ 2 ) T 0 ... ... 0<br />
⎞<br />
. ⎛<br />
Q(ρ 2 ) T P (ρ 2 ) T ..<br />
0 Q(ρ 2 ) T . .. . ..<br />
. 0 0 .. . .. . ..<br />
⎜<br />
⎝<br />
⎜<br />
⎝<br />
.<br />
.<br />
.<br />
.. P (ρ2 ) T ⎟<br />
⎠<br />
0 0 ... ... Q(ρ 2 ) T<br />
⎛<br />
M η1,η 2<br />
(ρ 2 )<br />
⎜<br />
⎝<br />
z 0 (ρ 2 )<br />
−z 1 (ρ 2 )<br />
z 2 (ρ 2 )<br />
.<br />
(−1) η1 z η1 (ρ 2 )<br />
z 0 (ρ 2 )<br />
−z 1 (ρ 2 )<br />
z 2 (ρ 2 )<br />
.<br />
.<br />
(−1) η1 z η1 (ρ 2 )<br />
⎞<br />
=<br />
⎟<br />
⎠<br />
⎞<br />
=0<br />
⎟<br />
⎠<br />
(11.25)<br />
where the block matrix M η1,η 2<br />
(ρ 2 ) has dimensions (η 1 +2) m × (η 1 +1) n. The rank<br />
of the matrix M η1,η 2<br />
(ρ 2 ) is denoted by r η1,η 2<br />
and it holds that r η1,η 2<br />
< (η 1 +1)n.<br />
Since the variable η 2 denotes the degree of ρ 2 in z(ρ 1 ,ρ 2 ), z i (ρ 2 ) can be written<br />
as:<br />
z i (ρ 2 )=z i,0 + ρ 2 z i,1 + ρ 2 2 z i,2 + ...+ ρ η2<br />
2 z i,η 2<br />
, (11.26)<br />
for i =0,...,η 1 .<br />
When (11.26) is substituted in<strong>to</strong> the equations of (11.25) and the relationships<br />
for the coefficients are worked out, a system of equations can be set up which only<br />
involves constant coefficients. When P (ρ 2 ) T = B T + ρ 2 D T and Q(ρ 2 ) T = C T are<br />
plugged in<strong>to</strong> the expressions, the resulting system of equations can be written in