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Balanced Truncation: Difference between revisions

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<math> (\hat{A},\hat{B},\hat{C},\hat{D})=(A_{11},B_1,C_1,D) </math>  
<math> (\hat{A},\hat{B},\hat{C},\hat{D})=(A_{11},B_1,C_1,D) </math>  
== Implementation: SR Method==
One computes it for example by the SR Method.
One computes it for example by the SR Method.
First one computes the (Cholesky) factors of the gramians <math>P=S^TS, Q=R^TR</math>. Then we compute the singular value decomposition of <math> SR^T</math>
First one computes the (Cholesky) factors of the gramians <math>P=S^TS,\; Q=R^TR</math>. Then we compute the singular value decomposition of <math> SR^T\;</math>
 
 
<math> SR^T=\begin{bmatrix} U_1 U_2 \end{bmatrix} \begin{bmatrix} \Sigma_1 & \\ & \Sigma_2\end{bmatrix} \begin{bmatrix} V_1^T\\V_2^T\end{bmatrix}</math>
 
Then the reduced order model is given by <math>(W^TAV,W^TB,CV,D)\;</math> where
 
<math> W=R^T V_1\Sigma_1^{-\frac{1}{2}},\quad V= S^T U_1 \Sigma_1^{-\frac{1}{2}}.</math>
 
 
We get then that <math>V^TW=I_r</math> which makes <math> VW^T</math> an oblique projector and hence balanced trunctation a Petrov-Galerkin projection method. The reduced model is stable with Hankel Singular Values given by <math>\sigma_1,\dots,\sigma_r</math>. It is possible to choose r via the computable error bound


<math> \|y-\hat{y}\|_2\leq (2\sum_{k=r+1}^n\sigma_k)\|u\|_2. </math>


<math> SR^T=\begin{bmatrix} U_1 U_2 \end{bmatrix} \begin{bmatrix} \Sigma_1 & \\ & \Sigma_2\end{bmatrix}</math>
==References==
==References==

Revision as of 12:37, 25 March 2013


An important projection model reduction method which delivers high quality reduced models by making an extra effort in choosing the projection subspaces.


A stable system Σ , realized by (A,B,C,D) is called balanced, if the Gramians, i.e. the solutions P,Q of the Lyapunov equations

AP+PAT+BBT=0,ATQ+QA+CTC=0


satisfy P=Q=diag(σ1,,σn) with σ1σ2σn0

The spectrum of (PQ)12 which is {σ1,,σn} are the Hankel singular values.


In order to do balanced truncation one has to first compute a balanced realization via state-space transformation


(A,B,C,D)(TAT1,TB,CT1,D)=([A11A12A21A22],[B1B2][C1C2],D)

The truncated reduced system is then given by

(A^,B^,C^,D^)=(A11,B1,C1,D)

Implementation: SR Method

One computes it for example by the SR Method. First one computes the (Cholesky) factors of the gramians P=STS,Q=RTR. Then we compute the singular value decomposition of SRT


SRT=[U1U2][Σ1Σ2][V1TV2T]

Then the reduced order model is given by (WTAV,WTB,CV,D) where

W=RTV1Σ112,V=STU1Σ112.


We get then that VTW=Ir which makes VWT an oblique projector and hence balanced trunctation a Petrov-Galerkin projection method. The reduced model is stable with Hankel Singular Values given by σ1,,σr. It is possible to choose r via the computable error bound

yy^2(2k=r+1nσk)u2.

References