| Robust Control Toolbox | |
| Provide feedback about this page |
Simplified access to Hankel singular value based model reduction functions
Syntax
GRED = reduce(G) GRED = reduce(G,order) [GRED,redinfo] = reduce(G,'key1','value1',...) [GRED,redinfo] = reduce(G,order,'key1','value1',...)
Description
returns a reduced order model reduce
GRED of G and a struct array redinfo containing the error bound of the reduced model, Hankel singular values of the original system and some other relevant model reduction information.
An error bound is a measure of how close GRED is to G and is computed based on either additive error, || G-GRED ||
, multiplicative error, || G-1(G-GRED) ||
, or nugap error (ref.: ncfmr) [1],[4],[5].
Hankel singular values of a stable system indicate the respective state energy of the system. Hence, reduced order can be directly determined by examining the system Hankel SV's. Model reduction routines, which based on Hankel SV's are grouped by their error bound types. In many cases, the additive error method GRED=reduce(G,ORDER) is adequate to provide a good reduced order model. But for systems with lightly damped poles and/or zeros, a multiplicative error method (namely, GRED=reduce(G,ORDER,'ErrorType','mult')) that minimizes the relative error between G and GRED tends to produce a better fit.
This table describes input arguments for reduce.
A batch run of a serial of different reduced order models can be generated by specifying order = x:y, or a vector of integers. By default, all the anti-stable part of a physical system is kept, because from control stability point of view, getting rid of unstable state(s) is dangerous to model a system.
'MaxError' can be specified in the same fashion as an alternative for 'ORDER' after an 'ErrorType' is selected. In this case, reduced order will be determined when the sum of the tails of the Hankel SV's reaches the 'MaxError'
Argument
Value
Description
'Algorithm''balance''schur''hankel''bst''ncf'Default for
'add' (balancmr)
Option for 'add' (schurmr)
Option for 'add' (hankelmr)
Default for 'mult' (bstmr)
Default for 'ncf' (ncfmr) 'ErrorType''add''mult''ncf'Additive error (default)
Multiplicative error at model output
NCF nugap error'MaxError'A real number or a vector of different errors
Reduce to achieve H
error.
When present, 'MaxError' overrides ORDER input.'Weights'{Wout,Win} cell arrayOptimal 1x2 cell array of LTI weights
Wout (output) and Win (input); default is both identity; used only with 'ErrorType', 'add'. Weights must be invertible.'Display''on' or 'off'Display Hankel singular plots (default
'off'). 'Order'Integer, vector or cell array
Order of reduced model. Use only if not specified as 2nd argument.
.
Weights on the original model input and/or output can make the model reduction algorithm focus on some frequency range of interests. But weights have to be stable, minimum phase and invertible.
This table describes output arguments.
G can be stable or unstable. G and GRED can be either continuous or discrete.
A successful model reduction with a well-conditioned original model G will ensure that the reduced model GRED satisfies the infinity norm error bound.
Example
Given a continuous or discrete, stable or unstable system, G, the following commands can get a set of reduced order models based on your selections:
rand('state',1234); randn('state',5678);G = rss(30,5,4); [g1, redinfo1] = reduce(G); % display Hankel SV plot % and prompt for order [g2, redinfo2] = reduce(G,20); % default to balancmr [g3, redinfo3] = reduce(G,[10:2:18],'algorithm','schur'); % select schurmr [g4, redinfo] = reduce(G,'ErrorType','mult','MaxError',[0.01, 0.05]); rand('state',12345); randn('state',6789); wt1 = rss(6,5,5); wt1.d = eye(5)*2; wt2 = rss(6,4,4); wt2.d = 2*eye(4); [g5, redinfo5] = reduce(G, [10:2:18],'weight',{wt1,wt2}); [g6, redinfo6] = reduce(G,'ErrorType','add','algorithm','hankel', ...'maxerror',[0.01]); for i = 1:6 figure(i); eval(['sigma(G,g' num2str(i) ');']); end
Reference
[1] K. Glover, "All Optimal Hankel Norm Approximation of Linear
Multivariable Systems, and Their L
- error Bounds," Int. J. Control, vol. 39,
no. 6, pp. 1145-1193, 1984.
[2] M. G. Safonov and R. Y. Chiang, "A Schur Method for Balanced Model Reduction," IEEE Trans. on Automat. Contr., vol. AC-2, no. 7, July 1989, pp. 729-733.
[3] M. G. Safonov, R. Y. Chiang and D. J. N. Limebeer, "Optimal Hankel Model Reduction for Nonminimal Systems," IEEE Trans. on Automat. Contr., vol. 35, No. 4, April, 1990, pp. 496-502.
[4] M. G. Safonov and R. Y. Chiang, "Model Reduction for Robust Control: A Schur Relative-Error Method," International Journal of Adaptive Control and Signal Processing, vol. 2, pp. 259-272, 1988.
[5] K. Zhou, "Frequency weighted L
error bounds," Syst. Contr. Lett., Vol. 21,
115-125, 1993.
See Also
balancmr Balanced truncation via square-root method
schurmr Balanced truncation via Schur method
bstmr Balanced stochastic truncation via Schur method
ncfmr Balanced truncation for normalized coprime factors
hankelmr Hankel minimum degree approximation
hankelsv Hankel singular value
| Provide feedback about this page |
![]() | frd/rcond | repmat | ![]() |
| © 1984-2008- The MathWorks, Inc. - Site Help - Patents - Trademarks - Privacy Policy - Preventing Piracy - RSS |