reduce
简化访问汉克尔基于奇异值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 modelreduce
GRED
ofG
and a struct arrayredinfo
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 closeGRED
is toG
and is computed based on eitheradditive error,∥G-GRED
∥∞,multiplicative error,∥G
–1(G-GRED)
∥∞, ornugap 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 singular values are grouped by their error bound types. In many cases, the additive error methodGRED=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 betweenG
andGRED
tends to produce a better fit.
This table describes input arguments forreduce
.
Argument |
Description |
---|---|
G |
LTI model to be reduced (without any other inputs will plot its Hankel singular values and prompt for reduced order). |
ORDER |
(Optional) Integer for the desired order of the reduced model, or optionally a vector packed with desired orders for batch runs. |
A batch run of a serial of different reduced order models can be generated by specifyingorder = 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 |
---|---|---|
|
|
Default for Option for Option for Default for Default for |
|
|
Additive error (default) Multiplicative error at model output NCF nugap error |
|
A real number or a vector of different errors |
Reduce to achieve H∞error. When present, |
|
|
Optimal 1x2 cell array of LTI weights |
|
|
Display Hankel singular plots (default |
|
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.
Argument |
Description |
---|---|
GRED |
LTI reduced order model. Becomes multi-dimensional array when input is a serial of different model order array. |
REDINFO |
A STRUCT array with 3 fields:
|
G
can be stable or unstable.G
andGRED
can be either continuous or discrete.
A successful model reduction with a well-conditioned original modelG
will ensure that the reduced modelGRED
satisfies the infinity norm error bound.
Examples
References
[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[[BULLET]] error bounds," Syst. Contr. Lett., Vol. 21, 115-125, 1993.