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Time update . Compute:
P .k C 1/ D J .x.k//P.k/J T .x.k// C Q.k/
x .k C 1/ D .x.k// C L.k/ u .k/
(4.93)
4.12.2
Design of a Disturbance Observer for the Model
of the Coupled Neurons
Using Eq. ( 4.69 ), the nonlinear model of the coupled neurons can be written in the
MIMO canonical form that was described in Sect. 4.8 , that is
0
@
1
A D
0
@
1
A
0
@
1
A C
0
@
1
A
z 1
z 2
z 3
z 4
0100
0000
0010
0000
z 1
z 2
z 3
z 4
00
10
00
01
v 1
v 2
(4.94)
where z 1 D y 1 , z 2 Dy 1 , z 3 D y 2 and z 4 Dy 2 , while v 1 D L f h 1 .x/ C
L g 1 L f h 1 .x/ u 1 C L g 2 L f h 1 .x/ u 2 and v 2 D L f h 2 .x/ C L g 1 L f h 2 .x/ u 1 C
L g 2 L f h 2 .x/ u 2 . Thus one has a MIMO linear model of the form
z D A z C B v
z m D C z
(4.95)
where z D Πz 1 ; z 2 ; z 3 ; z 4 T and matrices A,B,C are in the MIMO canonical form
0
1
0
1
0
1
0100
0000
0010
0000
00
10
00
01
10
00
01
00
@
A
@
A
@
A
A D
B D
C T
D
(4.96)
Assuming now the existence of additive input disturbances in the linearized model
of the coupled neurons described in Eq. ( 4.69 ) one gets
L f h 1 .x/
L f h 2 .x/
!
z 2
z 2
D
(4.97)
L g 1 L f h 1 .x/ L g 2 L f h 1 .x/
L g 1 L f h 2 .x/ L g 2 L f h 2 .x/
u 1 C d 1
u 2 C d 2
C
These disturbances can be due to external perturbations affecting the coupled
neurons and can also represent parametric uncertainty for the neurons' model. It
can be assumed that the additive disturbances d i ;iD 1;2 are described by the
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