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where yFREE(t) and yINT(t) denote the output<br />
containing terms with and without interactions.<br />
In terms of the former definitions (12) is rewritten<br />
as<br />
y1(t) = [11,1] + [12,2] +<br />
[11,1|11,1] + [11,1|12,1] + [11,1|21,1] +<br />
[11,1|22,2] + [12,2|11,1] + [12,2|12,2] +<br />
[12,2|21,1] + [12,2|22,2] + [11,1|11,1|11,1]<br />
+ [11,1|11,1|12,2] + [11,1|12,2|11,1] +<br />
[11,1|12,2|12,2] + [11,1|11,1|21,1] +<br />
[11,1|11,1|22,2] + [11,1|12,2|21|1]<br />
+[11,1|12,2|22,1] +[11,1|11,1|21,1] +<br />
[11,1|11,1|22,2] + [11,1|12,2|21,1]<br />
+[11,1|12,2|22,2] + [11,1|21,1|21,|1] +<br />
[11,1|21,1|22,2] + [11,1|22,2|21,1] +<br />
[11,1|22,2|22,2] +[12,2|11,1|11,1] +<br />
[12,2|11,1|12,2] + [12,2|12,2|11,1]<br />
+[12,2|12,2|12,2] +[12,2|11,1|21,1] +<br />
[12,2|11,1|22,2] + [12,2|12,2|21,1] +<br />
[12,2|12,2|22,2] + [12,2|21,1|11,1] +<br />
[12,2|21,1|12,2] + [12,2|22,2|11,1] +<br />
[12,2|22,2|12,2] + [12,2|21,1|21,1] +<br />
[12,2|21,1|22,2] + [12,2|22,2|21,1] +<br />
[12,2|22,2|22,2]. (13)<br />
Same as (11) the full expression relating the<br />
third order diagonal terms are recognized with<br />
36 additional interactions terms by adding complexities<br />
to the individual output,<br />
y1(t) = Diag3 [11,1] + Diag3 [12,2] +<br />
[11,1|12,1] + [11,1|21,1] + [11,1|22,2] +<br />
[12,2|11,1] + [12,2|21,1] + [12,2|22,2] +<br />
[11,1|11,1|12,2] + [11,1|12,2|11,1] +<br />
[11,1|12,2|12,2] + [11,1|11,1|21,1] +<br />
[11,1|11,1|22,2] + [11,1|12,2|21|1] +<br />
[11,1|12,2|22,1] + [11,1|11,1|21,1] +<br />
[11,1|11,1|22,2] + [11,1|12,2|21,1] +<br />
[11,1|12,2|22,2] + [11,1|21,1|21,|1] +<br />
[11,1|21,1|22,2] + [11,1|22,2|21,1] +<br />
[11,1|22,2|22,2] + [12,2|11,1|11,1] +<br />
[12,2|11,1|12,2] + [12,2|12,2|11,1] +<br />
[12,2|11,1|21,1] + [12,2|11,1|22,2] +<br />
[12,2|12,2|21,1] + [12,2|12,2|22,2] +<br />
[12,2|21,1|11,1] + [12,2|21,1|12,2] +<br />
[12,2|22,2|11,1] + [12,2|22,2|12,2] +<br />
[12,2|21,1|21,1] + [12,2|21,1|22,2] +<br />
[12,2|22,2|21,1] + [12,2|22,2|22,2] (14)<br />
with Diag3 [11,1] = [11,1] + [11,1|11,1] +<br />
[11,1|11,1|11,1] and Diag3 [12,2] = [12,2] +<br />
[12,2|12,2] + [12,2|12,2|12,2]. The hypothesis<br />
CIENCIA, CULTURA Y TECNOLOGÍA - UNIVERSIDAD TECNOLÓGICA DEL PERÚ<br />
in this study is that the equation (14) containing<br />
only in a first instance diagonal terms would be<br />
an identification system tool up to certain grade<br />
of approximation. Nevertheless, it is important<br />
to recall that the non-diagonal terms can also<br />
add more information on the instabilities and intrinsic<br />
properties of system. Now the main task<br />
is that of taking data from plant and to perform<br />
comparisons in order to validate the equations<br />
(11) and (14).<br />
III POWER PLAN AND DATA ACQUISITION<br />
A. Power Plant Generalities and Data<br />
Data have been taped from an ordinary run at<br />
the 160 MW combined cycle plant located at<br />
Lima North (Ventanilla) which is responsible to<br />
produce electricity power for a 10% of the whole<br />
population at Lima City.<br />
Figure 1. Data extracted from combined cycle plant by showng<br />
the mosphologies of input and output curves. Time runs in<br />
seconds.<br />
The combined cycle takes both water vapor and<br />
natural gas extracted from Camisea, a nature<br />
gas reservoir located in Cuzco. From a common<br />
perspective, it can be perceived as a 2×2 MIMO<br />
system. The valve position and the water flux<br />
act as the input ones, whereas the drum level<br />
and pressure as the output ones. In Fig. 1 is<br />
depicted data by showing the behavior at the<br />
first 120 seconds of run. It is noteworthy that<br />
all trajectories share the same morphology. Perhaps<br />
an exception occurs with the drum level<br />
whose history shows a dip on the 45th second<br />
[4]. On the other hand this event is not seen to<br />
be strongly correlated with each other. Indeed, it<br />
should be noted that a good indicator which tell<br />
us about the normal (or healthy) functionality<br />
of the tank is that of the drum pressure which<br />
acquires an interesting stability over the horizon,<br />
starting at the first 35 seconds of run. Two<br />
minor fluctuations appear on the 35th and 55th<br />
seconds. We noted also that the water flux and<br />
valve position posses a similar trajectory. By the<br />
other hand, water flux curve exhibits a substan-<br />
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