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for a substantial time in advance. I apply the<br />

tunable system identification for eliminating the<br />

zeros but not the overflows. Once that convolution<br />

integrals have been set off the parameters<br />

I move the time steps forward and backward for<br />

T= - 1 and T = -2 because the past time steps<br />

are necessary for identifying the possible source<br />

of collapses. When the parameters are tested to<br />

be positive all them stay for a next evaluation<br />

with different values. This operation is repeated<br />

once more time and the results are seen in the<br />

figure 2 when the collapse situations are under<br />

control with only one collapse remains.<br />

Fig. 2.- Recovering of tunable system by<br />

reducing the instabilities which appear as<br />

consequence of the choice parameters set<br />

constants for next and previous time steps.<br />

In figure 2 also one sees the presence of the<br />

collapsing over the 14 th time step. It tells that<br />

a new evaluation should be done. It is done<br />

and the figure 3 which indicates the absence<br />

of collapses to zero but still remains the values<br />

which provides overflow to the system. Finally<br />

en figure 3 one sees the absence of overflows<br />

which means besides the termination of attacks<br />

aftermaths. However there are some small fallings<br />

but the systems is recovered sudden and<br />

fast within a range of 1/10 time step. It has<br />

an explanation: the tunable system is identified<br />

just for the former parameters but the initial<br />

shooting set parameters has to be changed<br />

from a metric 0000001 to one 1100111. It is<br />

because the first time steps are recorded with<br />

errors since the 12 th up to the 14 th time step.<br />

Two things: every system is sometimes composed<br />

of real parameters and some time they<br />

are depending on the complex part when the<br />

transfer functions have zeros in their denominator.<br />

It is not mandatory for tunable system identification,<br />

because in this method we evaluate<br />

directly by using the metric for each time step.<br />

Second, the absence of attacks to some system<br />

does not means that they should be build<br />

without any strategy for stopping it for previous<br />

evaluation of the convolution integral. For the<br />

most general representation, system should<br />

bring a protection mechanism to be tunable not<br />

CIENCIA, CULTURA Y TECNOLOGÍA - UNIVERSIDAD TECNOLÓGICA DEL PERÚ<br />

only time but also in parameters metric. Once<br />

the metric is given for a few time steps the job<br />

of any tunable system identification will be that<br />

of predicting the future from those given at past<br />

without any knowledge to priori. It represents<br />

a firm advantage for trying identifying systems<br />

which normally are not under control after successive<br />

collapses and which would not have any<br />

chance to be restored [3]. In future I will do<br />

a similar study but with the simulation of time<br />

step history for clarifying the hypothesis of tunable<br />

system identification.<br />

Fig. 3.- Full recovering of tunable system<br />

without any zero but still the overflows are<br />

not negligible. Tunable system identification is<br />

therefore successfully applied.<br />

Acknowledgments<br />

I express my sincere thanks to Eng. Pamela<br />

Calipuy, Eng. Alert Mendoza by their enormous<br />

support in various aspects of my work at the<br />

FIEM-<strong>UTP</strong>.<br />

References<br />

[1] Tunable microwave and millimeter-wave<br />

band-pass filters Uher, J.; Hoefer, W.J.R.<br />

Microwave Theory and Techniques, IEEE Transactions<br />

on Volume 39, Issue: 4<br />

Digital Object Identifier: 10.1109/22.76427<br />

Publication Year: 1991 , Page(s): 643 – 653.<br />

[2] MEMS-Based Tunable LC Bandstop Filter<br />

With an Ultra-Wide Continuous Tuning Range<br />

Hyung Suk Lee; Dong-Hoon Choi; Jun-Bo Yoon<br />

Microwave and Wireless Components Letters,<br />

IEEE Volume 19, Issue: 11<br />

Digital-Object-Identifier:10.1109/LMWC.2009.<br />

203210 Publication Year: 2009 , Page(s): 710<br />

– 712.<br />

[3] Synthesis of tunable optical waveguide filters<br />

using digital signal processing technique<br />

Nam Quoc-Ngo;Binh-L.N, Lightwave Technology,<br />

Journal of Volume: 24 , Issue: 9<br />

DigitalObjectIdentifier:10.1109/<br />

JLT.2006.880160<br />

Publication Year: 2006 , Page(s): 3520 – 3531.<br />

29

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