Power spectrum of the combined dynamic systems.
Stremy, Maximilian ; Bezak, Tomas
Abstract: In the article there are mentioned combined discrete
dynamic systems and analysis of their power spectrum especially aimed to
the event activated part of the system. Combined dynamic systems, also
called hybrid systems are the fusion result of the time-driven and event
activated systems. System consists of a combination of cyclically
recurring processes in each period of processing and the stochastically
emerging events. Power spectrum determination, described in the article,
assumes stochastic events generation corresponding to the Normal
probability distribution. The power spectrum of stochastic events
generated by the Normal Poisson distribution in the combined systems is
created using the theory of white noise.
Key words: normal distribution, stochastic events, combined dynamic
systems, power spectrum, white noise
1. INTRODUCTION
Combined systems consist of two discrete systems parts: discrete
time-dynamic-activated systems, as well as discrete events systems.
Combined dynamic systems, also called hybrid systems are the fusion
result of time-driven and event activated systems. In case that notion
"Hybrid system" is used in connection between distributed
control system and programmable logical controllers, neural networks,
genetic algorithms and fuzzy logics, or combination of electric and
mechanical power units (Zdansky, 2009), for better prediction and better
identification the concept of "Combined dynamic system" was
introduced.
Generally, [T.sub.O] sampling period in dynamic systems is
considered as constant and includes only the [T.sub.R] time required to
process all the necessary control and cyclically recurring processes in
the system. In contrast, the combined dynamic systems contemplate the
sampling period, regardless of whether it is constant or variable,
extended by the time constant [T.sub.P] needed to execute random events
in the system (Fig. 1).
Event component of the sampling period significantly affects the
behavior of the entire system. It affects controllability, stability and
overall dynamic properties of the combined systems that are designed by
ratio of events and time-controlled discrete systems. Time-controlled
part of the combined discrete systems is realized by a constant cyclic
monitoring, processing and evaluation of inputs and states of the
system. Event part is in automated control systems implemented by
service interruptions, called upon the occurrence of any of the events.
A particular problem in such systems appears to be how to determine the
impact of stochastically changing event component of their dynamic
properties and quality control (Stremy, 2010).
[FIGURE 1 OMITTED]
2. NORMAL PROBABILITY DISTRIBUTION OF EVENT-TIME CONSTANT
Normal probability distribution predicts balanced arising events
distribution along the average value Ta calculated from the equation
[T.sub.a] = [T.sub.c]/N, (1)
where [T.sub.c] is the time required to service all existing
interrupts and N is the number of interruptions occurring in a given
cycle. Root mean square (rms) deviation from the mean value of [T.sub.a]
is then determined by the relationship
[sigma] = [square root of [n.summation over (i=1)[([x.sub.i] -
[mu]).sup.2]]/n - 1], (2)
where [mu] = [T.sub.a]--average time needed to handle new events.
Using the rms value criteria of randomly generated interrupts could
be determined. This means how likely the events that occur in the
sampling period of the combined dynamic system will be executed. The
size of the sampling period corresponds to the time mean value [mu] in
this case. The probability that the events in this interval extended /
shortened by the time, which is the rms value equals to:
* 68,3%--in the [mu] + -[sigma],
* 95,6%--in the [mu] + -2[sigma],
* 99,7%--in the [mu] + -3[sigma].
Probability density distribution f(t) is the derivation of the
distribution function F(t). By this it is possible to determine the
probability of particular events generation N as well as the probability
of this events creation amount in time interval [DELTA]t (Banks, 2001):
f(t) = dF(t)/dt [approximately equal to] [n.sub.x](t + [DELTA]t) -
[n.sub.x](t)/N[DELTA]t. (3)
Probability density distribution f(t) at time t has the form:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII], (4)
while its maximum value corresponds to the function f(t) at time
[T.sub.a]
f([T.sub.a]) = 1/[sigma][square root of 2[pi]]. (5)
Time constant [T.sub.p], in the combined system may be equal to:
(1) the mean of the time needed to handle new events [??] [T.sub.p]
= [T.sub.a],
(2) the mean of the time needed for handling events generated
enlarged / reduced by the value [DELTA] [??] [T.sub.p] = [T.sub.a] +
-[DELTA], including time needed to handle events with a fixed
probability percentage (e.g. + [sigma] means probability around 74%)
(3) the mean of the time needed to handle new events and three
times the rms value of [T.sub.p] = [T.sub.a] + 3[sigma]. This value
includes handling of all events in the cycle with a probability of
99.7%.
3. POWER SPECTRUM OF STOCHASTIC SIGNALS
It is known that the harmonic analysis of deterministic processes
can be used to express them by means of Fourier series or Fourier
integral depending on whether a periodic or aperiodic processes. In a
similar way we can characterize the distribution of energy in stationary
random processes using correlation analysis, respectively their internal
structure and apply this procedure for needs of spectral analysis and
optimization of combined dynamical systems dynamical properties.
We can express the relationship between the autocorrelation function Kx([tau]) of stationary stochastic process and its power
spectral density Sx([omega]) (Levin, 1960) based on the Wiener-Khinchin
relations. If the following conditions are met:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII], (6)
where M and N are optional final.
Because the autocorrelation function is real and odd, if [tau] = 0,
we can write:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (7)
which is actually an expression of the overall standardized mean
performance of the stationary stochastic signal. Similarly, we can
express the spectral power density for [omega] = 0:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII], (8)
We can see that the area under the autocorrelation function is
proportional to the value of power spectral density for [omega] = 0.
Theory of white noise is applied to the combined dynamical systems,
while the stochastic part of these systems approaching the normal
probability distribution is represented as a process of constant and
frequency unlimited intensity of power spectral density. Discoloration of white noise is expected to within the system. Using the normal
probability distribution assumptions we can derive the Gaussian white
noise intensity value, respectively value of combined dynamical systems
stochastic part.
White noise is a stationary random process, in which the power
spectral density is constant throughout the frequency range (Ondracek,
2003):
[S.sub.x] ([omega]) = N = const. (9)
Autocorrelation function of white noise, whose mean power is
infinite, by the Wiener-Khinchin relations is:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (10)
Dispersion of frequency-limited white noise can be described by the
intensity in the form (Besekerskij, 1969):
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (11)
Mean square error [sigma] is then equal to
[sigma] = [square root of N][square root of [DELTA]f], (12)
the autocorrelation function for frequency limited white noise has
form:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (13)
For the normal probability distribution the dispersion of the
stochastic process will be equal to D = 6[sigma]. After substituting
into equation (12) we obtain expression of random process intensity:
N = D/[DELTA]f = 6[sigma]/[DELTA]f. (14)
4. CONCLUSION
To determine the [T.sub.P], time necessary for the execution of
random events service routines in a given cycle, we are using the
statistical evaluation of emerging events and their probability
estimation. The white noise is a theoretical assumption--the colored
noise is the input in practical terms. In our case, the system input in
the form of stochastic events will be decolorized. It will assume
generating of events underlying to the requirements of white noise (or
frequency-limited white noise), while the color is transferred to the
system itself.
5. REFERENCES
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Besekerskij, V. A. (1969). Sbornik zadac po teorii automaticheskovo
regulirovanja iI upravlenja, Nauka, pp. 588, Moscow
Levin, B. R. (1960). Teoria sluchajnych procesov i jijo primenenie
z padiotechniky, Izdatelstvo Sovetskoe Radio, pp. 662, Moscow
Ondracek, O. (2003). Signaly a sustavy, Slovak University of
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