Reliability and effectiveness of systems of independent automats.
Nanasi, Tibor
1. INTRODUCTION
Reliability, availability and effectiveness of production are the
most important attributes of the quality of production systems
(Boyadjiev et al., 2007; Gerstbakh, 2005). Methods of assessing the
influence of failure probability on the overall volume of production are
prominent topic of interest to factory management (Tolio et al., 2002;
O'Connor, 2009). Failed units are usually repaired and the
temporary overhaul of individual failed machine is covered by activation
of redundant units (Bertsche, 2008; Dekys et al., 2004). The present
paper analyses the influence of failure rate, repair rate, renewal
capacity and the influence of number of redundant units on the overall
production. Redundant units are allowed to act in cold, warm or hot
standby regime. The stochastic model adopted here is Markov process describing the probabilities of states by set of coupled
Kolmogorov-Chapman differential equations (Meixner & Kolnikova,
1984; Lisnianski & Levitin, 2003). Somewhat surprising are the
following conclusions drawn from the present analysis:
--the overall production volume in steady state is linear function
of both the ratio of failure and the repair intensity
--probability of individual states is almost insensitive to the
number of redundant units when the repair capacity is nonzero dominant
influence of the system configuration (k,m,r) on the production volume.
2. MODEL DESCRIPTION
We consider system of independent production units together with a
few standby units. Let k is the number of possible positions for
producing units, which under normal conditions is also the number of
producing machines until the pool of redundant units and the renewal
capacity is exhausted. Let m be the number of redundant units and r is
the measure of the renewal capacity usually identified with the number
of failed units, which can be repaired simultaneously. Total number of
units is then n=k+m. The state of the system is represented by number of
failed units, i.e. in state 0 all units are in up state, in state 1 one
of k units is failed and its repair commences immediately and at the
same time the failed unit is replaced without any delay by one of
redundant units. Thus, the total production continues in full capacity
of k active units. From the state 1 the system returns to state 0 after
the repair of single failed unit is finished or eventually it can pass
from state 1 to state 2 if a failure of another unit happens, etc.
When there are no more redundant units, the production continues
with decreased capacity proportional to k-1 until the repair of failed
units is finished, etc. Ultimately, in state n = k + m all units
including the redundant units are failed and the production ceases until
at least one of failed units is repaired. Thus, the system is at any
time in one of n + 1 possible states. In line with usual assumptions
about Markov process only single failure or single renewal is admitted
at any moment. Consequently, there are only transitions between
neighbouring states. The transitions between states are described by the
failure transition intensity [[lambda].sub.j] and the repair transition
intensity [[mu].sub.j]. Transition intensities multiplied by short time
interval [DELTA]t represent the probability of the event of failure or
repair at time interval (t, t + [DELTA]t). For identical units the
transitional failure intensities [[lambda].sub.j] from state j + 1 to
state the repair intensities [[mu].sub.j] for transition from state j +
1 to state j and the number of actively producing units [[alpha].sub.j]
are given in general by formulas
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (1)
The first formula accounts for the possibility of cold, warm or hot
standby regime of redundant units by including the factor v [member of]
<0,1>, which transforms the failure rate [lambda] of active units
to failure rate [[lambda].sub.s] of standby units. Max(0,m-j) is number
of disposable redundant units at the state j, Min(0,m-j) is counter of
missing working units after all redundant units have been used to
substitute m or more failed units. The number of actively producing
units [[alpha].sub.j] at state j is given by a combination of Min(0,m-j)
with k, the number of working positions. Min(j+1,r) accounts for
disposable repair capacity at state j, which is restricted from above by
number r.
Time evolution of the probabilities [P.sub.i](t) of individual
states can be computed by the system of Kolmogorov-Chapman differential
equations
d/dt P(t) = AP(t) (2)
where A is the system matrix reflecting the probabilities of
possible transitions between states, [P.sup.T](t) = [[P.sub.0](t),
[P.sup.1](t), ..., [P.sub.n](t)] is the vector of probabilities of
individual states. When all units are initially in perfect state, the
initial conditions are of form
[P.sup.T] (0) = [[P.sub.0](0), [P.sub.1](0), ..., [P.sub.n](0)] =
[1, 0, ..., 0] (3)
In the case of generalized Birth and Death process the system
matrix is of tridiagonal structure and the transitions are mapped by the
following matrix for production chain of identical machines of
parameters k=5, m=3, r=3, i.e. there are
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]
5 working positions occupied by 5 machines in perfect state in time
t=0, number of redundant units is 3 as well as at most 3 failed units
can simultaneously and independently undergo the repair. Then the number
of disposable machines is n = 8 and the number of states is N=n+1=9.
3. NUMERICAL RESULTS
The overall volume V(t) of production of the production chain at
time t is directly proportional to the scalar product of the vector
[alpha] = [[[alpha].sub.0], [[alpha].sub.1], ..., [[alpha].sub.n]] with
P(t)
V (t) = u h [alpha] . P(t) = u h [summation over i=0]
[[alpha].sub.i][P.sub.i](t) (4)
where u is production of single unit per unit time, h is the
observed time, [[alpha].sub.i] is number of actively producing units at
state i and [P.sub.i](t) is the probability of state i.
[FIGURE 1 OMITTED]
Numerical results are presented here only for the steady state
solution of the Kolmogorov--Chapman equations (1), as the state
probabilities are typically rapidly decaying functions in time with
tendency to converge to limiting values of the steady state solutions.
Figure 1 illustrates the combinations of failure and repair rate
necessary to achieve the desired level of production steady state for
k=5,m=3,r=3 as well as for k=5,m=1,r=1 on the right. Unlike the time
dependence of state probabilities, here the influence of the
configuration is dominant. The relation (4) has been applied for unit
time interval h=1 and unit production u =1 per hour so that the full
production is 5 when k=5 positions are open. It is obvious that constant
levels of production are implied by linear relation between the failure
and the repair rate. From Figure 1 immediately follows that the
effectiveness of the system is markedly influenced also by such factors
like the renewal capacity and the number of redundant units.
4. CONCLUSION
Somewhat surprising are the following conclusions drawn from the
present analysis:
--the overall production volume in steady state is linear function
of both the ratio of failure and the repair intensity
--probability of individual states is almost insensitive to the
number of redundant units when the repair capacity is nonzero
--dominant influence of the system configuration (k,m,r) on the
production volume.
5. ACKNOWLEDGEMENTS
The work has been supported by grant projects VEGA 1/0256/09 and
VEGA--1/0373/08.
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