Reliability of simple pneumatic systems.
Nanasi, Tibor
1. INTRODUCTION
Pneumatic systems have reputation of extremely high reliability
when compared to hydraulic or mechanical equipment. Producers estimate
the life cycle of various types of valves, which are key elements of
pneumatic systems, up to as high numbers as fifty million of cycles
(Smith, 2001). Production lines are usually designed without any
redundancy except for situations, where extremely high requirements are
laid on the safety of the system (Birolini, 1999). Basic reliability
model of such systems has usually the form of series system when
expressed by conventional reliability block diagram. High number of
elements in serial layout has destroying effect on the overall
reliability even in case of excellent reliability of individual element.
Conventional reliability model gives conservative estimate of the global
reliability of the complete system. Moreover, individual components are
in most cases modelled as two state elements which are either fully
functional or in failure. However, real subsystems of technical systems
may admit many intermediate partially functional states between the two
extremes (Papazoglou, 1998). This is manifested by the existence of
several different failure modes and failure mechanisms that contribute
to the loss of functionality. Another obvious fact is, that complex
systems are sufficiently robust in withstanding the failure of those
subsystems, that are not absolutely vital for their functionality
(Kececioglu, 2002a; Dekys et al., 2004).
[FIGURE 1 OMITTED]
More realistic alternative to conventional analysis are methods,
which allow for multi-state nature of elements and subsystems, resulting
in less conservative and more realistic reliability estimates. In this
paper elements of simple pneumatic productive system are modelled via
Markov process to allow for multi-state nature of the possible failure
mechanism. Numerical results demonstrate slight improvement over the
conventional analysis.
2. MULTISTATE FAILURE MODEL
Let us consider the textbook example of simple pneumatic production
system, see Fig. 1. To simplify the analysis, the pneumatic press is
decomposed to two subsystems. Connecting links and the air supply are
neglected in our simplified analysis. First subsystem is the pair of
identical 3/2 valves with pushbuttons (marked as 3 in Fig. 1), the
second one is the linear actuator together with the controlling 5/2
valve buttons (marked as 1 and 2, respectively, in Fig. 1). The valve of
the first subsystem is required to be open while the push-button is
pressed by the operator and to be closed when push-button released.
Internal state of the push-button should be changed due to the action of
the operator and the valve should react appropriately. Possible states
of the first subsystem under above simplifications are summarised in
Table 1 together with the evaluation of the functionality of the system.
Bracketed values at the second column and rows 6 and 7 are
acceptable, when spurious opening or spurious closure of the valve is
acceptable. Typical case would be a single mission system. If many
cycles of steady faultless operation are required, then the values in
bracket should be refused. States of the first subsystem can be defined
as follows:
STATE 1: Nr.1 &2 (fully functional system)
STATE 2: Nr. 6 & 7 (failed valve and push-button)
STATE 3: Nr. 5 & 8 (failed push-button)
STATE 4: Nr. 3 & 4 (failed valve).
To set up the corresponding Markov process, the transition
probabilities between states are to be introduced. For system without
repairs the appropriate failure rates are for assumed failure modes as
follows:
[[lambda].sub.13]--failure rate of the push-button
[[lambda].sub.14]--failure rate of the valve
[[lambda].sub.42]--failure rate of the push-button after the valve
failed
[[lambda].sub.32]--failure rate of the valve after push-button
failed
[[lambda].sub.12]--failure rate because of unspecified cause.
[FIGURE 2 OMITTED]
We remind, that failure rates [[lambda].sub.ij] express the
conditional probabilities ([[lambda].sub.ij] [DELTA]t) of the occurence
of a failure between time t and t + [DELTA]t provided that failure did
not happen until time t.
3. NUMERICAL RESULTS
Markovian model corresponding to state diagram in Fig. 2 results in
Chapman-Kolmogorov differential equations (Birolini, 1999; Kececioglu,
2002b), which are a set of four coupled first order linear differential
equations for probabilities [P.sub.i](t) of states i=1,2,3,4.
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII]
The Chapman-Kolmogorov system was solved by direct numerical
integration for initial conditions
[P.sub.1](0) = 1, [P.sub.2](0) = 0, [P.sub.3] (0) = 0, [P.sub.4]
(0) = 0,
and for transient probabilities [[lambda].sub.13] =
[[lambda].sub.42] = 0.1 [10.sup.-6], [[lambda].sub.14] =
[[lambda].sub.32] = 0.9 [10.sup.-6] and [[lambda].sub.12] = 0.09
[10.sup.-6] estimated ad hoc according to data given in (Smith, 2001).
Fig. 3 shows probabilities [P.sub.1](t), [P.sub.1](t) + [P.sub.2](t),
[P.sub.1](t) + [P.sub.2](t) + [P.sub.3](t) and [P.sub.1](t) +
[P.sub.2](t) + [P.sub.3](t) ) + [P.sub.4](t)=1 as they are changing with
the time. For convenience the time scale is running in thousands of
hours and the transient probabilities [[lambda].sub.ij] are given in
failures per million hours.
[FIGURE 3 OMITTED]
[FIGURE 4 OMITTED]
The thick curve in Fig. 4 corresponds to the traditional
reliability function [P.sub.1](t), thin line gives [P.sub.2](t), lower
dashed curve is the [P.sub.3](t) and the upper long dashed curve
corresponds to the time dependence of the probability [P.sub.4](t) of
state 4. These illustrative results demonstrate that allowing for
multi-states has the potential of increasing the conservative estimate
of reliability of systems. The formulation the Markov process for the
second subsystem is not treated here, as it is a complete analogy of the
first subsystem except for different numerical values of transitional
probabilities.
4. CONCLUSION
The present paper demonstrates the usefullness of treating the
components of pneumatic systems as multi-state elements. For properly
defined states and corresponding transition probabilities it is possible
to set up Markov process leading to Chapman-Kolmogorov equations. Key
element of such analysis is the realistic definition of individual
states, which is always highly dependent on detailed knowledge of actual
failure modes of the system under consideration. Due to lack of detailed
experimental data future research might be focused on development of
consistent methods to estimate the transitional probabilities.
The author greatly acknowledges the financial support for this work
by the research projects KEGA-2/4154/06 and AV-4/0102/06
5. REFERENCES
Birolini, A. (1999). Reliability Engineering. Theory and Practice.
3rd Edition, Springer-Verlag, ISBN 3-540-663851, Berlin
Dekys, V.; Saga, M. & Zmindak, M. (2004). Dynamika a
spol'ahlivost' mechanickych sustav, VTS ZU, ISBN 80969165-2-1,
Zilina
Kececioglu, D. (2002a). Reliability Engineering Handbook Vol. 1,
DEStech Publications, ISBN 1-932078-00-2, Lancaster, USA
Kececioglu, D. (2002b). Reliability Engineering Handbook Vol. 2,
DEStech Publications, ISBN 1-932078-01-2, Lancaster, USA
Papazoglou, I. A. (1998). Functional Block Diagrams and Automated
Construction of Event Trees. Reliability Engineering and System Safety,
Vol. 61, pp. 185-214
Smith, D. J. (2001). Reliability, Maintainability and Risk.
Practical Methods for Engineers, 6th Edition, Butterworth Heinemann,
ISBN 0-7506-5168-7, Oxford
Tab 1. Possible states of 3/2 valve.
Nr. Functionality Operator's Button's Valve
of the system action state opened
1 1 1 1 1
2 1 0 0 0
3 0 0 0 1
4 0 1 1 0
5 0 1 0 0
6 0 (1) 1 0 1
7 0 (1) 0 1 0
8 0 0 1 1