5 COMPUTATIONAL RESULTS
Zhang (2000) estimated these ARLs at
0, 0.5, 1,
2 and 3.0 in units of
X
on simulations utilizing at
least 4,000 realizations from the AR(1) processes
with
= 0.25, 0.5, 0.75 and 0.9. In contrast
to the proposed methodology, we do the same
parameter combinations in Zhang’s studies. The
results are listed in Table II for
>0 and in Table III
for
<0.
As indicated in Table II, it is clear that when the
process is positively autocorrelated, the ARLs of our
computational results are in agreement with those
obtained by Zhang’s simulation results. Let the
relative difference (r.d.) represent the difference
between Zhang’s results and those obtained by the
proposed method. Table II also shows that when
mean shifts are small and
is large, the simulation
results deviate more from the computational results.
This phenomenon indicates that due to the inflation
of
2
t
z
, the larger the
, the more simulation runs
are required.
As indicated in Table III, it is clear that when the
process is negatively autocorrelated, the ARLs are
also in agreement with Zhang’s results. Table III
also shows an interesting phenomenon: when
becomes increasingly negative and large, the
EWMAST chart becomes more sensitive. This
property is completely opposite to a positive
autocorrelated process. As for the r.d. index, we can
also observe that the results of a simulation with few
realizations results in an unstable estimate of ARL,
especially in the case of an in-control situation with
highly correlated data.
6 CONCLUSIONS
In this research, the performance of an EWMAST
chart has been investigated for various parameter
settings when the AR(1) process is utilized. These
results demonstrate guidelines for parameter (
, L)
selection when the in-control ARL and the
autogressive parameter are specified. A numerically
analytical expression was also used to evaluate the
ARLs of the EWMAST chart, in the important
special case of an autocorrelated process.
Importantly, this method enables the assessment of
the run-length distribution of an EWMAST chart
using underlying data from an AR(1) process. For an
application of the results, the ARL algorithm can be
extended to calculate run-length distribution and
ARLs for other stationary-process data with
determined parameters. Although these results are
relatively narrow in scope when compared to the
results in Lucas and Saccucci (1990), they are still
helpful to the operator for setting parameters when
using an EWMAST chart. As for the other
requirements of in-control ARLs and the different
values listed in Table I, a larger table covering a
wider range of ARL values is available from the
authors on request.
ACKNOWLEDGEMENTS
The authors wish to express their appreciation for
the financial support by National Sciences Council
of the Republic of China, Grant No NSC 102-2221-
E-212-018, MOST 103-2221-E-343 -002, NSC 101-
2221-E-007-045-MY3 and Da-Yeh University,
Taiwan,
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