
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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