<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJS</journal-id><journal-title-group><journal-title>Open Journal of Statistics</journal-title></journal-title-group><issn pub-type="epub">2161-718X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojs.2014.411091</article-id><article-id pub-id-type="publisher-id">OJS-52863</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Comparison of Rectangular and Elliptical Control Region EWMA Schemes for Joint Quality Monitoring
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>M. Razmy</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>T.</surname><given-names>S. G. Peiris</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Mathematical Sciences, Faculty of Engineering, University of Moratuwa, Moratuwa, Sri Lanka</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematical Sciences, Faculty of Applied Sciences, South Eastern University of Sri Lanka, Sammanthurai, Sri Lanka</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>amrazmy@seu.ac.lk(.MR)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>12</month><year>2014</year></pub-date><volume>04</volume><issue>11</issue><fpage>970</fpage><lpage>976</lpage><history><date date-type="received"><day>4</day>	<month>October</month>	<year>2014</year></date><date date-type="rev-recd"><day>2</day>	<month>November</month>	<year>2014</year>	</date><date date-type="accepted"><day>18</day>	<month>November</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The exponential weighted moving average technique used in process mean and variance monitoring charts was combined by Gan in 1997 and proposed two combined joint monitoring schemes one with rectangular control region and the other with elliptical control region. Performance of these two schemes may very depend on the shifts in mean or variance to be detected quickly. In this paper, performances of these two schemes are evaluated with respect to the average run length properties. The results reveal that elliptical scheme is little faster in detecting the shifts in process mean and increase in variance within a limit.
 
</p></abstract><kwd-group><kwd>Average Run Length</kwd><kwd> Exponential Weighted Moving Average</kwd><kwd> Joint Monitoring</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Exponential weighted moving average (EWMA) chart for monitoring a shift in process mean was introduced by Roberts in 1959 and the design procedure of EWMA mean charts was reported by Crowder in 1989 [<xref ref-type="bibr" rid="scirp.52863-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.52863-ref2">2</xref>] . Later Chang and Gan showed that EWMA chart can also be used to monitor the sample variance [<xref ref-type="bibr" rid="scirp.52863-ref3">3</xref>] . However, Gan emphasized the importance of jointly monitoring the mean and variance, as that process monitoring is a bivariate problem [<xref ref-type="bibr" rid="scirp.52863-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.52863-ref5">5</xref>] . The current practice of joint monitoring scheme consists of a mean and a variance chart to look a bivariate problem using two univariate procedures. Two combined joint monitoring schemes using EWMA charts with a rectangular control region (EE<sub>r</sub>) and an elliptical control region (EE<sub>e</sub>) were proposed by Gan [<xref ref-type="bibr" rid="scirp.52863-ref4">4</xref>] . When there is more than one scheme for joint monitoring, it is needed to compare the performances of the schemes under different scenarios. The performance of individual EWMA chart was studied using its run length distribution by Crowder, Lucas and Saccucci [<xref ref-type="bibr" rid="scirp.52863-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.52863-ref7">7</xref>] . In this paper the performance of the EE<sub>r</sub> and EE<sub>e</sub> schemes is evaluated different scenarios based on average run length (ARL) properties. ARL is defined as the average number of samples taken until an out-of-control signal is issued in quality control schemes.</p></sec><sec id="s2"><title>2. Methodology</title><p>An EWMA chart for monitoring the sample mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x5.png" xlink:type="simple"/></inline-formula> is obtained by plotting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x6.png" xlink:type="simple"/></inline-formula> against the sample number t<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x7.png" xlink:type="simple"/></inline-formula>, where E<sub>0</sub> is usually set at target mean &#181;<sub>0</sub>, l<sub>E</sub> is a constant such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x8.png" xlink:type="simple"/></inline-formula> and it is selected based on the shift in the mean to be detected quickly. An out-of-control signal is issued if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x9.png" xlink:type="simple"/></inline-formula> where H<sub>E</sub> and h<sub>E</sub> are the upper control limit and lower control limit respectively. The EWMA chart for monitoring the sample variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x10.png" xlink:type="simple"/></inline-formula> can be obtained by plotting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x11.png" xlink:type="simple"/></inline-formula> against the sample number t, where e<sub>0</sub> is usually set at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x12.png" xlink:type="simple"/></inline-formula>, l<sub>e</sub> is a positive constant such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x13.png" xlink:type="simple"/></inline-formula> and it is selected based on the shift in the variance to be detected quickly. An out-of-control signal is issued if e<sub>t</sub> is greater than the H<sub>e</sub> or e<sub>t</sub> is less than the h<sub>e</sub>. H<sub>e</sub> and h<sub>e</sub> are the upper and lower control limits respectively for the EWMA variance chart.</p><p>In the EE<sub>r</sub> scheme, EWMA mean chart and the EWMA variance chart are combined by plotting the EWMA of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x14.png" xlink:type="simple"/></inline-formula> against the EWMA of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x15.png" xlink:type="simple"/></inline-formula>. The upper and lower control limits of the two charts form four sides of a rectangular control region. In EE<sub>e</sub> scheme, the distance from the point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x16.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x17.png" xlink:type="simple"/></inline-formula>will decide whether a point falls inside the elliptical control region or not. This distance is calculated using Hotelling type statistics T<sup>2</sup> for each sample. The quantity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x18.png" xlink:type="simple"/></inline-formula> for a point in which e<sub>t</sub> is greater than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x19.png" xlink:type="simple"/></inline-formula> is given as</p><disp-formula id="scirp.52863-formula575"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1240446x20.png"  xlink:type="simple"/></disp-formula><p>and for a point in which e<sub>t</sub> is less than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x22.png" xlink:type="simple"/></inline-formula>is given as</p><disp-formula id="scirp.52863-formula576"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1240446x23.png"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig1">Figure 1</xref> illustrates the difference between the rectangular and elliptical control regions in which point B is an in-control point with respect to the EE<sub>r</sub> scheme, but it is an out-of control point with respect to the EE<sub>e</sub> scheme. Similarly, point A is an out-of-control point with respect to the EE<sub>r</sub> scheme, but it is an in-control point with respect to the EE<sub>e</sub> scheme. In process monitoring, both the magnitude of the shift and the direction are important and therefore it advisable to plot the individual samples.</p><p>Simulated data set were used for comparing the performance of the two combined schemes. For this simulation, the in-control mean (&#181;<sub>0</sub>) and variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x24.png" xlink:type="simple"/></inline-formula> are assumed to be 0 and 1 respectively with sample size 5. This means each sample comprises 5 normally distributed observations. The optimal parameters for constructing these schemes were obtained for two commonly used ARLs 250 and 370 and rechecked by simulation performed in SAS using proc RANNO. Simulations were run until the standard error of the ARL was less than 1% of the pre-specified ARL. The control chart parameters of these two schemes for in-control ARL’s of 250 and 370 are given in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The performances of the schemes are compared based on out of control ARLs when there is a shift in mean or variance or in both. Schemes detect various magnitudes of shifts in mean and variance based on their sensitivities. The scheme which gives smaller ARL when there is a shift in mean or variance is the better scheme. The shifts in mean and variance investigated are given by</p><disp-formula id="scirp.52863-formula577"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1240446x25.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.52863-formula578"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1240446x26.png"  xlink:type="simple"/></disp-formula><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Control Chart parameters for the EE<sub>r</sub> and EE<sub>e</sub> schemes in a steady state when ARL = 250, 370 and n = 5</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Scheme</th><th align="center" valign="middle" >Control Region</th><th align="center" valign="middle" >Control Chart Parameters ARL = 250</th><th align="center" valign="middle" >Control Chart Parameters ARL = 370</th></tr></thead><tr><td align="center" valign="middle" >EE<sub>r</sub></td><td align="center" valign="middle" >Rectangular</td><td align="center" valign="middle" >l<sub>E</sub> = 0.134, E<sub>0</sub> =0 H<sub>E</sub> = 0.345, h<sub>E</sub> = −0.345 l<sub>e</sub> = 0.106, e<sub>0</sub> = −0.270 H<sub>e</sub> = 0.215, h<sub>e</sub> = −0.867</td><td align="center" valign="middle" >l<sub>E</sub> = 0.120, E<sub>0</sub> = 0 H<sub>E</sub> = 0.3385, h<sub>E</sub> = −0.3385 l<sub>e</sub> = 0.100, e<sub>0</sub> = −0.270 H<sub>e</sub> = 0.2205, h<sub>e</sub> = −0.8772</td></tr><tr><td align="center" valign="middle" >EE<sub>e</sub></td><td align="center" valign="middle" >Elliptical</td><td align="center" valign="middle" >l<sub>E</sub> = 0.134, E<sub>0</sub> = 0 H<sub>E</sub> = 0.372, h<sub>E</sub> = −0.372 l<sub>e</sub> = 0.106, e<sub>0</sub> = −0.270 H<sub>e</sub> = 0.250, h<sub>e</sub> = −0.92</td><td align="center" valign="middle" >l<sub>E</sub> = 0.120, E<sub>0</sub> = 0 H<sub>E</sub> = 0.3722, h<sub>E</sub> = −0.3722 l<sub>e</sub> = 0.100, e<sub>0</sub> = −0.270 H<sub>e</sub> = 0.2540, h<sub>e</sub> = −0.8994</td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Rectangular and elliptical control regions of the combined EWMA schemes</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1240446x27.png"/></fig><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x28.png" xlink:type="simple"/></inline-formula> The process is in-con- trol when ∆ = 0.0 and δ = 1.00 and otherwise the process has changed. For each scheme and each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x29.png" xlink:type="simple"/></inline-formula>combination 1,000,000 runs were performed to estimate the out-of-control ARL. The standard deviations of run length (SDRL) values were ensured that SDRL were less than 1% of the estimated ARL. For making the comparison, a comparison efficiency index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x30.png" xlink:type="simple"/></inline-formula> is introduced:</p><disp-formula id="scirp.52863-formula579"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1240446x31.png"  xlink:type="simple"/></disp-formula><p>where,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x32.png" xlink:type="simple"/></inline-formula>= Comparative efficiency of a scheme for ∆ shift in mean and δ shift in variance;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x33.png" xlink:type="simple"/></inline-formula>= ARL for ∆ shift in mean and δ shift in variance;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x34.png" xlink:type="simple"/></inline-formula>= Minimum ARL observed among EE<sub>r</sub> and EE<sub>e</sub> schemed for a ∆ shift in mean and a δ shift in variance for particular in-control ARL.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p><xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref> shows the out-of-control ARLs for different magnitudes of shifts in mean and variance for in-control ARLs of 250 and 370. <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref> compare the efficiency of the two schemes using the index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x35.png" xlink:type="simple"/></inline-formula>. According to the <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref>, in general, the EE<sub>r</sub> scheme performs very similar with EE<sub>e</sub> scheme. <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref> shows when δ &gt; 1, EE<sub>e</sub> scheme detect the shifts quicker than the EE<sub>r</sub> scheme. However this property is lost when ∆ &gt; 1.5 but it does not harm because after ∆ &gt; 1.5 both schemes detect the shifts very quickly. When δ &lt; 1, EE<sub>e</sub> scheme gives larger out-of-control ARLs compare to the EE<sub>r</sub> scheme and therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x36.png" xlink:type="simple"/></inline-formula> index for EE<sub>e</sub> scheme is smaller compare to EE<sub>r</sub> scheme. This is a good property because decrease in variance is always favored. The design procedure of these schemes can be introduced through software for industrial use so that it can be a readymade scheme.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Average run lengths of combined schemes with respect to the process mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x37.png" xlink:type="simple"/></inline-formula> and standard deviation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x38.png" xlink:type="simple"/></inline-formula>. In-control ARL = 250</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x39.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x40.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >EE<sub>r</sub></th><th align="center" valign="middle" >EE<sub>e</sub></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x41.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x42.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >EE<sub>r</sub></th><th align="center" valign="middle" >EE<sub>e</sub></th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.80</td><td align="center" valign="middle" >6.33</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.70</td><td align="center" valign="middle" >4.95</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >21.90</td><td align="center" valign="middle" >24.57</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >9.66</td><td align="center" valign="middle" >8.58</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >235.44</td><td align="center" valign="middle" >252.32</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >10.19</td><td align="center" valign="middle" >10.64</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >250.00</td><td align="center" valign="middle" >250.00</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >10.14</td><td align="center" valign="middle" >10.55</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >136.53</td><td align="center" valign="middle" >129.33</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >10.04</td><td align="center" valign="middle" >10.25</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >67.70</td><td align="center" valign="middle" >63.44</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >9.86</td><td align="center" valign="middle" >9.78</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >18.89</td><td align="center" valign="middle" >18.13</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >8.74</td><td align="center" valign="middle" >8.04</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.17</td><td align="center" valign="middle" >7.9</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >6.40</td><td align="center" valign="middle" >5.83</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.57</td><td align="center" valign="middle" >2.47</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.52</td><td align="center" valign="middle" >2.41</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.79</td><td align="center" valign="middle" >6.27</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >4.89</td><td align="center" valign="middle" >4.05</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >21.75</td><td align="center" valign="middle" >22.6</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >5.66</td><td align="center" valign="middle" >5.49</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >134.57</td><td align="center" valign="middle" >135.1</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >5.74</td><td align="center" valign="middle" >6.03</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >128.94</td><td align="center" valign="middle" >128.88</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5.75</td><td align="center" valign="middle" >6.03</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >88.34</td><td align="center" valign="middle" >83.03</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >5.97</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >53.72</td><td align="center" valign="middle" >49.33</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >5.88</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >18.02</td><td align="center" valign="middle" >16.96</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >5.66</td><td align="center" valign="middle" >5.46</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.08</td><td align="center" valign="middle" >7.75</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >4.6</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.57</td><td align="center" valign="middle" >2.46</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.46</td><td align="center" valign="middle" >2.34</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.79</td><td align="center" valign="middle" >6.05</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >2.59</td><td align="center" valign="middle" >2.48</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >20.46</td><td align="center" valign="middle" >18.43</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >2.71</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >51.56</td><td align="center" valign="middle" >52.17</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >2.63</td><td align="center" valign="middle" >2.77</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >48.54</td><td align="center" valign="middle" >49.24</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" >2.77</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >41.48</td><td align="center" valign="middle" >39.89</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" >2.77</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >32.82</td><td align="center" valign="middle" >30.27</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >2.65</td><td align="center" valign="middle" >2.77</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >15.83</td><td align="center" valign="middle" >14.56</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >2.68</td><td align="center" valign="middle" >2.75</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >7.83</td><td align="center" valign="middle" >7.42</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >2.71</td><td align="center" valign="middle" >2.68</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.56</td><td align="center" valign="middle" >2.46</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.16</td><td align="center" valign="middle" >2.03</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.79</td><td align="center" valign="middle" >5.74</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >16.90</td><td align="center" valign="middle" >14.07</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >24.43</td><td align="center" valign="middle" >25.13</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >23.69</td><td align="center" valign="middle" >24.41</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >22.20</td><td align="center" valign="middle" >21.92</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >20.08</td><td align="center" valign="middle" >18.95</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >13.17</td><td align="center" valign="middle" >11.98</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >7.44</td><td align="center" valign="middle" >6.95</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.55</td><td align="center" valign="middle" >2.44</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Average run lengths of combined schemes with respect to the process mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x43.png" xlink:type="simple"/></inline-formula> and standard deviation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x44.png" xlink:type="simple"/></inline-formula>. In-control ARL = 370</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x45.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x46.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >EE<sub>r</sub></th><th align="center" valign="middle" >EE<sub>e</sub></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x47.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1240446x48.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >EE<sub>r</sub></th><th align="center" valign="middle" >EE<sub>e</sub></th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >6.23</td><td align="center" valign="middle" >6.45</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >6.16</td><td align="center" valign="middle" >5.18</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >24.37</td><td align="center" valign="middle" >24.63</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >10.54</td><td align="center" valign="middle" >9.31</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >331.51</td><td align="center" valign="middle" >310.88</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >11.09</td><td align="center" valign="middle" >11.81</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >370.07</td><td align="center" valign="middle" >370.0</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >10.98</td><td align="center" valign="middle" >11.84</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >186.01</td><td align="center" valign="middle" >185.27</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >10.88</td><td align="center" valign="middle" >11.53</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >84.16</td><td align="center" valign="middle" >81.51</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >10.75</td><td align="center" valign="middle" >10.99</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >21.22</td><td align="center" valign="middle" >20.56</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >9.62</td><td align="center" valign="middle" >8.94</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.89</td><td align="center" valign="middle" >8.67</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >6.98</td><td align="center" valign="middle" >6.39</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.76</td><td align="center" valign="middle" >2.67</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.72</td><td align="center" valign="middle" >2.6</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >6.24</td><td align="center" valign="middle" >6.38</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >5.3</td><td align="center" valign="middle" >4.31</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >24.35</td><td align="center" valign="middle" >22.98</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >6.12</td><td align="center" valign="middle" >6.01</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >176.66</td><td align="center" valign="middle" >169.82</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >6.21</td><td align="center" valign="middle" >6.68</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >166.54</td><td align="center" valign="middle" >175.29</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >6.23</td><td align="center" valign="middle" >6.7</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >112.41</td><td align="center" valign="middle" >110.38</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >6.23</td><td align="center" valign="middle" >6.64</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >65.66</td><td align="center" valign="middle" >61.8</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >6.23</td><td align="center" valign="middle" >6.56</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >20.14</td><td align="center" valign="middle" >19.15</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >6.15</td><td align="center" valign="middle" >6.04</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.83</td><td align="center" valign="middle" >8.53</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >5.5</td><td align="center" valign="middle" >5.04</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.77</td><td align="center" valign="middle" >2.68</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" >2.52</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >6.27</td><td align="center" valign="middle" >6.2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >2.85</td><td align="center" valign="middle" >2.75</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >22.89</td><td align="center" valign="middle" >19.06</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >2.83</td><td align="center" valign="middle" >2.99</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >59.98</td><td align="center" valign="middle" >62.22</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >2.84</td><td align="center" valign="middle" >3.05</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >56.58</td><td align="center" valign="middle" >61.13</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2.84</td><td align="center" valign="middle" >3.06</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >47.87</td><td align="center" valign="middle" >48.81</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >2.85</td><td align="center" valign="middle" >3.05</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >38.21</td><td align="center" valign="middle" >35.85</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >2.86</td><td align="center" valign="middle" >3.05</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >17.7</td><td align="center" valign="middle" >16.33</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >2.88</td><td align="center" valign="middle" >3.01</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.52</td><td align="center" valign="middle" >8.13</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >2.93</td><td align="center" valign="middle" >2.91</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.77</td><td align="center" valign="middle" >2.66</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.34</td><td align="center" valign="middle" >2.2</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >6.23</td><td align="center" valign="middle" >5.9</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.75</td><td align="center" valign="middle" >18.84</td><td align="center" valign="middle" >14.94</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >27.13</td><td align="center" valign="middle" >29.11</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >26.29</td><td align="center" valign="middle" >28.42</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >24.81</td><td align="center" valign="middle" >25.55</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >22.6</td><td align="center" valign="middle" >21.85</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >14.63</td><td align="center" valign="middle" >13.36</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >8.12</td><td align="center" valign="middle" >7.57</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.75</td><td align="center" valign="middle" >2.64</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> E<sub>∆,δ</sub> index to compare the efficiency of EE<sub>r</sub> and EE<sub>e</sub> schemes when in-control ARL = 250</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1240446x49.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> E<sub>∆,δ</sub> index to compare the efficiency of EE<sub>r</sub> and EE<sub>e</sub> schemes when in-control ARL = 370</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1240446x50.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>In overall the EE<sub>e</sub> scheme is faster than the EE<sub>r</sub> scheme in detecting the shifts in process mean and variance but the design procedure of EE<sub>e</sub> scheme is little complex due to its complex equations. Further less variance is signaled slowly in the EE<sub>e</sub> schemes compare to EE<sub>r</sub> scheme which is a preferred characteristic. Therefore EE<sub>e</sub> scheme outperformed the EE<sub>r</sub> scheme.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by the South Eastern University of Sri Lanka and the Higher Education for the Twenty First Century Project, Sri Lanka [SEUSL/O-AS/N1].</p></sec></body><back><ref-list><title>References</title><ref id="scirp.52863-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Roberts, S.W. (1959) Control Chart Tests Based on Geometric Moving Averages. Technometrics, 1, 239-250.  
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