<?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.2016.62022</article-id><article-id pub-id-type="publisher-id">OJS-65865</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>
 
 
  Bias and Mean Square Error of Reliability Estimators under the One and Two Random Effects Models: The Effect of Non-Normality
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ohamed</surname><given-names>M. Shoukri</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tusneem</surname><given-names>Al-Hassan</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Michael</surname><given-names>DeNiro</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abdelmoneim</surname><given-names>El Dali</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Futwan</surname><given-names>Al-Mohanna</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Biostatistics, Epidemiology and Scientific Computing, King Faisal Specialist Hospital and 
Research Center, Riyadh, Saudi Arabia</addr-line></aff><aff id="aff2"><addr-line>The Oncology Center, King Faisal Specialist Hospital and Research Center, Riyadh, Saudi Arabia</addr-line></aff><aff id="aff4"><addr-line>Al-Faisal University College of Medicine, Riyadh, Saudi Arabia</addr-line></aff><aff id="aff1"><addr-line>Department of Cell Biology, King Faisal Specialist Hospital and Research Center, Riyadh, Saudi Arabia</addr-line></aff><pub-date pub-type="epub"><day>12</day><month>04</month><year>2016</year></pub-date><volume>06</volume><issue>02</issue><fpage>254</fpage><lpage>273</lpage><history><date date-type="received"><day>14</day>	<month>February</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>23</month>	<year>April</year>	</date><date date-type="accepted"><day>26</day>	<month>April</month>	<year>2016</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 coefficient of reliability is often estimated from a sample that includes few subjects. It is therefore expected that the precision of this estimate would be low. Measures of precision such as bias and variance depend heavily on the assumption of normality, which may not be tenable in practice. Expressions for the bias and variance of the reliability coefficient in the one and two way random effects models using the multivariate Taylor’s expansion have been obtained under the assumption of normality of the score (Atenafu et al. [1]). In the present paper we derive analytic expressions for the bias and variance, hence the mean square error when the measured responses are not normal under the one-way data layout. Similar expressions are derived in the case of the two-way data layout. We assess the effect of departure from normality on the sample size requirements and on the power of Wald’s test on specified hypotheses. We analyze two data sets, and draw comparisons with results obtained via the Bootstrap methods. It was found that the estimated bias and variance based on the bootstrap method are quite close to those obtained by the first order approximation using the Taylor’s expansion. This is an indication that for the given data sets the approximations are quite adequate.
 
</p></abstract><kwd-group><kwd>Rater’s Reliability</kwd><kwd> Random Effects Models</kwd><kwd> Multivariate Taylor’s Expansion</kwd><kwd> Wald’s Confidence  Interval</kwd><kwd> Bootstrap Methods</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Statistics is the science of transforming data into information and knowledge. Therefore producing reliable information requires error free data. Measurement errors can seriously affect statistical analysis and interpretation; it therefore becomes important to quantify the magnitude of such errors by calculating what is known as “reliability coefficient” and assessing its statistical properties. The topic of reliability has gained much attention in the literature as evidenced in the books by Dunn [<xref ref-type="bibr" rid="scirp.65865-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>] , and the recent reviews by Shoukri et al. [<xref ref-type="bibr" rid="scirp.65865-ref4">4</xref>] and Shoukri [<xref ref-type="bibr" rid="scirp.65865-ref5">5</xref>] . As a general feature of this coefficient, it must distinguish within-subject variation from variation between subjects.</p><p>A widely recognized index that possesses this property is the intraclass correlation coefficient (ICC) defined as the proportion of between-subject variation relative to the total variation. In the most frequently adopted design, k subjects are each rated by the same n raters (for inter-rater reliability). A similar approach, however, can also be adopted when a single subject is assessed repeatedly on each of several occasions (test-retest reliability), or when replicates consisting of different occasions are taken on different subjects by a single rater [<xref ref-type="bibr" rid="scirp.65865-ref6">6</xref>] . In each of these cases, and for continuous and categorical assessments, Fisher [<xref ref-type="bibr" rid="scirp.65865-ref7">7</xref>] showed that r can be estimated from an appropriate one-way analysis of variance (ANOVA).</p><p>There are numerous versions of the intraclass correlation coefficient (ICC) that can give quite different results when applied to the same data. Each form is appropriate for specific situations defined by the experimental design and the conceptual intent of the study. The differences among these forms and their applications were discussed in Shrout and Fleiss [<xref ref-type="bibr" rid="scirp.65865-ref8">8</xref>] , and McGraw and Wong [<xref ref-type="bibr" rid="scirp.65865-ref9">9</xref>] . Shrout and Fleiss [<xref ref-type="bibr" rid="scirp.65865-ref8">8</xref>] provided specific guidelines for choosing the appropriate form of the ICC by adopting two linear additive models. The fundamental question is: which appropriate statistical model for the reliability study, may be selected to address the questions of interest.</p><p>Much of the work in reliability studies focused on the estimation (point and interval), hypothesis testing, and sample size requirements to achieve certain power [<xref ref-type="bibr" rid="scirp.65865-ref10">10</xref>] and or maximizing the precision of estimation under cost constraint [<xref ref-type="bibr" rid="scirp.65865-ref11">11</xref>] .</p><p>Only recently the issue of correcting the ICC for bias, under the one-way ANOVA was investigated. Assuming the normality of the distribution of scores, Atenafu et al. [<xref ref-type="bibr" rid="scirp.65865-ref1">1</xref>] investigated the issues related to bias correction of the ANOVA estimator of ICC from the one-way layout. The authors investigated the effect of non-normality through Monte-Carlo simulations by generating data from known skewed distributions.</p><p>This article has two-fold objectives: First, under the one-way ANOVA, we evaluate the bias, the variance (and hence the mean square error) of the ICC when the assumption of normality is not tenable. We further investigate the effect of non-normality on the sample size requirements to achieve certain levels of power on specific null hypotheses on the reliability parameter for a given level of type I error. Second, under the two-way ANOVA we derive the first order approximation for the bias and the variance of the ICC. This allows for the comparison between the Wald confidence interval and other proposed confidence intervals. We analyze data of two examples using the R package.</p><p>The paper is structured as follows: In Section 2 we derive analytic expressions for bias and variance of ICC when the assumption of normality is not satisfied. In Section 3 we extend our approach to the case of two-way data layout. We obtain analytic expressions for bias and variance of ICC, and construct a Wald’s type confidence interval. Moreover we evaluate the empirical power using simulations. In Section 4 we introduce two examples and assess the accuracy of the first order approximation for bias and variance using the bootstrap technology for the two-way model. We discuss the results in Section 5.</p></sec><sec id="s2"><title>2. The Effect of Non-Normality on the Bias and Variance of the One-Way ANOVA Estimator of the Reliability Coefficient</title><p>In most interrater reliability study, each of a random sample of k subjects is rated independently by n raters. There usually are two situations that are of interest to us:</p><p>1) Each subject is rated by asset n different raters, randomly selected from a larger population of raters.</p><p>2) A random sample of n &gt; 1 raters is selected from a larger population, and each judge rates each subject, that is, each judge rates k subjects. We shall assume that the number of raters is less than the number of subjects.</p><p>Conceptually the two situations should produce close estimates of the ICC, but components of variations in the scores should appropriately be specified to avoid misspecification bias. Each of the postulated models specifies the decomposition of a rating made by the jth rater on the ith subject in terms of various effects. In this paper we consider the decomposition into subject component, rater component and random error component. Depending on the way the study is designed, different assumptions are made about the effects, and the structure of the corresponding ANOVA will be different.</p><p>We start by specifying the simplest design used to assess the reliability sets of scores; namely the one-way random effect model. Suppose that we have k subjects and we would like to take n measurements by a single device. How can we assess the consistency of the set of measurements taken from each subject? The one-way model stipulates that:</p><disp-formula id="scirp.65865-formula2549"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x6.png"  xlink:type="simple"/></disp-formula><p>The Y<sub>ij</sub> is the jth measurement taken on the ith subject, μ is the bias, b<sub>i</sub> is the subject effect, and e<sub>ij</sub> is a random measurement error, assumed independent of b<sub>i</sub> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x7.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x8.png" xlink:type="simple"/></inline-formula>. We assume that b<sub>i</sub> and e<sub>ij</sub> are mutually independent random variables. Clearly, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x10.png" xlink:type="simple"/></inline-formula>, and</p><disp-formula id="scirp.65865-formula2550"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x11.png"  xlink:type="simple"/></disp-formula><p>Therefore the reliability coefficient, or the intraclass correlation coefficient (ICC) is defined as:</p><disp-formula id="scirp.65865-formula2551"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x12.png"  xlink:type="simple"/></disp-formula><p>The reliability estimate of ρ is obtained once suitable estimate of the components of variance are obtained.</p><disp-formula id="scirp.65865-formula2552"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x13.png"  xlink:type="simple"/></disp-formula><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x14.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x15.png" xlink:type="simple"/></inline-formula> are the estimates of the corresponding variance components and are obtained either from the maximum likelihood estimation, or the one-way random effects ANOVA (<xref ref-type="table" rid="table1">Table 1</xref>).</p><p>Using the notations, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x16.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x17.png" xlink:type="simple"/></inline-formula>, the corrected sums of squares are given as:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x18.png" xlink:type="simple"/></inline-formula>,</p><p>which is the between subjects sums of squares, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x19.png" xlink:type="simple"/></inline-formula>, is the within subjects sum of squares. The total sum of squares is thus given by,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x20.png" xlink:type="simple"/></inline-formula>. Unbiased estimates of the variance components are given by:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x21.png" xlink:type="simple"/></inline-formula>.</p><p>Hence the variance components estimator of the ICC is given by:</p><disp-formula id="scirp.65865-formula2553"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x22.png"  xlink:type="simple"/></disp-formula><p>(See; Searle et al. [<xref ref-type="bibr" rid="scirp.65865-ref12">12</xref>] ).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The one-way ANOVA table</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >S.O.V.</th><th align="center" valign="middle" >DF</th><th align="center" valign="middle" >SS</th><th align="center" valign="middle" >MS</th><th align="center" valign="middle" >EMS</th></tr></thead><tr><td align="center" valign="middle" >Between subjects</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x23.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SSB</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x24.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x25.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Within subjects</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x26.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SSW</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x27.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x28.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Total</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x29.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SST</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>With the additional assumptions of normality and independence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x30.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x31.png" xlink:type="simple"/></inline-formula> we have:</p><disp-formula id="scirp.65865-formula2554"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x32.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x33.png" xlink:type="simple"/></inline-formula>.</p><p>Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x34.png" xlink:type="simple"/></inline-formula> denotes a chi-square random variable with α degrees of freedom. Using the delta method we can derive the asymptotic bias and variance of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x35.png" xlink:type="simple"/></inline-formula>. After some simplifications we can show that:</p><disp-formula id="scirp.65865-formula2555"><label>. (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x36.png"  xlink:type="simple"/></disp-formula><p>Equation (4) indicates that the estimator of the ICC from the one-way ANOVA is negatively biased for all values of, n, and ρ.</p><p>Dropping the assumptions of normality regarding the distributions of b<sub>i</sub> and e<sub>ij</sub> has two consequences:</p><p>1) The mean squares S<sub>B</sub> and S<sub>W</sub> will not have chi-square distributions.</p><p>2) The mean squares S<sub>B</sub> and S<sub>W</sub> are no longer independent, and hence the ratio of the mean squares will not have the usual F-distribution.</p><p>Relaxing the assumption of normality both the measures of Kurtosis of b<sub>i</sub> and e<sub>ij</sub> are needed in the calculation of the asymptotic variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x37.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x38.png" xlink:type="simple"/></inline-formula> and the amount of bias [<xref ref-type="bibr" rid="scirp.65865-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref14">14</xref>] .</p><p>Let δ<sub>e</sub> and δ<sub>b</sub> denote respectively the coefficients of kurtosis of e<sub>ij</sub> and b<sub>i</sub>. These quantities are defined as:</p><disp-formula id="scirp.65865-formula2556"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x39.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x40.png" xlink:type="simple"/></inline-formula>.</p><p>Using results for the balanced one way ANOVA [<xref ref-type="bibr" rid="scirp.65865-ref14">14</xref>] we have:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x41.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x42.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x43.png" xlink:type="simple"/></inline-formula>, where</p><disp-formula id="scirp.65865-formula2557"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x44.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2558"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x45.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x46.png" xlink:type="simple"/></inline-formula>.</p><p>Using the delta method, the first order approximation for the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x47.png" xlink:type="simple"/></inline-formula> is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x48.png" xlink:type="simple"/></inline-formula>.</p><p>Simplifying we get:</p><disp-formula id="scirp.65865-formula2559"><label>. (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x49.png"  xlink:type="simple"/></disp-formula><p>We shall write the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x50.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x51.png" xlink:type="simple"/></inline-formula>. Note that under normality<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x52.png" xlink:type="simple"/></inline-formula>, and in this case the variance expression reduces to variance expression given in Donner [<xref ref-type="bibr" rid="scirp.65865-ref15">15</xref>] :</p><disp-formula id="scirp.65865-formula2560"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x53.png"  xlink:type="simple"/></disp-formula><p>Using the Taylor’s expansion for the two variables case (see Appendix I) we obtain, to the first order of approximation the asymptotic bias of the ANOVA estimator of the ICC when the assumption of normality is not satisfied as:</p><disp-formula id="scirp.65865-formula2561"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x54.png"  xlink:type="simple"/></disp-formula><p>We can then evaluate the mean square error<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x55.png" xlink:type="simple"/></inline-formula>. Expressions (4) and (6) demonstrate the dependence of these quantities on the kurtosis of both the between subject and within variables. To calculate the estimated bias and variance we need not specify the complete distributions of b<sub>i</sub> and e<sub>ij</sub> but good guesses for δ<sub>b</sub> and δ<sub>e</sub> will suffice.</p><p>One question that may be stated is: which component of variation has the largest effect on the bias and variance of the reliability estimate. We answer this question empirically in two different ways. First in <xref ref-type="table" rid="table2">Table 2</xref>, we demonstrate the direct effect of the combinations of the model parameters on the bias. Subsequently, we investigate the effect of departure from normality on the sample size requirements in a typical reliability study and summarize the results in <xref ref-type="table" rid="table2">Table 2</xref>. We see from <xref ref-type="table" rid="table2">Table 2</xref> that for selected values of the parameters combination (n, k, ρ) the smallest bias occurs when δ<sub>b</sub> = δ<sub>e</sub> = 0. Larger values δ<sub>b</sub> increase the bias of the estimates of ICC and has more adverse effect on the bias than that caused by large values of δ<sub>e</sub>. The conclusion here is that, we are worse-off by miss-specifying the distribution of the between subjects effects relative to the error term distribution. We note also from Equation (6) that δ<sub>e</sub> is divided by the factor {kn} in c<sub>1</sub>, c<sub>2</sub>, and c<sub>12</sub>. The implication is that, as the number of subjects increase, the kurtosis of the error term has negligible effect on the bias and variance of the estimated reliability.</p><p>Note that the selected values for δ<sub>b</sub> and δ<sub>e</sub> are not arbitrary as it may seem. For example, if we assume that the error term {e} is a random variable that has a mixture of two normal distributions with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x56.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x57.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x58.png" xlink:type="simple"/></inline-formula> and a mixing proportions p<sub>1</sub>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x59.png" xlink:type="simple"/></inline-formula>, we can show in general that</p><disp-formula id="scirp.65865-formula2562"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x60.png"  xlink:type="simple"/></disp-formula><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Effect non-normality on bias one-way ANOVA</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >k</th><th align="center" valign="middle" >ρ</th><th align="center" valign="middle" >δ<sub>e</sub></th><th align="center" valign="middle" >δ<sub>b</sub></th><th align="center" valign="middle" >BIAS</th></tr></thead><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >−0.0460</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−0.0019</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >−0.0457</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0237</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−0.0015</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0796</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0355</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >−0.0650</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−0.0092</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >−0.0451</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >126</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−0.0024</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >126</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−0.0022</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >126</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0109</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >117</td><td align="center" valign="middle" >0.65</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0115</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >−0.0261</td></tr></tbody></table></table-wrap><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x61.png" xlink:type="simple"/></inline-formula>.</p><p>And a coefficient of kurtosis <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x62.png" xlink:type="simple"/></inline-formula> given by:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x63.png" xlink:type="simple"/></inline-formula>.</p><p>For the case, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x66.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x67.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x68.png" xlink:type="simple"/></inline-formula>, the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x69.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x70.png" xlink:type="simple"/></inline-formula>and the kurtosis will be 3.0625. This justifies our choice for the values of δ<sub>b</sub> and δ<sub>e</sub>.</p><p>As well, non-normality has an effect on the required sample size through its influence on the variance of the estimated reliability coefficient. Suppose that we need to determine the number of subjects to detect the departure from the null hypothesis <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x71.png" xlink:type="simple"/></inline-formula> in the direction of the one-sided alternative<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x72.png" xlink:type="simple"/></inline-formula>, with type-one error rate α and power<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x73.png" xlink:type="simple"/></inline-formula>. For fixed n, we have:</p><disp-formula id="scirp.65865-formula2563"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x74.png"  xlink:type="simple"/></disp-formula><p>If we set the Type I error rate at 5% and power at 80%, for given values of ρ<sub>0</sub>, ρ<sub>1</sub>, n, δ<sub>b</sub> and δ<sub>e</sub>, the estimated values of k are given in <xref ref-type="table" rid="table3">Table 3</xref>.</p><p>In this table we demonstrate the interplay between the effect size (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x75.png" xlink:type="simple"/></inline-formula>), δ<sub>b</sub>, δ<sub>e</sub>, and the required sample size. Specifically, the two red-colored rows of <xref ref-type="table" rid="table3">Table 3</xref> show that for the same effect size<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x76.png" xlink:type="simple"/></inline-formula>, δ<sub>b</sub> = 0, and δ<sub>e</sub> = 6, and n = 5, we need to recruit 6 subjects (see the first red row), while for the same range of values of the reliability parameter we need to recruit 21 subjects if δ<sub>b</sub> = 6, and δ<sub>e</sub> = 0 (the second red row). The worst situation when the two components of variation are far from being normal. This illustrates the impact of the departure from normality of the distribution of between subjects on the sample size requirements.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Effect of non-normality on sample size under the one-way ANOVA</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >ρ<sub>0</sub></th><th align="center" valign="middle" >ρ<sub>1</sub></th><th align="center" valign="middle" >δ<sub>e</sub></th><th align="center" valign="middle" >δ<sub>b</sub></th><th align="center" valign="middle" >k</th></tr></thead><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >7</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >17</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >11</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >26</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >38</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >839</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >84</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >21</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >28</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >6.000</td><td align="center" valign="middle" >21</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.98</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >67</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >3.000</td><td align="center" valign="middle" >14</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.98</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >18</td></tr></tbody></table></table-wrap><p>In the previous section we investigated the effect of departure from normality on the bias and the sample size requirements. In the simple case of one-way design the evaluations depend on a number of parameters. In order to extend the one-way model to the more complex model of a two-way layout, we adopt the situation when a random sample of n raters is selected from a larger population, and each judge rates each subject, that is, each judge rates k subjects. We investigate the issues of bias, mean square error (as a measure of precision of the estimated reliability parameter) and the power of hypothesis testing when the scores are not normally distributed, and when the model generating the data is that of a two-way layout. Although the extension is straight forward, we have to deal with several parameters, some of them are treated as nuisance, and others are considered essential so that we can produce useful results.</p></sec><sec id="s3"><title>3. Bias and Variance of Estimating the Reliability under the Two-Way Random Effects Models</title><p>As summarized in the previous section, the sampling theory and formula for the standard error of the reliability estimates rely heavily on the normality assumptions, despite the fact that real data seldom satisfy these assumptions. At best we may expect that normality would be only approximately satisfied, and it does not logically follow, of course, that approximately satisfying the normality requirements guarantees automatic approximation of the actual distribution to the distribution given under normal theory. A similar problem exists for statistical inference in the two-way fixed model ANOVA, though it has been found that the distribution of the ratio of mean squares is quite robust with respect to non-normality under certain conditions [<xref ref-type="bibr" rid="scirp.65865-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref17">17</xref>] .</p><p>The present model is the two-way mixed model ANOVA, with one observation per cell, and the primary concern is the distribution of a function of the variance component estimates, unlike the fixed model, in which the primary concern is the location parameter estimates. Thus findings in [<xref ref-type="bibr" rid="scirp.65865-ref16">16</xref>] cannot be generalized to reliability theory without thorough investigation. In this section we consider the model:</p><disp-formula id="scirp.65865-formula2564"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x77.png"  xlink:type="simple"/></disp-formula><p>The corrected sums of squares as shown in <xref ref-type="table" rid="table4">Table 4</xref> are given as:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x78.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x79.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x80.png" xlink:type="simple"/></inline-formula>.</p><p>The total sum of squares:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x81.png" xlink:type="simple"/></inline-formula>,</p><p>where:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x82.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x83.png" xlink:type="simple"/></inline-formula>. Moreover,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x84.png" xlink:type="simple"/></inline-formula>.</p><p>It is assumed that b<sub>i</sub>, r<sub>j</sub>, and e<sub>ij</sub> are mutually stochastically independent with</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x85.png" xlink:type="simple"/></inline-formula>.</p><p>The variance of Y<sub>ij</sub> is:</p><disp-formula id="scirp.65865-formula2565"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x86.png"  xlink:type="simple"/></disp-formula><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> The ANOVA table under the two way layout</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >S.O.V.</th><th align="center" valign="middle" >DF</th><th align="center" valign="middle" >SS</th><th align="center" valign="middle" >MS</th><th align="center" valign="middle" >EMS</th></tr></thead><tr><td align="center" valign="middle" >Between subjects</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x87.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SSB</td><td align="center" valign="middle" >SB</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x88.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Within subjects</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x89.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SSR</td><td align="center" valign="middle" >SR</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x90.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Error</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x91.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >SSE</td><td align="center" valign="middle" >SE</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x92.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Total</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x93.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >TSS</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>and the covariance between two measurements on the same subject, taken by the jth and j’th raters, is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x94.png" xlink:type="simple"/></inline-formula>.</p><p>Under the above set-up, we have:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x95.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x96.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x97.png" xlink:type="simple"/></inline-formula>.</p><p>Hence, under this model, the appropriate intraclass correlation to measure interrater reliability becomes:</p><disp-formula id="scirp.65865-formula2566"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x98.png"  xlink:type="simple"/></disp-formula><p>Under the assumption of normality the second, third central moments of mean squares SB, SR, and SE are given <xref ref-type="table" rid="table5">Table 5</xref>.</p><p>Define, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x99.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x100.png" xlink:type="simple"/></inline-formula>. The ICC is thus written as:</p><disp-formula id="scirp.65865-formula2567"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x101.png"  xlink:type="simple"/></disp-formula><p>The variance components estimator of the ICC, using the mean squares given in <xref ref-type="table" rid="table4">Table 4</xref> is:</p><disp-formula id="scirp.65865-formula2568"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x102.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x103.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x104.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x105.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x106.png" xlink:type="simple"/></inline-formula>.</p><p>Note that from (10) we can write,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x107.png" xlink:type="simple"/></inline-formula>. This means that the model will have one parameter of in-</p><p>terest, ρ<sub>2</sub>, and a nuisance parameter θ<sub>2</sub> which will be treated as fixed. Using the Taylor’s series expansion as a function of three variables, under the assumption of normality, we use the delta method and the information in <xref ref-type="table" rid="table4">Table 4</xref> to obtain expressions for the variance and bias of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x108.png" xlink:type="simple"/></inline-formula> and these are given in Appendix III. We noted from our calculations of the bias, variance and the MSE that:</p><p>1) For fixed values of θ<sub>2</sub>, k, and n, the MSE values decrease as the values of ρ<sub>2</sub> increase. For example, when k = 20, and n = 5, θ<sub>2</sub> = 0.1, and ρ<sub>2</sub> = 0.7, the MSE = 0.007. While for the same set of parameters values, but ρ<sub>2</sub> = 0.9, the MSE = 0.001. This means that the precision of the ICC estimator increases near its upper boundary. This in fact is the situation in reliability studies where high values of the ICC estimator are expected;</p><p>2) For fixed values of ρ<sub>2</sub>, k, and n, the MSE values increase (decrease in precision) as the values of θ<sub>2</sub> increase. For example, when k = 20, and n = 5, θ<sub>2</sub> = 0.1, and ρ<sub>2</sub> = 0.7, the MSE = 0.007. While for the same set of parameters values, with θ<sub>2</sub> = 0.5, the MSE = 0.009. Furthermore, when k = 20, and n = 5, θ<sub>2</sub> = 0.9, and ρ<sub>2</sub> = 0.7, the MSE = 0.011. The implication is that when the between rater’s variance relative to the error variance ratio increases, one should expect a loss in precision of the estimate of ICC.</p><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Higher moments of the corrected mean squares under the assumption of normality</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >M.S.</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x109.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x110.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x111.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >SB</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x112.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x113.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x114.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >SR</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x115.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x116.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x117.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >SE</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x118.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x119.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x120.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><sec id="s3_1"><title>3.1. Variances and Covariance under Non-Normality</title><p>Note that in this case we need an additional coefficient of kurtosis which we denote by δ<sub>r</sub> for the random effect representing raters. In his seminal paper Tukey [<xref ref-type="bibr" rid="scirp.65865-ref18">18</xref>] obtained the variance of the variance estimates under various ANOVA models by employing “polykays”. We modified Tukey’s results to fit our two-way random effect model. After some algebra we can show that:</p><disp-formula id="scirp.65865-formula2569"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x121.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2570"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x122.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2571"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x123.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2572"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x124.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2573"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x125.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x126.png" xlink:type="simple"/></inline-formula>.</p><p>To investigate the effect non-normality, we again use the Taylor’s expansion to derive expression for the variance bias, and the mean square error of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x127.png" xlink:type="simple"/></inline-formula>. See Appendix VI.</p><p>To explore the effect of non-normality on the mean square error of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x128.png" xlink:type="simple"/></inline-formula>, we consider four scenarios, and the results are summarized in <xref ref-type="table" rid="table6">Table 6</xref>, <xref ref-type="table" rid="table7">Table 7</xref>, <xref ref-type="table" rid="table8">Table 8</xref>, and <xref ref-type="table" rid="table9">Table 9</xref>. We fixed the number of subjects, the number raters, the values of the ICC and the nuisance θ<sub>2</sub>, but we varied the kurtoses of the variance components parameters. In <xref ref-type="table" rid="table6">Table 6</xref> we set δ<sub>b</sub> = 3, δ<sub>e</sub> = 0, δ<sub>r</sub> = 0, in both the variance and bias terms (Appendix IV) a scenario indicating that the between subjects component of variation is not normally distributed, in <xref ref-type="table" rid="table7">Table 7</xref> we set δ<sub>b</sub> = 0, δ<sub>r</sub> = 0, δ<sub>e</sub> = 3, a scenario indicating that only the error term is not normally distributed, in <xref ref-type="table" rid="table8">Table 8</xref> we set δ<sub>b</sub> = 0, δ<sub>e</sub> = 0, δ<sub>r</sub> = 3, indicating that the between raters component of variation is not normally distributed. <xref ref-type="table" rid="table9">Table 9</xref> summarizes the results when the three kurtosis parameters are set to zero (the normal case). The comparison among the four tables is restricted to variation in the MSE values (the last column in <xref ref-type="table" rid="table6">Table 6</xref>, <xref ref-type="table" rid="table7">Table 7</xref>, <xref ref-type="table" rid="table8">Table 8</xref>, and <xref ref-type="table" rid="table9">Table 9</xref>). We conclude that:</p><p>1) When the number of subjects is fairly large (k &gt; 25) and for all the parameters values, the kurtosis parameter of any of the components has minor or negligible effect on the MSE.</p><p>2) For small values of ρ<sub>2</sub> (&lt;0.4) the bias is positive, and is negative for larger values. The variation in the nuisance parameter θ<sub>2</sub> does affect the bias, the variance and ultimately the MSE. For small values of ρ<sub>2</sub>, the MSE decreases with increasing values of θ<sub>2</sub>, however, for large values of ρ<sub>2</sub>, the MSE increases with increasing values of θ<sub>2</sub>.</p><p>3) On comparing the MSE values in <xref ref-type="table" rid="table6">Table 6</xref>, <xref ref-type="table" rid="table7">Table 7</xref> and <xref ref-type="table" rid="table8">Table 8</xref> to <xref ref-type="table" rid="table9">Table 9</xref>, we find that a non-zero kurtosis δ<sub>r</sub> produces the highest MSE as compared to non-zero δ<sub>b</sub>. As we indicated the MSE values are smaller in the case of a non-zero kurtosis of the error term.</p></sec></sec><sec id="s4"><title>4. Data Analysis</title><p>In this section we analyze two data sets. Using the large sample bias and variance given in Appendix IV, we construct a Wald’s type large sample confidence:</p><disp-formula id="scirp.65865-formula2574"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1240660x129.png"  xlink:type="simple"/></disp-formula><p>Because of the lack of exact expressions, and to assess the accuracy of the proposed approximations, we</p><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> δ<sub>b</sub> = 3, δ<sub>e</sub> = 0, δ<sub>r</sub> = 0</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >k</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >ρ<sub>2</sub></th><th align="center" valign="middle" >θ<sub>2</sub></th><th align="center" valign="middle" >Bias</th><th align="center" valign="middle" >Variance</th><th align="center" valign="middle" >MSE</th></tr></thead><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01922</td><td align="center" valign="middle" >0.15451</td><td align="center" valign="middle" >0.15488</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.01050</td><td align="center" valign="middle" >0.14530</td><td align="center" valign="middle" >0.14541</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.02814</td><td align="center" valign="middle" >0.09669</td><td align="center" valign="middle" >0.09748</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.07690</td><td align="center" valign="middle" >0.02164</td><td align="center" valign="middle" >0.02755</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.01411</td><td align="center" valign="middle" >0.02808</td><td align="center" valign="middle" >0.02828</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.08968</td><td align="center" valign="middle" >0.02332</td><td align="center" valign="middle" >0.03136</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.00454</td><td align="center" valign="middle" >0.07236</td><td align="center" valign="middle" >0.07238</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00291</td><td align="center" valign="middle" >0.06695</td><td align="center" valign="middle" >0.04374</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.02943</td><td align="center" valign="middle" >0.04288</td><td align="center" valign="middle" >0.06101</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01340</td><td align="center" valign="middle" >0.00309</td><td align="center" valign="middle" >0.00327</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.01761</td><td align="center" valign="middle" >0.00387</td><td align="center" valign="middle" >0.00418</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.02033</td><td align="center" valign="middle" >0.00736</td><td align="center" valign="middle" >0.00777</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.01232</td><td align="center" valign="middle" >0.00160</td><td align="center" valign="middle" >0.00175</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.01704</td><td align="center" valign="middle" >0.00258</td><td align="center" valign="middle" >0.00287</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.02059</td><td align="center" valign="middle" >0.00705</td><td align="center" valign="middle" >0.00747</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00429</td><td align="center" valign="middle" >0.00061</td><td align="center" valign="middle" >0.00062</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00517</td><td align="center" valign="middle" >0.00111</td><td align="center" valign="middle" >0.00114</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00259</td><td align="center" valign="middle" >0.00121</td><td align="center" valign="middle" >0.00122</td></tr></tbody></table></table-wrap><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> δ<sub>b</sub> = 0, δ<sub>r</sub> = 0, δ<sub>e</sub> = 3</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >k</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >ρ<sub>2</sub></th><th align="center" valign="middle" >θ<sub>2</sub></th><th align="center" valign="middle" >Bias_RO2</th><th align="center" valign="middle" >Var_RO2</th><th align="center" valign="middle" >MSE</th></tr></thead><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.10490</td><td align="center" valign="middle" >0.12162</td><td align="center" valign="middle" >0.13262</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.09409</td><td align="center" valign="middle" >0.11278</td><td align="center" valign="middle" >0.12164</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.04242</td><td align="center" valign="middle" >0.07346</td><td align="center" valign="middle" >0.07526</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.02304</td><td align="center" valign="middle" >0.01569</td><td align="center" valign="middle" >0.01622</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.02898</td><td align="center" valign="middle" >0.01602</td><td align="center" valign="middle" >0.01686</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.03936</td><td align="center" valign="middle" >0.03181</td><td align="center" valign="middle" >0.03336</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.04597</td><td align="center" valign="middle" >0.06213</td><td align="center" valign="middle" >0.06424</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.03874</td><td align="center" valign="middle" >0.05626</td><td align="center" valign="middle" >0.05776</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.01018</td><td align="center" valign="middle" >0.03497</td><td align="center" valign="middle" >0.03508</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00422</td><td align="center" valign="middle" >0.00230</td><td align="center" valign="middle" >0.00232</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00597</td><td align="center" valign="middle" >0.00259</td><td align="center" valign="middle" >0.00263</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00593</td><td align="center" valign="middle" >0.00554</td><td align="center" valign="middle" >0.00557</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00449</td><td align="center" valign="middle" >0.00109</td><td align="center" valign="middle" >0.00111</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00630</td><td align="center" valign="middle" >0.00161</td><td align="center" valign="middle" >0.00165</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00612</td><td align="center" valign="middle" >0.00541</td><td align="center" valign="middle" >0.00545</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00165</td><td align="center" valign="middle" >0.00031</td><td align="center" valign="middle" >0.00031</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00195</td><td align="center" valign="middle" >0.00055</td><td align="center" valign="middle" >0.00056</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00064</td><td align="center" valign="middle" >0.00076</td><td align="center" valign="middle" >0.00076</td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table8">Table 8</xref></label><caption><title> δ<sub>b</sub> = 0, δ<sub>e</sub> = 0, δ<sub>r</sub> = 3</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >k</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >ρ<sub>2</sub></th><th align="center" valign="middle" >θ<sub>2</sub></th><th align="center" valign="middle" >Bias</th><th align="center" valign="middle" >Variance</th><th align="center" valign="middle" >MSE</th></tr></thead><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.34706</td><td align="center" valign="middle" >0.27031</td><td align="center" valign="middle" >0.39076</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.31681</td><td align="center" valign="middle" >0.24705</td><td align="center" valign="middle" >0.34742</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.16019</td><td align="center" valign="middle" >0.13180</td><td align="center" valign="middle" >0.15747</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00454</td><td align="center" valign="middle" >0.03182</td><td align="center" valign="middle" >0.03184</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.01411</td><td align="center" valign="middle" >0.02808</td><td align="center" valign="middle" >0.02828</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.04406</td><td align="center" valign="middle" >0.01852</td><td align="center" valign="middle" >0.02046</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.15600</td><td align="center" valign="middle" >0.14456</td><td align="center" valign="middle" >0.16890</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.13748</td><td align="center" valign="middle" >0.12826</td><td align="center" valign="middle" >0.14716</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.05347</td><td align="center" valign="middle" >0.05815</td><td align="center" valign="middle" >0.06101</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.00107</td><td align="center" valign="middle" >0.00704</td><td align="center" valign="middle" >0.00705</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00193</td><td align="center" valign="middle" >0.00596</td><td align="center" valign="middle" >0.00596</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00709</td><td align="center" valign="middle" >0.00370</td><td align="center" valign="middle" >0.00375</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00269</td><td align="center" valign="middle" >0.00270</td><td align="center" valign="middle" >0.00271</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00511</td><td align="center" valign="middle" >0.00253</td><td align="center" valign="middle" >0.00256</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00805</td><td align="center" valign="middle" >0.00302</td><td align="center" valign="middle" >0.00308</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00118</td><td align="center" valign="middle" >0.00071</td><td align="center" valign="middle" >0.00071</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00174</td><td align="center" valign="middle" >0.00070</td><td align="center" valign="middle" >0.00071</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00102</td><td align="center" valign="middle" >0.00050</td><td align="center" valign="middle" >0.00050</td></tr></tbody></table></table-wrap><table-wrap id="table9" ><label><xref ref-type="table" rid="table9">Table 9</xref></label><caption><title> Bias and MSE of the ICC estimator under the normality assumption</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >k</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >ρ<sub>2</sub></th><th align="center" valign="middle" >θ<sub>2</sub></th><th align="center" valign="middle" >Bias</th><th align="center" valign="middle" >Variance</th><th align="center" valign="middle" >MSE</th></tr></thead><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.10483</td><td align="center" valign="middle" >0.12149</td><td align="center" valign="middle" >0.13248</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.09384</td><td align="center" valign="middle" >0.11232</td><td align="center" valign="middle" >0.12112</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.03829</td><td align="center" valign="middle" >0.06607</td><td align="center" valign="middle" >0.06754</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.02320</td><td align="center" valign="middle" >0.01535</td><td align="center" valign="middle" >0.01589</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.02956</td><td align="center" valign="middle" >0.01481</td><td align="center" valign="middle" >0.01569</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.04731</td><td align="center" valign="middle" >0.01619</td><td align="center" valign="middle" >0.01843</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.04591</td><td align="center" valign="middle" >0.06201</td><td align="center" valign="middle" >0.06412</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.03851</td><td align="center" valign="middle" >0.05584</td><td align="center" valign="middle" >0.05732</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.00682</td><td align="center" valign="middle" >0.02916</td><td align="center" valign="middle" >0.02920</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00429</td><td align="center" valign="middle" >0.00221</td><td align="center" valign="middle" >0.00222</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00619</td><td align="center" valign="middle" >0.00229</td><td align="center" valign="middle" >0.00232</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00800</td><td align="center" valign="middle" >0.00311</td><td align="center" valign="middle" >0.00317</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00455</td><td align="center" valign="middle" >0.00099</td><td align="center" valign="middle" >0.00101</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00653</td><td align="center" valign="middle" >0.00128</td><td align="center" valign="middle" >0.00133</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00825</td><td align="center" valign="middle" >0.00289</td><td align="center" valign="middle" >0.00295</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >−0.00168</td><td align="center" valign="middle" >0.00027</td><td align="center" valign="middle" >0.00027</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >−0.00205</td><td align="center" valign="middle" >0.00046</td><td align="center" valign="middle" >0.00047</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >−0.00103</td><td align="center" valign="middle" >0.00049</td><td align="center" valign="middle" >0.00049</td></tr></tbody></table></table-wrap><p>compare the results to the distribution free bootstrap techniques. Moreover we compare the approximate Wald’s confidence interval, in terms of width, with other proposed approximate confidence intervals proposed in the literature. To be specific we shall compare our results with:</p><p>1) Fleiss and Shrout [<xref ref-type="bibr" rid="scirp.65865-ref19">19</xref>] approximate confidence interval for which they applied Satterthwaite’s two-moment approximation to arrive at an approximate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x130.png" xlink:type="simple"/></inline-formula> per cent one-sided upper bound (U) and one-sided lower bound (L).</p><p>2) Capelleri JC, Ting N [<xref ref-type="bibr" rid="scirp.65865-ref20">20</xref>] modified the moments approximation initially proposed by Zou and McDermott [<xref ref-type="bibr" rid="scirp.65865-ref21">21</xref>] to obtain more accurate coverage probabilities.</p><p>3) BC<sub>a</sub> or bootstrap confidence intervals, known as the “bias corrected-bias accelerated” confidence intervals [<xref ref-type="bibr" rid="scirp.65865-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref23">23</xref>] .</p><p>We analyze the two data sets using the R-packages [<xref ref-type="bibr" rid="scirp.65865-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref25">25</xref>] (PSY), and (bootstrap). We provide the R-code for the first data set only since it is the same code needed for the second data set.</p><p>Example 1: Agreement among pathologists (see <xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>Landis and Koch [<xref ref-type="bibr" rid="scirp.65865-ref26">26</xref>] evaluated the agreement among seven who classified most involved lesion of the uterine cervix. Pathologists were asked to categorize 117 using a score in the range (1 - 4): Category 1: negative, category 2: atypical squamous hyperplasia, category 3: carcinoma in situ; category 4: squamous carcinoma with early stromal invasion; category 5: invasive carcinoma. We ignored the categorical nature of the data and estimated the ICC under the model given in (8).</p><p>R-CODE</p><p>x&lt;-Slide_2</p><p>x$Slide&lt;-NULL</p><p>x$Serial&lt;-NULL</p><p>head(x)</p><p>library(psy)</p><p>library(boot)</p><p>icc.c1&lt;-function (data)</p><p>{</p><p>score &lt;- as.matrix(na.omit(data))</p><p>n &lt;- dim(score)[<xref ref-type="bibr" rid="scirp.65865-ref1">1</xref>]</p><p>p &lt;- dim(score)[<xref ref-type="bibr" rid="scirp.65865-ref2">2</xref>]</p><p>data2 &lt;- matrix(ncol = 3, nrow = p * n)</p><p>attr(score, &quot;dim&quot;) &lt;- c(p * n, 1)</p><p>data2[, 1] &lt;- score</p><p>subject &lt;- as.factor(rep(1:n, p))</p><p>rater &lt;- as.factor(rep(1:p, each = n))</p><p>data2[, 2] &lt;- subject</p><p>data2[, 3] &lt;- rater</p><p>ms &lt;- anova(lm(score ~ subject + rater))[[<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>]]</p><p>names(ms) &lt;- NULL</p><p>v.s &lt;- (ms[<xref ref-type="bibr" rid="scirp.65865-ref1">1</xref>] - ms[<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>])/p</p><p>v.r &lt;- (ms[<xref ref-type="bibr" rid="scirp.65865-ref2">2</xref>] - ms[<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>])/n</p><p>res &lt;- ms[<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>]</p><p>icc.a &lt;- v.s/(v.s + v.r + res)</p><p>#icc.c &lt;- v.s/(v.s + res)</p><p>return(icc.a)</p><p>}</p><p>icc.c1(x)</p><p>case.fun&lt;-function(d,i)</p><p>icc.c1(d[i,])</p><p>icc_boot</p><p>icc_boot&lt;-boot(x,case.fun,R=1000)</p><p>icc_boot</p><p>est&lt;-icc_boot$t</p><p>m&lt;-mean(est)</p><p>var(est)</p><p>sd(est)</p><p>plot(icc_boot,qdist = &quot;norm&quot;)</p><p>boot.ci(icc_boot, type = &quot;BCa&quot;)</p><p>Results:</p><p>Bootstrap Statistics: original bias std. error</p><disp-formula id="scirp.65865-formula2575"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x131.png"  xlink:type="simple"/></disp-formula><p>boot.ci(icc_boot, type = &quot;all&quot;)</p><p>Intervals:</p><p>Level Normal Basic</p><p>95% (0.5720, 0.7320) (0.5716, 0.7333)</p><p>Level Percentile BCa</p><p>95% (0.5618, 0.7235) (0.5749, 0.7320)</p><p>The ANOVA estimator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x132.png" xlink:type="simple"/></inline-formula> has a standard error = 0.037; which is comparable to the Bootstrap standard error = 0.041. Moreover, the analytical bias in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x133.png" xlink:type="simple"/></inline-formula> is −0.002, while the Bootstrap bias is −0.004.</p><p>Comments:</p><p>It is clear that our proposed Wald’s 95% confidence interval is quite close to the BC<sub>a</sub>, and this is attributed to the large sample size. Moreover, we can see from the histogram, and the q-q plot of the bootstrap samples of t<sup>*</sup>, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, which is in fact<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x134.png" xlink:type="simple"/></inline-formula>, that it has a symmetric normal distribution even though we are certain that the original scores are not normal.</p><p>Example 2: Grading of retinopathy (see <xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>Retinopathy score of retinal whole mounts was performed using fluorescent microscopy, and images were acquired using a digital camera. The extent of retinal neovascularization (NV) was estimated by implementing a specific retinal NV scoring system. In brief, the entire retina was outlined to distinguish the total retinal area of each eye. Then, the images were given threshold to emphasize only the FITC-perfused vessels. This permitted the measurement of total blood vessel area of each retina and the percentage of each retina that is engrossed with blood vessels. The scoring system was based on selecting several criteria, these are; 1) the size of the central avascular area, 2) blood vessel tuft formation, 3) extra-retinal neovascularization and 4) presence of blood vessel tortuosity. For the purposes of this model, we divided the retina into three areas: zone 1, the inner circumferential third of the retina around the optic disc; zone 2, the middle third of the retina; and zone 3, the outer third of the retina. The extent of disease was specified by clock hours or distance around the retina (number of twelfths similar to a clock). The scoring was performed in a masked fashion, by employing fluorescence microscopy, evaluating and scoring each retina in a blinded manner by three observers. The minimum score according to this method is 0, and the maximum score is 13. Maximal vaso-proliferation in this mouse model has previously been reported to occur from P17 to P21. The average retinopathy score for each animal was used for statistical analysis [<xref ref-type="bibr" rid="scirp.65865-ref27">27</xref>] .</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Graphs of histogram and q-q plot of the 1000 bootstrap sample for example 1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1240660x135.png"/></fig><p>Bootstrap Statistics: original bias std. error</p><disp-formula id="scirp.65865-formula2576"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x136.png"  xlink:type="simple"/></disp-formula><p>The ANOVA estimator is 0.958, with standard error = 0.019. The analytic bias is −0.006, but the Bootstrap bias is −0.005.</p><p>Comments:</p><p>Although the sample here is much smaller (k = 16) the Wald’s 95% confidence interval is quite close to the corresponding bootstrap confidence interval. But the distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x137.png" xlink:type="simple"/></inline-formula> is far from being normally distributed as can be seen from the histogram (skewed to the left) and the curved q-q plot in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>For example 1, <xref ref-type="table" rid="table1">Table 1</xref>0 gives the ANOVA results, and <xref ref-type="table" rid="table1">Table 1</xref>1 gives the 95% CI for the 6 methods. For example 2, <xref ref-type="table" rid="table1">Table 1</xref>2 gives the ANOVA results, and <xref ref-type="table" rid="table1">Table 1</xref>3 gives the 95% CI for the 6 methods.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Graphs of histogram and q-q plot of the 1000 bootstrap sample for example 2</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-1240660x138.png"/></fig><table-wrap id="table10" ><label><xref ref-type="table" rid="table1">Table 1</xref>0</label><caption><title> ANOVA table for the first data set</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >S.O.V.</th><th align="center" valign="middle" >d. f</th><th align="center" valign="middle" >s.o.s</th><th align="center" valign="middle" >M.S.</th></tr></thead><tr><td align="center" valign="middle" >Slides</td><td align="center" valign="middle" >116</td><td align="center" valign="middle" >613.04</td><td align="center" valign="middle" >5.285</td></tr><tr><td align="center" valign="middle" >Raters</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >77.72</td><td align="center" valign="middle" >12.954</td></tr><tr><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >969</td><td align="center" valign="middle" >195.42</td><td align="center" valign="middle" >0.281</td></tr></tbody></table></table-wrap><table-wrap id="table11" ><label><xref ref-type="table" rid="table1">Table 1</xref>1</label><caption><title> Comparing 95% CI by alternative methods</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Method</th><th align="center" valign="middle" >95% confidence units</th></tr></thead><tr><td align="center" valign="middle" >FS</td><td align="center" valign="middle" >(0.600, 0.740)</td></tr><tr><td align="center" valign="middle" >Modified Z.M.</td><td align="center" valign="middle" >(0.414, 0.784)</td></tr><tr><td align="center" valign="middle" >Wald’s</td><td align="center" valign="middle" >(0.574, 0.719)</td></tr><tr><td align="center" valign="middle" >Bootstrap normal</td><td align="center" valign="middle" >(0.572, 0.732)</td></tr><tr><td align="center" valign="middle" >Bootstrap BCa</td><td align="center" valign="middle" >(0.575, 0.732)</td></tr><tr><td align="center" valign="middle" >Bootstrap percentile</td><td align="center" valign="middle" >(0.562, 0.724)</td></tr></tbody></table></table-wrap><table-wrap id="table12" ><label><xref ref-type="table" rid="table1">Table 1</xref>2</label><caption><title> ANOVA table for data of example 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >S.O.V.</th><th align="center" valign="middle" >d.f</th><th align="center" valign="middle" >s.o.s</th><th align="center" valign="middle" >M.S.</th></tr></thead><tr><td align="center" valign="middle" >Subject</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >1066</td><td align="center" valign="middle" >71.067</td></tr><tr><td align="center" valign="middle" >Raters</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.542</td><td align="center" valign="middle" >0.271</td></tr><tr><td align="center" valign="middle" >Error</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" >1.071</td></tr></tbody></table></table-wrap><table-wrap id="table13" ><label><xref ref-type="table" rid="table1">Table 1</xref>3</label><caption><title> Comparing 95% confidence intervals by different methods for data of example 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Method</th><th align="center" valign="middle" >95% confidence units</th></tr></thead><tr><td align="center" valign="middle" >FS</td><td align="center" valign="middle" >(0.891, 0.989)</td></tr><tr><td align="center" valign="middle" >Modified ZM</td><td align="center" valign="middle" >(0.907, 0.984)</td></tr><tr><td align="center" valign="middle" >Wald’s</td><td align="center" valign="middle" >(0.918, 0.994)</td></tr><tr><td align="center" valign="middle" >Bootstrap normal</td><td align="center" valign="middle" >(0.905, 0.999)</td></tr><tr><td align="center" valign="middle" >Bootstrap BCa</td><td align="center" valign="middle" >(0.908, 0.999)</td></tr><tr><td align="center" valign="middle" >Bootstrap percentile</td><td align="center" valign="middle" >(0.901, 0.974)</td></tr></tbody></table></table-wrap></sec><sec id="s5"><title>5. Discussion</title><p>The use of the intraclass correlation to assess the reliability of judgments made by the observers is ubiquitous in medical research. Unreliable measurements can eventually affect the diagnosis of diseases and hence expose patients to undesired health risks. Several examples regarding the applications can be found in [<xref ref-type="bibr" rid="scirp.65865-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.65865-ref5">5</xref>] .</p><p>1) In the one-way we observe that from the tables that the effect of normality on the variance and the bias of the estimated ICC depend on the kurtosis of the distributions of the components of variation. We noted that the kurtosis of the between subjects component of variation is multiplied by the factor k<sup>−</sup><sup>1</sup>, kurtosis of the between rater’s component of variation is multiplied by a factor n<sup>−</sup><sup>1</sup> and that of the error component multiplied by a factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x139.png" xlink:type="simple"/></inline-formula>. Therefore the effect of non-normality of the between raters component will dominate that of the subjects component would dominate the effect of non-normality of the error (within subjects) components. In general, non-zero kurtosis of the observed distribution of measurements substantially affects the sampling distribution, the bias, and standard error of reliability estimates. For the two-way model, there is an interaction between the values of ρ and the nuisance parameter (ratio of between subjects variance to the error variance).</p><p>2) The magnitude of ρ has an effect on the sampling distribution of the reliability estimate. The larger the value of ρ the smaller the mean square error of its estimator. This observation is relevant within the framework of reliability studies since we are interested in producing large values of the estimate.</p></sec><sec id="s6"><title>6. Summary</title><p>From the above discussion we summarize our conclusions in three points:</p><p>Firstly, the effect of non-normality of the scores distribution is not tangible for k &gt; 25 (fairly large), where k is the number subjects. Secondly, large value of reliability, which is our main concern, has smaller variance, and hence a Wald’s confidence interval on the population ICC would be acceptable. This conclusion is based on the empirical evidence; as we have shown that the Wald’s interval is almost identical in length to the interval based on the bootstrap methods. Thirdly, in the design stage of a reliability study a reasonable guess of the kurtosis is required to satisfy, for given effect size and type I error rate, the sample size requirements to achieve a certain power on specific hypotheses.</p><p>We should also note that the estimation problem in the two-way model can be more complex particularly when the raters are required to repeat the assessment of each patient, in order to reduce bias and increase precision of the reliability estimator. In this case the sample size question can be: what is the number of subjects, the number of raters, and the number of repeats per subjects to achieve certain power level. In such case one has to seriously consider the cost of replications in the early stages of designing reliability study.</p></sec><sec id="s7"><title>Cite this paper</title><p>Mohamed M. Shoukri,Tusneem Al-Hassan,Michael DeNiro,Abdelmoneim El Dali,Futwan Al-Mohanna, (2016) Bias and Mean Square Error of Reliability Estimators under the One and Two Random Effects Models: The Effect of Non-Normality. Open Journal of Statistics,06,254-273. doi: 10.4236/ojs.2016.62022</p></sec><sec id="s8"><title>Appendices</title><p>Appendix I: The Taylor’s expansion of a function of several variables.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x140.png" xlink:type="simple"/></inline-formula> be a random vector with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x141.png" xlink:type="simple"/></inline-formula> be a real valued continuously differentiable function of X.</p><p>The Taylor series expansion of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x142.png" xlink:type="simple"/></inline-formula> around <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x143.png" xlink:type="simple"/></inline-formula> is given by:</p><disp-formula id="scirp.65865-formula2577"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x144.png"  xlink:type="simple"/></disp-formula><p>Appendix II: Analytic formula of the bias of the estimated intraclass correlation under the one-way random effects model.</p><p>1) The non-normal case:</p><disp-formula id="scirp.65865-formula2578"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x145.png"  xlink:type="simple"/></disp-formula><p>2) Under normality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x146.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x147.png" xlink:type="simple"/></inline-formula>. Hence</p><disp-formula id="scirp.65865-formula2579"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x148.png"  xlink:type="simple"/></disp-formula><p>Appendix III: Analytic expression for variance and bias of the estimated intraclass correlation in the two- way random effects model:</p><p>1) Variance Expression under normality:</p><disp-formula id="scirp.65865-formula2580"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x149.png"  xlink:type="simple"/></disp-formula><p>It would be most informative to express the bias and variance in terms of ρ (the primary parameter of interest) and simplify the expressions accordingly:</p><disp-formula id="scirp.65865-formula2581"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x150.png"  xlink:type="simple"/></disp-formula><p>We can now write variance expression as</p><disp-formula id="scirp.65865-formula2582"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x151.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2583"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x152.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2584"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x153.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x154.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x155.png" xlink:type="simple"/></inline-formula></p><p>2) Bias in Estimating <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x156.png" xlink:type="simple"/></inline-formula> under normality.</p><p>A first order approximation of the bias under the assumption of normality is given by:</p><disp-formula id="scirp.65865-formula2585"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x157.png"  xlink:type="simple"/></disp-formula><p>The terms of the bias expression are:</p><disp-formula id="scirp.65865-formula2586"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x158.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2587"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x159.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.65865-formula2588"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x160.png"  xlink:type="simple"/></disp-formula><p>Appendix IV: variance and bias of estimated intraclass correlation under non-normality.</p><p>Variance:</p><disp-formula id="scirp.65865-formula2589"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x161.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.65865-formula2590"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x162.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2591"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x163.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2592"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x164.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2593"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x165.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2594"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x166.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2595"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x167.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x168.png" xlink:type="simple"/></inline-formula></p><p>Bias:</p><p>The delta method is used to derive the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x169.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.65865-formula2596"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x170.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2597"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x171.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1240660x172.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.65865-formula2598"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x173.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2599"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x174.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2600"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x175.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2601"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x176.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2602"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x177.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65865-formula2603"><graphic  xlink:href="http://html.scirp.org/file/5-1240660x178.png"  xlink:type="simple"/></disp-formula></sec></body><back><ref-list><title>References</title><ref id="scirp.65865-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Atenafu, E.G., Hamid, J.S., To, T., Willan, A., Feldman, B. and Beyene, J. 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