<?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.2021.115052</article-id><article-id pub-id-type="publisher-id">OJS-112779</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>
 
 
  Stochastic SIR Household Epidemic Model with Misclassification
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Umar</surname><given-names>M. Abdulkarim</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Nasarawa State University, Keffi, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>27</day><month>09</month><year>2021</year></pub-date><volume>11</volume><issue>05</issue><fpage>886</fpage><lpage>905</lpage><history><date date-type="received"><day>21,</day>	<month>July</month>	<year>2021</year></date><date date-type="rev-recd"><day>25,</day>	<month>October</month>	<year>2021</year>	</date><date date-type="accepted"><day>28,</day>	<month>October</month>	<year>2021</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>
 
 
  In this work, we developed a theoretical framework leading to misclassification of the final size epidemic data for the stochastic SIR (Susceptible-In
  fective
  -Removed), household epidemic model, with false negative and false positive misclassification probabilities. Maximum likelihood based algorithm is then employed for its inference. We then analyzed and compared the estimates of the two dimensional model with those of the three and four dimensional models associated with misclassified final size data over arrange of theoretical parameters, local and global infection rates and corresponding proportion infected in the permissible region, away from its boundaries and misclassification probabilities.
   
  The adequacies of the three models to the final size data are examined. The four and three-dimensional models are found to outperform the two dimensional model on misclassified final size data.
 
</p></abstract><kwd-group><kwd>Final Size Epidemic</kwd><kwd> Infectious Period Distribution</kwd><kwd> Maximum Likelihood Es-timates</kwd><kwd> Misclassification Probabilities</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Inference of the stochastic SIR household epidemic model without misclassification is well analyzed in [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.112779-ref6">6</xref>]. The work of [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] and [<xref ref-type="bibr" rid="scirp.112779-ref7">7</xref>] provided maximum likelihood based algorithm for its inferences. But sometimes, the final size epidemic data is subject to misclassification error. This occurs in categorical data when the actual and recorded categories for subject differs [<xref ref-type="bibr" rid="scirp.112779-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref9">9</xref>]. For example, the susceptibles may be wrongly be classified as infectives or an infectives wrongly classified as susceptibles. It then becomes necessary to adjust our inferences to such errors in order to get the precise parameter estimates and model that adequately fits the final size epidemic data. Using the theoretical framework developed in this work with simulations, we explored the estimates of the parameters of the models and the adequacy of their fitness to the final size epidemic data for a range misclassification probabilities ε F N , ε F P ∈ [ 0,0.5 ) . We do this by exploring the plots of the root mean square error of the estimates defined over the range of the misclassification probabilities in [0, 0.5), in order to provide clarity on the nature of their fitness to the final size epidemic data. This enables us to identify the model that adequately fits better to the final size epidemic data.</p></sec><sec id="s2"><title>2. Material and Methods</title>The Model<p>We have assumed that the stochastic SIR household final size data of [<xref ref-type="bibr" rid="scirp.112779-ref4">4</xref>], is subject to misclassification error; which may be caused by susceptibles wrongly classified as infectives or infectives wrongly classified as susceptibles.</p><p>The probability of observing i infectives in a household of size n given that the true number of infectives is j and that of the susceptibles is n − j takes cognisance of the true and false positives with their classification probabilities 1 − ε F N and ε F P .</p><p>Let x and y be the observed false and true positives in a household of size n. Then the probability of observing x + y = i positives, given that the true number of positives is j can be written as,</p><p>P i , j ( n ) = P ( x + y = i | True infect = j , household size = n ) . (1)</p><p>We can express, the probability of making correct and precise observation of an infective when it is a true infective, and a susceptible, when it is a true susceptible, independently as, 1 − ε F N and 1 − ε F P . The distribution of observing i number of infectives correctly and incorrectly is Binomial distributed, Bin ( j ,1 − ε F N ) , and Bin ( n − j , ε F P ) . Equally the probability of observing the susceptibles correctly and incorrectly are Binomial distributed, Bin ( n − j ,1 − ε F P ) and Bin ( j , ε F N ) respectively.</p><p>The number of infectives observed is the sum of the true and false positives and has the sum of the Binomial distributions,</p><p>Bin ( j ,1 − ε F N ) + Bin ( n − j , ε F P ) . (2)</p><p>Equally, the number of susceptibles observed is the sum of the true and false negatives and has the sum of the Binomial distributions,</p><p>Bin ( n − j ,1 − ε F P ) + Bin ( j , ε F N ) . (3)</p><p>The probability of observing i infectives in a household of size of n can then be written as,</p><p>q n , i = ∑ j = 0 n     P ( Obs = i , True infect = j , household size = n ) . (4)</p><p>Since,</p><p>P ( Obs = i , True = j , household size = n ) = P ( Obs = i | True = j , household size = n ) P ( True = j ) . (5)</p><p>q n , i = ∑ j = 0 n     P ( x + y = i | True&#160;infect = j , household&#160;size = n ) P ( True = j ) , (6)</p><p>where P ( True = j ) , j = 0,1, ⋯ , n are the final size probabilities. We can then write,</p><p>q n , i = ∑ j = 0 n     P i , j ( n ) P j ( n ) , i = 0 , 1 , ⋯ , n . (7)</p><p>where</p><p>P i , j ( n ) = P ( x + y = i | True = j , household size = n ) . (8)</p><p>We can generalize the expression, P i , j ( n ) for i ,   j = 0 , 1 , 2 , ⋯ , n and any r ∈ ℤ + ≤ n using the results of P 0, j ( n ) , P 1, j ( n ) , ⋯ , P i , j ( n ) as,</p><p>P i , j ( n ) = j ( j − 1 ) ( j − 2 ) ⋯ ( j − i + 1 ) r ! ε F N j − i ( 1 − ε F N ) r ( 1 − ε F P ) n − j   + j ( j − 1 ) ⋯ ( j − i + 2 ) ( i − 1 ) ! ( n − j ) ε F P ( 1 − ε F P ) n − j − 1 ε F N j − i + 1 ( 1 − ε F N ) i − 1   + j ( j − 1 ) ( j − 2 ) ⋯ ( j − i + 3 ) ( i − 2 ) ! ( n − j ) ( n − j − 1 ) 2 ! ε F P 2 ( 1 − ε F P ) n − j − 2 ε F N j − i + 2 ( 1 − ε F N ) i − 2   + j ( j − 1 ) ( j − 2 ) ⋯ ( j − i + 4 ) ( r − 3 ) ! ( n − j − 1 ) ( n − j − 2 ) 3 ! ε F P 3 ( 1 − ε F P ) n − j − 3 ( 1 − ε F N ) i − 3 ε F N j − i + 3   + ⋯ + ( n − j ) ( n − j − 1 ) ⋯ ( n − j − i + 2 ) ( r − 1 ) ! ε F P i − 1 ( 1 − ε F P ) n − j − i + 1 j ( 1 − ε F N ) ε F N j − 1   + ( n − j ) ( n − j − 1 ) ⋯ ( n − j − i + 1 ) r ! ε F P i ( 1 − ε F P ) n − j − i ε F N j (9)</p><p>Knowing the terms of P i , j ( n ) , i ,   j = 0 , 1 , ⋯ , n , the expression for q n , i , i = 0 , 1 , ⋯ , n are evaluated. For example the probability of observing i = 0 infectives in a household of size n can be evaluated as,</p><p>q n , 0 = ∑ j = 0 n     P 0 , j ( n ) P j ( n ) , j = 0 , 1 , ⋯ , n .</p><p>where P j ( n ) are the final size probabilities, defined as the probability of observing j infectives in a household of size n, [<xref ref-type="bibr" rid="scirp.112779-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref11">11</xref>].</p><p>Similarly, the chance of observing i = 1 infectives in a household of size n can be obtained using the terms of P 1 , j ( n ) , ∀ j ∈ ℤ + ≤ n . This probability reduces to,</p><p>q n , 1 = ∑ j = 0 n     P 1 , j ( n ) P j ( n )</p><p>In general, the probability of observing i ∈ ℤ + ≤ n infectives in a household of size n, is obtained as,</p><p>P r , j ( n ) = ∑ k = 0 r ( j r − k ) ( n − j k ) ε F N j − r + k ( 1 − ε F N ) r − k ε F P k ( 1 − ε F P ) n − j − k (10)</p><p>Equations (10) is the sum of two Binomial distributions, Bin ( j , ( 1 − ε F N ) ) and Bin ( n − j , ε F P ) defined as the probabilities of observing r − k true positives from the true j number of infectives and k false positives from the remaining n − j number of susceptibles in a household of size n.</p><p>Alternatively, P r , j ( n ) has the form,</p><p>P r , j ( n ) = ∑ k = 0 r ( j k ) ( n − j r − k ) ε F N j − k ( 1 − ε F N ) k ε F P r − k ( 1 − ε F P ) n − j − r + k . (11)</p><p>Equation (11) is also the sum of two Binomial distributions in Equation (10) and defined as the probability of observing k true positives from the true j infectives and r − k false positives from the remaining n − j susceptibles in a household of size n.</p><p>Here, both Equations (10) and (11) for P r , j ( n ) satisfies,</p><p>∑ i = 0 n     P i , j ( n ) = 1 ,   ∀ j ∈ ℤ + ≤ n .</p></sec><sec id="s3"><title>3. The Three-Dimensional Model</title><p>If the false positive and false negative misclassification probabilities are the same then Equations (2) and (3) for the distribution of the number of infected individuals observed and those of the susceptible individuals observed only depend on the common misclassification probability denoted here as ε . In these equations, ε F N and ε F P are replaced by ε same as in the expressions for P i , j ( n ) , i , j = 0 , 1 , ⋯ , n and simplified as,</p><p>P i , j ( n ) = ∑ k = 0 i ( j i − k ) ( n − j k ) ε j − i + 2 k ( 1 − ε ) n − j + i − 2 k ,   i , j = 0 , 1 , ⋯ , n . (12)</p><p>Alternatively, we can employ</p><p>P i , j ( n ) = ∑ k = 0 i ( j k ) ( n − j i − k ) ε j + i − 2 k ( 1 − ε ) n − j − i + 2 k ,   i , j = 0 , 1 , ⋯ , n . (13)</p><p>Equations (12) and (13) for P i , j ( n ) which are particular cases of Equations (10) and (11) when the misclassification probabilities are the same are made of two Binomial distributions. While Equation (12) expresses the probability of observing i − k infectives from the true j infectives and k infectives from the remaining n − j susceptibles in the household of size n, Equation (13) expresses the probability of observing k infectives from the true j infectives and i − k infectives from the remaining n − j susceptibles in the household of size n.</p><p>Since they are probabilities, both equations P i , j ( n ) , must satisfy,</p><p>∑ i = 0 n     P i , j ( n ) = 1 , ∀ j ∈ { 0 , 1 , ⋯ , n } .</p></sec><sec id="s4"><title>4. Maximum Likelihood Estimation</title><p>The distribution of the final size epidemic data x n , i is multinomial, [<xref ref-type="bibr" rid="scirp.112779-ref12">12</xref>] where x n , i are the number of households of size n in which i infectives are observed and q n , i are the probabilities of observing i infectives in a household of size n, [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref13">13</xref>]. The approximate likelihood function of the model parameters is then a function of q n , i and dependent on the parameters to be estimated from the four dimensional model. These are the local infection rate λ L , the probability of avoiding infection from outside the household π , the false positive misclassification probability, ε F P and the false negative misclassification probability, ε F N and hence q n , i has the form q n , i ( λ L , π , ε F P , ε F N ) .</p><p>The approximate likelihood function can be written as,</p><p>L ( λ L , π , ε F P , ε F N ) ∝ ∏ n = 1 max   ∏ i = 0 n     q n , i ( λ L , π , ε F P , ε F N ) x n , i . (14)</p><p>where max is the maximum household size.</p><p>Since the estimates that maximize the approximate likelihood function also maximize the approximate loglikelihood function, we can write,</p><p>l ( λ L , π , ε F P , ε F N ) = ∑ n = 1 max   ∑ i = 0 n ( x n , i log e ( ∑ j = 0 n     P i , j ( n ) P j ( n ) ) ) ,   i , j = 0 , 1 , ⋯ , n . (15)</p><p>where log ( L ( λ L , π , ε F P , ε F N ) ) = l ( λ L , π , ε F P , ε F N )</p><p>The approximate likelihood function for the three dimensional model also has similar representation with differences in the number of parameters to be estimated.</p></sec><sec id="s5"><title>5. Numerical Simulation and Inference on the Three and Four Dimensional Final Size Epidemic Data</title><p>How precise are the maximum likelihood estimates from the numerical optimizations, given the minimum epidemic and population sizes, the proportion of the initial susceptibles infected and the magnitude of the misclassification probabilities? Which of these parameters are intractable to estimate in the face of large misclassification probabilities? Which model best fits the final size epidemic data in the face of varying misclassification probabilities in the permissible region, [ 0,0.5 ) ? These are some of the questions to be explored in this section using simulation studies.</p>Fitting the Three Models to Data from the Four Dimensional Model<p>We demonstrate the computational procedures of fitting the three models to four dimensional epidemic data from simulation studies and examined the behaviours of the estimates using some functions and subroutines developed for this work as,</p><p>Run the function FourDimThreeATwoSNsimhousesScatterPlotsMisspec to simulate four dimensional household epidemic data with Gamma ( a , b ) infectious period distribution, theoretical parameters, λ L , λ G and ε F N ,   ε F P ∈ [ 0,0.5 ) . It then calculate the corresponding parameters of the three models with Gamma ( a , b ) infectious period distribution computes, their mean, standard deviation and root mean square error of the estimates and plot the estimates using the following subroutines.</p><p>a) LampaiD ( m a t ) , provides starting values for the two dimensional model parameters, λ L and π according to [<xref ref-type="bibr" rid="scirp.112779-ref12">12</xref>].</p><p>b) Enegloglik 4 ( y , n , a , b , m a t ) , computes the negative of the loglikelihood function associated with the three dimensional model using the parameters of Gamma ( a , b ) infectious period distribution, the final size epidemic data and the starting parameters values obtained by inverse transformation of the parameter space.</p><p>c) negloglik 2 ( x , n , a , b , m a t ) , computes the negative loglikelihood function associated with the two dimensional model from the parameters of Gamma ( a , b ) infectious period distribution, the final size epidemic data and the starting values according to [<xref ref-type="bibr" rid="scirp.112779-ref12">12</xref>].</p><p>d) Misclass 2 ( ε , n ) , computes the misclassification Probabilities associated with the three dimensional model from the misclassification probability parameter ε and maximum household size n.</p><p>e) final _ sizep ( a , b , π , n , λ L ) computes the final size probabilities associated with the two dimensional model from the parameters of Gamma ( a , b ) infectious period distribution, π , λ L and maximum household size n.</p><p>f) Misclass 3 ( a , b , n , π , λ L , ε ) , computes the sum of the product of the misclassification probabilities and the final size probabilities associated with the three dimensional model for the computation of the negative loglikelihood function.</p><p>g) falseMisclass 2 ( ε F N , ε F P , n ) , computes the misclassification probabilities associated with the four dimensional model.</p><p>h) SIRfalsePmisclass ( a , b , n , π , λ L , fneg , fpos ) , computes the products of the misclassification probabilities and the final size probabilities associated with the loglikelihood function of the four dimensional model.</p><p>i) pinf 2 ( a , b , π , λ L houses ) , calculates z and λ G , from the parameters of Gamma ( a , b ) infectious period distribution, model parameters π , λ L and vector of household sizes, where houses is the vector of household sizes.</p><p>j) RSTER 2 ( a , b , c , λ L , λ G , h o u s e s ) calculates the threshold parameter, R ∗ from the parameters of Gamma ( a , b ) infectious period distribution, theoretical parameters λ L , λ G and vector of household sizes, houses.</p><p>Using the theoretical parameters, z = 0.7298 , λ L = 0.1 , λ G = 0.29 , π = 0.4199 , R ∗ = 2.2166 , household structure in [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] but fifty times its population size given by 70700, minimum epidemic size of 1000 and simulation runs of 1000. The estimates of the parameters of the three models were obtained for the following pairs of the misclassification probabilities ( ε F N = 0.02 , ε F P = 0.1 ), ( ε F N = 0.3 , ε F P = 0.2 ) and ( ε F N = 0.2 , ε = 0.2 ) respectively shown in Figures 1-3 and analyzed in Tables 1-3 respectively.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1"><xref ref-type="table" rid="table">Table </xref>1</xref></label><caption><title> <xref ref-type="table" rid="table">Table </xref>of the mean of the parameter estimates of the three models</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par. Estim.</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.02 , ε F P = 0.1</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.3 , ε F P = 0.2</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.2 , ε F P = 0.2</th><th align="center" valign="middle"  rowspan="2"  >Theo. Param</th></tr></thead><tr><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.084899</td><td align="center" valign="middle" >0.090811</td><td align="center" valign="middle" >0.10138</td><td align="center" valign="middle" >0.018974</td><td align="center" valign="middle" >0.14651</td><td align="center" valign="middle" >0.13265</td><td align="center" valign="middle" >0.03056</td><td align="center" valign="middle" >0.10032</td><td align="center" valign="middle" >0.117</td><td align="center" valign="middle" >0.1</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.3129</td><td align="center" valign="middle" >0.31015</td><td align="center" valign="middle" >0.28961</td><td align="center" valign="middle" >0.32242</td><td align="center" valign="middle" >0.23107</td><td align="center" valign="middle" >0.2744</td><td align="center" valign="middle" >0.33117</td><td align="center" valign="middle" >0.29025</td><td align="center" valign="middle" >0.28441</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.38599</td><td align="center" valign="middle" >0.3865</td><td align="center" valign="middle" >0.4211</td><td align="center" valign="middle" >0.47438</td><td align="center" valign="middle" >0.52772</td><td align="center" valign="middle" >0.45322</td><td align="center" valign="middle" >0.42115</td><td align="center" valign="middle" >0.41985</td><td align="center" valign="middle" >0.4338</td><td align="center" valign="middle" >0.4199</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.74206</td><td align="center" valign="middle" >0.74761</td><td align="center" valign="middle" >0.72958</td><td align="center" valign="middle" >0.56414</td><td align="center" valign="middle" >0.67592</td><td align="center" valign="middle" >0.71616</td><td align="center" valign="middle" >0.6369</td><td align="center" valign="middle" >0.72953</td><td align="center" valign="middle" >0.72469</td><td align="center" valign="middle" >0.7298</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.020239</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.30444</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.20185</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.097445</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.20979</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.19559</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.01074</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.31411</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.19921</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >2.2495</td><td align="center" valign="middle" >2.2857</td><td align="center" valign="middle" >2.2164</td><td align="center" valign="middle" >1.5467</td><td align="center" valign="middle" >2.0074</td><td align="center" valign="middle" >2.1721</td><td align="center" valign="middle" >1.7365</td><td align="center" valign="middle" >2.2151</td><td align="center" valign="middle" >2.2004</td><td align="center" valign="middle" >2.2166</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table">Table </xref>2</label><caption><title> <xref ref-type="table" rid="table">Table </xref>of the standard deviation of the parameter estimates of the three models</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par. Estim.</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.02 , ε F P = 0.1</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.3 , ε F P = 0.2</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.2 , ε F P = 0.2</th></tr></thead><tr><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.0015409</td><td align="center" valign="middle" >0.0044091</td><td align="center" valign="middle" >0.011434</td><td align="center" valign="middle" >0.00088506</td><td align="center" valign="middle" >0.056186</td><td align="center" valign="middle" >0.074851</td><td align="center" valign="middle" >0.0010531</td><td align="center" valign="middle" >0.012306</td><td align="center" valign="middle" >0.060019</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.0024536</td><td align="center" valign="middle" >0.0030933</td><td align="center" valign="middle" >0.017684</td><td align="center" valign="middle" >0.0018842</td><td align="center" valign="middle" >0.014262</td><td align="center" valign="middle" >0.05958</td><td align="center" valign="middle" >0.002174</td><td align="center" valign="middle" >0.0063406</td><td align="center" valign="middle" >0.047968</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.0042913</td><td align="center" valign="middle" >0.0043876</td><td align="center" valign="middle" >0.029889</td><td align="center" valign="middle" >0.0031843</td><td align="center" valign="middle" >0.015945</td><td align="center" valign="middle" >0.10611</td><td align="center" valign="middle" >0.0035712</td><td align="center" valign="middle" >0.006532</td><td align="center" valign="middle" >0.084542</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.0034378</td><td align="center" valign="middle" >0.0051624</td><td align="center" valign="middle" >0.015988</td><td align="center" valign="middle" >0.0024631</td><td align="center" valign="middle" >0.016208</td><td align="center" valign="middle" >0.057152</td><td align="center" valign="middle" >0.0027625</td><td align="center" valign="middle" >0.011531</td><td align="center" valign="middle" >0.044632</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.011379</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.019208</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.019286</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.06998</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.12818</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.12458</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0072381</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.015834</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.01398</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >0.016441</td><td align="center" valign="middle" >0.030185</td><td align="center" valign="middle" >0.064045</td><td align="center" valign="middle" >0.0050586</td><td align="center" valign="middle" >0.049663</td><td align="center" valign="middle" >0.23955</td><td align="center" valign="middle" >0.0075251</td><td align="center" valign="middle" >0.062329</td><td align="center" valign="middle" >0.18484</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table">Table </xref>3</label><caption><title> <xref ref-type="table" rid="table">Table </xref>of the root mean square error of the parameter estimates of the three models</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par. Estim.</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.02 , ε F P = 0.1 .</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.3 , ε F P = 0.2</th><th align="center" valign="middle"  colspan="3"  >ε F N = 0.2 , ε F P = 0.2</th></tr></thead><tr><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td><td align="center" valign="middle" >2Dim.</td><td align="center" valign="middle" >3Dim.</td><td align="center" valign="middle" >4Dim.</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.015179</td><td align="center" valign="middle" >0.01019</td><td align="center" valign="middle" >0.011506</td><td align="center" valign="middle" >0.081031</td><td align="center" valign="middle" >0.072919</td><td align="center" valign="middle" >0.081593</td><td align="center" valign="middle" >0.069448</td><td align="center" valign="middle" >0.012298</td><td align="center" valign="middle" >0.062322</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.023027</td><td align="center" valign="middle" >0.020387</td><td align="center" valign="middle" >0.017671</td><td align="center" valign="middle" >0.032475</td><td align="center" valign="middle" >0.060628</td><td align="center" valign="middle" >0.061531</td><td align="center" valign="middle" >0.041225</td><td align="center" valign="middle" >0.006339</td><td align="center" valign="middle" >0.048246</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.034178</td><td align="center" valign="middle" >0.033682</td><td align="center" valign="middle" >0.029883</td><td align="center" valign="middle" >0.054578</td><td align="center" valign="middle" >0.10899</td><td align="center" valign="middle" >0.11112</td><td align="center" valign="middle" >0.0037814</td><td align="center" valign="middle" >0.0065256</td><td align="center" valign="middle" >0.085593</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.012745</td><td align="center" valign="middle" >0.018553</td><td align="center" valign="middle" >0.015974</td><td align="center" valign="middle" >0.16567</td><td align="center" valign="middle" >0.056251</td><td align="center" valign="middle" >0.058699</td><td align="center" valign="middle" >0.092928</td><td align="center" valign="middle" >0.011522</td><td align="center" valign="middle" >0.044879</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.01137</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.019695</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.019355</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.069956</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.12842</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.12454</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.049788</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.066036</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.013988</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >0.036808</td><td align="center" valign="middle" >0.075438</td><td align="center" valign="middle" >0.063981</td><td align="center" valign="middle" >0.66988</td><td align="center" valign="middle" >0.21497</td><td align="center" valign="middle" >0.24341</td><td align="center" valign="middle" >0.48018</td><td align="center" valign="middle" >0.062283</td><td align="center" valign="middle" >0.18536</td></tr></tbody></table></table-wrap><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows fitting the Two, Three and Four Dimensional Models to the Four Dimensional the final Size Epidemic Data, when ε F N = 0.02 , ε F P = 0.1 .</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows fitting the Two, Three and Four Dimensional Models to the Four Dimensional the final Size Epidemic Data, when ε F N = 0.3 , ε F P = 0.2 .</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows fitting the Two, Three and Four Dimensional Models to the Four Dimensional the final Size Epidemic Data, when ε F N = 0.2 , ε F P = 0.2 .</p></sec><sec id="s6"><title>6. Comparison of the Models on the Four Dimensional Data</title><sec id="s6_1"><title>6.1. Simulations with the Theoretical Parameter, λ L = 0 . 1 3 , λ G = 0 . 1 7 , π = 0 . 7 4 2 3 , z = 0 . 4 2 7 5 , R ∗ = 1 . 4 3 1 6</title><p>We simulated household epidemic, with the following theoretical parameters, λ L = 0.13 , λ G = 0.17 , π = 0.7423 , R ∗ = 1.4316 and misclassification probabilities, ε F N = 0.2 − ε F P , ε F P ∈ [ 0 , 0.2 ] with step size of =0.005.</p><p>With theoretical parameters corresponding to z = 0.42755 , we found the estimates of λ L for the two dimensional model to be imprecise and biased especially when the misclassification probabilities increase from zero as in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a). The two dimensional model is not a sufficient fit to the four dimensional final epidemic data. These behaviours can be observed for other parameters for the two dimensional model as in Figures 4 (b)-(g).</p><p>The three dimensional model has precise estimates of λ L for misclassification probability in 0.08 ≤ ε F P ≤ 0.12 , while the four dimensional model is best</p><p>if 0 ≤ ε F P ≤ 0.08 and ε F P ≥ 0.17 . This shows that the four dimensional model has precise estimates of λ L compared to those of the two and three dimensional models, if the misclassification probabilities are large and far apart from each other.</p><p>In the case of λ G , the two dimensional model has imprecise and biased estimates, while those of the three dimensional model are precise if 0.08 ≤ ε F P ≤ 0.01 , those of the four dimensional model are precise if, 0 ≤ ε F P ≤ 0.075 and ε F P ≥ 0.115 .</p><p>In the case of π , the two dimensional model has precise estimates if, 0.02 ε F P ≤ 0.025 , while the three dimensional model has precise estimates, if 0.03 ≤ ε F P ≤ 0.105 , the four dimensional model is best if, 0 ≤ ε F P ≤ 0.015 and ε F P ≥ 0.111 .</p><p>In the case of z, we found that the two dimensional model is best if, 0.085 ≤ ε F P ≤ 0.095 , while the three dimensional model is best if 0.1 ≤ ε F P ≤ 0.11 . The estimates of the four dimensional model are precise if, 0 ≤ ε F P ≤ 0.08 and ε F P ≥ 0.115 .</p><p>In the case of the false positive misclassification probability estimates, the three dimensional model is best, if 0.09 ≤ ε F P ≤ 0.115 , while the four dimensional model is best if 0 ≤ ε F P ≤ 0.085 and ε F P ≥ 0.120 respectively.</p><p>In the case of the false negative misclassification probability, the three dimensional model is best if, 0.09 ≤ ε F P ≤ 0.115 , while the four dimensional model is best if, 0 ≤ ε F P ≤ 0.085 and ε F P ≥ 0.120 .</p><p>Similarly in the case of the threshold parameter, the two dimensional model is best if 0.09 ≤ ε F P ≤ 0.1 , the three dimensional model is best, if 0.1 ≤ ε F P ≤ 0.105 , while the four dimensional model is best, if 0 ≤ ε F P ≤ 0.085 and ε F P ≥ 0.110 .</p><p>In summary, we see in Figures 4(a)-(g) that the estimates from the four dimensional model are more precise than those from the two and three dimensional models when the misclassification probabilities are large and far apart from each other.</p><p>However if ε F P = 0.1 , then those of the three dimensional models are precise since the false negative misclassification probability, ε F N = 0.1 reduces to the false positive misclassification probability, which is a particular case of the four dimensional model.</p><p>The three dimensional are precise if the two misclassification probabilities are close to each other while those of the two dimensional model are best if the misclassification probabilities are zero or close to it.</p></sec><sec id="s6_2"><title>6.2. Simulations with Theoretical Parameters, λ L = 0 . 1 , λ G = 0 . 2 9 , π = 0 . 4 1 9 9 , z = 0 . 7 2 9 8 , R ∗ = 2 . 2 1 6 6</title><p>We simulated household epidemic with the following theoretical parameters along the line ε F N = 0.2 − ε F P , ε F P ∈ [ 0 , 0.2 ] , step size = 0.005. λ L = 0.1 , λ G = 0.29 , π = 0.4199 , R ∗ = 2.2166 .</p><p>We then obtained the estimates of the parameters of the three models and presented plots of their root mean square error in Figures 5 (a)-(g) for a range of misclassification probabilities in [ 0,0.2 ] .</p><p>From the simulation plots in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a), we see that the estimates of λ L from the two dimensional model are driven by bias and are precise if, ε F P ≤ 1.975 , while the estimates of λ L from three dimensional model are precise if, 0.050 ≤ ε F P ≤ 0.165 . Those of the four dimensional model are precise if, 0 ≤ ε F P ≤ 0.045 and ε F P ≥ 0.175 .</p><p>In the case of λ G in Figures 5(b), the estimates of the two dimensional model are best if, 0 ≤ ε F P ≤ 0.07 , those of the three dimensional model are best if, 0.075 ≤ ε F P ≤ 0.145 , while those of the four dimensional model are best if ε F P ≥ 0.150 .</p><p>Also, in the case of π in <xref ref-type="fig" rid="fig5">Figure 5</xref>(c), the estimates of the two dimensional are best if, 0.125 ≤ ε F P ≤ 0.175 , those of the three dimensional model are best if, 0.07 ≤ ε F P ≤ 0.120 , while those of the four dimensional model are best if, 0 ≤ ε F P ≤ 0.065 and ε F P ≥ 0.18 .</p><p>In the case of z, the estimates of the two dimensional model are best if, 0.13 ≤ ε F P ≤ 0.165 , those of the three dimensional model are best if,</p><p>0.065 ≤ ε F P ≤ 0.125 , while those of the four dimensional model are best if,</p><p>0 ≤ ε F P ≤ 0.06 and ε F P ≥ 0.17 .</p><p>In the case of the false positive misclassification probability, ε F N , the three dimensional model has precise estimates if, 0.05 ≤ ε F P ≤ 0.165 , while the four dimensional has precise estimates if, 0 ≤ ε F P ≤ 0.045 and ε F P ≥ 0.165 .</p><p>On the other hand, the estimates of the false negative misclassification probability from the three dimensional model are precise if 0.09 ≤ ε F P ≤ 0.105 , while from the four dimensional model the estimates are precise if, 0 ≤ ε F P ≤ 0.085 and ε F P ≥ 0.110 .</p><p>The threshold parameter, R ∗ has best estimates from the two dimensional model if, 0.14 ≤ ε F P ≤ 0.165 , while it has best from the three dimensional model if, 0.065 ≤ ε F P ≤ 0.135 . It has best estimates from the four dimensional model if, 0 ≤ ε F P ≤ 0.060 and ε F P ≥ 0.170 .</p></sec></sec><sec id="s7"><title>7. Simulation with Three Dimensional Epidemic Data</title><p>We studied the properties of the estimates of the three models on three dimensional epidemic data in the face of ε ∈ [ 0,0.5 ) using simulations with Gamma ( a , b ) infectious period distribution and pair of theoretical parameters ( λ L , λ G ) using the function and, subroutines developed for this work.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows fitting the Two, Three and Four Dimensional Models to the Three Dimensional Simulated Final Size Epidemic Data, when ε = 0.01 .</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows fitting the Two, Three and Four Dimensional Models to the Three Dimensional Simulated Final Size Epidemic Data, when ε = 0.02 .</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows fitting the Two, Three and Four Dimensional Models to the Three Dimensional Simulated Final Size Epidemic Data, when ε = 0.2 .</p><p>Tableof Mean, Standard Deviation and Root Mean Square Error of the Estimates for the Two, Three and Four Dimensional Models, When ε = 0.02 , 0.02 and ε = 0.2 are shown in Table4 and Table5.</p></sec><sec id="s8"><title>8. Simulations and Inferences of the Two and Three Dimensional Models for z ∈ [ 0 , 1 ]</title><p>We explored the estimates of the three models with two different sets of theoretical parameters with corresponding z = 0.2144 and z = 0.7298 away from their boundaries, simulation runs of 500, misclassification probabilities ε ∈ [ 0,0.1 ) , with stepsize of 0.01, household structure in [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.112779-ref14">14</xref>] and 50 times its population size, minimum epidemic size of 1000, to understand the properties of the estimates. We then simulate and estimate the models parameters, compute and plot the root mean square of the estimates. Beginning with</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table">Table </xref>4</label><caption><title> Mean of the parameter estimates of the two, three and four dimensional models where, 2Dim = two dimensional model, 3Dim = three dimensional model and 4Dim = four dimensional model</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par.</th><th align="center" valign="middle"  colspan="10"  >Misclassification probability and model.</th></tr></thead><tr><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >Theo</td></tr><tr><td align="center" valign="middle" >ε</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.094069</td><td align="center" valign="middle" >0.10023</td><td align="center" valign="middle" >0.10309</td><td align="center" valign="middle" >0.088669</td><td align="center" valign="middle" >0.099995</td><td align="center" valign="middle" >0.10278</td><td align="center" valign="middle" >0.030611</td><td align="center" valign="middle" >0.099752</td><td align="center" valign="middle" >0.11092</td><td align="center" valign="middle" >0.1000</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.29291</td><td align="center" valign="middle" >0.28987</td><td align="center" valign="middle" >0.28513</td><td align="center" valign="middle" >0.29577</td><td align="center" valign="middle" >0.29005</td><td align="center" valign="middle" >0.28576</td><td align="center" valign="middle" >0.33108</td><td align="center" valign="middle" >0.29038</td><td align="center" valign="middle" >0.28831</td><td align="center" valign="middle" >0.29</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.41882</td><td align="center" valign="middle" >0.42013</td><td align="center" valign="middle" >0.42827</td><td align="center" valign="middle" >0.41765</td><td align="center" valign="middle" >0.41995</td><td align="center" valign="middle" >0.42737</td><td align="center" valign="middle" >0.42125</td><td align="center" valign="middle" >0.41992</td><td align="center" valign="middle" >0.4268</td><td align="center" valign="middle" >0.4199</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.72472</td><td align="center" valign="middle" >0.72974</td><td align="center" valign="middle" >0.72572</td><td align="center" valign="middle" >0.72004</td><td align="center" valign="middle" >0.72962</td><td align="center" valign="middle" >0.72606</td><td align="center" valign="middle" >0.6369</td><td align="center" valign="middle" >0.72901</td><td align="center" valign="middle" >0.72763</td><td align="center" valign="middle" >0.7298</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.013024</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.022364</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.20014</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.030605</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.037319</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.18729</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.010366</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.019881</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.19867</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >2.188</td><td align="center" valign="middle" >2.2167</td><td align="center" valign="middle" >2.2018</td><td align="center" valign="middle" >2.161</td><td align="center" valign="middle" >2.2159</td><td align="center" valign="middle" >.2029</td><td align="center" valign="middle" >1.7367</td><td align="center" valign="middle" >2.2124</td><td align="center" valign="middle" >2.2105</td><td align="center" valign="middle" >2.2166</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table">Table </xref>5</label><caption><title> Standard deviation of the parameter estimates of the two, three and four dimensional models where, 2Dim = two dimensional model, 3Dim = three dimensional model and 4Dim = four dimensional model</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par.</th><th align="center" valign="middle"  colspan="9"  >Misclassification probability and model.</th></tr></thead><tr><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td></tr><tr><td align="center" valign="middle" >ε</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.0014753</td><td align="center" valign="middle" >0.0042391</td><td align="center" valign="middle" >0.0066601</td><td align="center" valign="middle" >0.0014404</td><td align="center" valign="middle" >0.0050092</td><td align="center" valign="middle" >0.0081937</td><td align="center" valign="middle" >0.0010274</td><td align="center" valign="middle" >0.01126</td><td align="center" valign="middle" >0.047973</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.0024073</td><td align="center" valign="middle" >0.0031445</td><td align="center" valign="middle" >0.0090772</td><td align="center" valign="middle" >0.0023992</td><td align="center" valign="middle" >0.0032744</td><td align="center" valign="middle" >0.010904</td><td align="center" valign="middle" >0.0022198</td><td align="center" valign="middle" >0.0060073</td><td align="center" valign="middle" >0.044444</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.0046921</td><td align="center" valign="middle" >0.0048705</td><td align="center" valign="middle" >0.015706</td><td align="center" valign="middle" >0.0046184</td><td align="center" valign="middle" >0.0048262</td><td align="center" valign="middle" >0.018881</td><td align="center" valign="middle" >0.0037478</td><td align="center" valign="middle" >0.0067691</td><td align="center" valign="middle" >0.077563</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.0038545</td><td align="center" valign="middle" >0.0049281</td><td align="center" valign="middle" >0.0093312</td><td align="center" valign="middle" >0.0037818</td><td align="center" valign="middle" >0.0056181</td><td align="center" valign="middle" >0.011074</td><td align="center" valign="middle" >0.0029132</td><td align="center" valign="middle" >0.010631</td><td align="center" valign="middle" >0.040697</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0079028</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0091772</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.017635</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.037529</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.043826</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.11707</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0064795</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0077986</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.012364</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >0.01685</td><td align="center" valign="middle" >0.024641</td><td align="center" valign="middle" >0.039134</td><td align="center" valign="middle" >0.016008</td><td align="center" valign="middle" >0.028788</td><td align="center" valign="middle" >0.046484</td><td align="center" valign="middle" >0.0076039</td><td align="center" valign="middle" >0.057059</td><td align="center" valign="middle" >0.16838</td></tr></tbody></table></table-wrap><p>theoretical parameters, λ L = 0.2 , λ G = 0.12 , π = 0.8999 , z = 0.2144 , R ∗ = 1.1653 , we simulate household epidemic, estimate the parameters of the models and examined their precision from the plots of the root mean square error for misclassification probabilities region ε ∈ [ 0,0.1 ) (<xref ref-type="table" rid="table">Table </xref>6).</p><p><xref ref-type="fig" rid="fig9">Figure 9</xref> shows Plots of the RMSE of the Parameter Estimates when, λ L = 0.2 , λ G = 0.12 , π = 0.8999 , z = 0.2144 , R ∗ = 1.1653 .</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows Plots of the RMSE of the Parameter Estimates when λ L = 0.1 , λ G = 0.29 , π = 0.4199 , z = 0.7298 , R ∗ = 2.2166 .</p><table-wrap id="table6" ><label><xref ref-type="table" rid="table">Table </xref>6</label><caption><title> Root mean square error of the parameter estimates of the two, three and four dimensional models where, 2Dim = two dimensional model, 3Dim = three dimensional model and 4Dim = four dimensional model</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Par.</th><th align="center" valign="middle"  colspan="9"  >Misclassification probability and model.</th></tr></thead><tr><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td><td align="center" valign="middle" >2Dim</td><td align="center" valign="middle" >3Dim</td><td align="center" valign="middle" >4Dim</td></tr><tr><td align="center" valign="middle" >ε</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.2</td></tr><tr><td align="center" valign="middle" >λ ^ L</td><td align="center" valign="middle" >0.006111</td><td align="center" valign="middle" >0.0042409</td><td align="center" valign="middle" >0.0073379</td><td align="center" valign="middle" >0.011422</td><td align="center" valign="middle" >0.0050042</td><td align="center" valign="middle" >0.0086443</td><td align="center" valign="middle" >0.069397</td><td align="center" valign="middle" >0.011252</td><td align="center" valign="middle" >0.049154</td></tr><tr><td align="center" valign="middle" >λ ^ G</td><td align="center" valign="middle" >0.0037761</td><td align="center" valign="middle" >0.0031442</td><td align="center" valign="middle" >0.0073379</td><td align="center" valign="middle" >0.0062438</td><td align="center" valign="middle" >0.0032715</td><td align="center" valign="middle" >0.0086443</td><td align="center" valign="middle" >0.041142</td><td align="center" valign="middle" >0.0060135</td><td align="center" valign="middle" >0.049154</td></tr><tr><td align="center" valign="middle" >π ^</td><td align="center" valign="middle" >0.0048073</td><td align="center" valign="middle" >0.0048714</td><td align="center" valign="middle" >0.017787</td><td align="center" valign="middle" >0.0051303</td><td align="center" valign="middle" >0.0048218</td><td align="center" valign="middle" >0.02029</td><td align="center" valign="middle" >0.0039827</td><td align="center" valign="middle" >0.0067624</td><td align="center" valign="middle" >0.077793</td></tr><tr><td align="center" valign="middle" >z ^</td><td align="center" valign="middle" >0.0063716</td><td align="center" valign="middle" >0.0049235</td><td align="center" valign="middle" >0.010172</td><td align="center" valign="middle" >0.010457</td><td align="center" valign="middle" >0.0056151</td><td align="center" valign="middle" >0.011675</td><td align="center" valign="middle" >0.092936</td><td align="center" valign="middle" >0.010648</td><td align="center" valign="middle" >0.040714</td></tr><tr><td align="center" valign="middle" >ε ^ F N</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0084544</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0095477</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.017617</td></tr><tr><td align="center" valign="middle" >ε ^ F P</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.04278</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0094679</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.11764</td></tr><tr><td align="center" valign="middle" >ε ^</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0064833</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.0077917</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >N/A</td><td align="center" valign="middle" >0.012423</td><td align="center" valign="middle" >N/A</td></tr><tr><td align="center" valign="middle" >R ^ ∗</td><td align="center" valign="middle" >0.033136</td><td align="center" valign="middle" >0.024617</td><td align="center" valign="middle" >0.041799</td><td align="center" valign="middle" >0.057782</td><td align="center" valign="middle" >0.028766</td><td align="center" valign="middle" >0.048413</td><td align="center" valign="middle" >0.47997</td><td align="center" valign="middle" >0.057153</td><td align="center" valign="middle" >0.16832</td></tr></tbody></table></table-wrap></sec><sec id="s9"><title>9. Results and Discussion</title><p>In Figures 1(a)-(c), we see that the estimates of the local and global infection rates from the two and three dimensional models are biased, while those of the four dimensional models have more variability around their true values.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) and <xref ref-type="fig" rid="fig2">Figure 2</xref>(c), the estimates of the two and three dimensional models are biased and imprecise when the misclassification probabilities are large and far apart from each other as theoretically expected.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b), the scatter points of the estimates from the three and four dimensional models are centered at their true value with less variability for the three dimensional model, while those of the two dimensional model in <xref ref-type="fig" rid="fig3">Figure 3</xref>(c) are biased. The estimates of the three dimensional model are more precise than those of the two and four dimensional models.</p><p>Figures 4(a)-(g) are plots of the root mean square error of the maximum likelihood estimates of the parameters of the three models with regions of precision when the theoretical parameters corresponds z = 0.4275 . We see that the root mean square error of the estimates from the four dimensional model are consistently stable throughout the misclassification probabilities region.</p><p>From <xref ref-type="fig" rid="fig6">Figure 6</xref>(c) the two dimensional models is beginning to struggle fitting to the three four dimensional data when ε = 0.01 , while those of the three and four dimensional models are unbiased and precisely estimated as in <xref ref-type="fig" rid="fig6">Figure 6</xref>(a) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b).</p><p>Figures 5(a)-(g) provides general summary of the properties of the estimates of the three models on four dimensional final size epidemic data. Their behaviours along the diagonal of the misclassification probabilities region [ 0,0.2 ] are similar to those examined along the vertical and horizontal axes of [ 0,0.2 ] but have only chosen to present those of the former to avoid repetition.</p><p>From Figures 7(a)-(c), we see that when ε = 0.02 , the parameter estimates from the two dimensional model become biased and imprecise, while those of the three and four dimensional models are unbiased and precise.</p><p>From <xref ref-type="fig" rid="fig8">Figure 8</xref>(c), we see that estimates from the two dimensional model are biased and imprecise while those from the three and four dimensional models in <xref ref-type="fig" rid="fig8">Figure 8</xref>(a) and <xref ref-type="fig" rid="fig8">Figure 8</xref>(b) are precise and unbiased as expected.</p><p>With large misclassification probability ε = 0.2 the three and four dimensional models are the appropriate fit to three dimensional epidemic data. The three dimensional model with less number of parameters is often chosen in line with the principle of parsimony.</p><p>In Figures 10(a)-(f), similar pattern of behaviour are observed except that the estimates of λ G in <xref ref-type="fig" rid="fig1">Figure 1</xref>0(c) for the four dimensional are less precise than those of the two dimensional model. This may be attributable to the size of the proportion infected z as compared to its behaviour with z = 0.2144 in <xref ref-type="fig" rid="fig9">Figure 9</xref>(c).</p><p>We see from <xref ref-type="table" rid="table">Table </xref>4 that the maximum likelihood estimates of the two dimensional models are precise only when the misclassification probability is close to 0 and hence outperforms the three and four dimensional models, otherwise those of the three and four dimensional models have better precision.</p><p>Also, from the regions where the models outperform each other on the three dimensional final size household epidemic data for the set of theoretical parameters and misclassification probabilities ε ∈ [ 0,0.1 ] , we see that the two dimensional model is sufficient on the three dimensional final size epidemic data if ε is close to 0, while the three and four dimensional model are also sufficient model fits, if the misclassification probability is large.</p><p>The estimates of the two dimensional model are initialized according to [<xref ref-type="bibr" rid="scirp.112779-ref10">10</xref>], with minimum computational cost. For example from the [<xref ref-type="bibr" rid="scirp.112779-ref1">1</xref>] A (H3N2) Tercumseh Michigan epidemic, we found the computational time for the estimates to be 1.2 seconds, while those of the Seattle 1975-9176 B (H1N1) epidemic, [<xref ref-type="bibr" rid="scirp.112779-ref15">15</xref>] is 9 seconds, those of 1978-1979 A (H1N1) epidemic, [<xref ref-type="bibr" rid="scirp.112779-ref15">15</xref>] is 4.2 seconds.</p><p>In summary, the computational time required for convergence of the maximum likelihood estimates depends on the choice of the starting values and population size. With appropriate choice of the starting values away from the boundaries and large population size the computational time is large compared to small population size. However inadequate population size leads to lack of information and hence makes convergence of the estimates impossible.</p></sec><sec id="s10"><title>10. Conclusions and Suggestions</title><p>We observed that, once there is no misclassification error in the final size epidemic data, the best model fit to the two dimensional final size data is the two dimensional model. The model with smaller number of parameters is therefore preferred. Making the two dimensional model the appropriate model fit to two dimensional final size epidemic data if ε = 0 .</p><p>However, if ε is far from 0, then the two dimensional model struggled fitting to three dimensional final size data.</p><p>With increasing ε , it becomes unreliable to use the two dimensional model. The three and four dimensional models provide good fit to the theoretical chi-square distribution in the face of increasing values of the misclassification probabilities.</p><p>Also, with large and different misclassification probabilities far apart from each other, the four dimensional model has precise estimates and therefore outperforms the two and three dimensional models on the four dimensional final size epidemic data as demonstrated.</p><p>With increasing misclassification probabilities, the two and three dimensional models struggled fitting to the four dimensional final size data, with disproportionate parameter estimates.</p><p>In summary, with large misclassification probabilities, the estimates of the four dimensional model are more precise than those from the two and three dimensional models in agreement with the discussion in Subsection 6.1.</p><p>Possible extension includes estimating the shape parameter of the Gamma infectious period distribution, if the infectious period distribution is unknown. For example if Gamma ( a , k / a ) is the assumed infectious period distribution, where k is known, then the shape parameter a can then estimate from the final size epidemic data.</p></sec><sec id="s11"><title>Acknowledgements</title><p>The authors will like to acknowledge Dr. Owen D. Lyne and Professor Martin Ridout for their valuable contributions.</p></sec><sec id="s12"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s13"><title>Cite this paper</title><p>Abdulkarim, U.M. (2021) Stochastic SIR Household Epidemic Model with Misclassification. Open Journal of Statistics, 11, 886-905. https://doi.org/10.4236/ojs.2021.115052</p></sec></body><back><ref-list><title>References</title><ref id="scirp.112779-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Addy, C., Longini Jr., I.M. and Haber, M. 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