<?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">JCC</journal-id><journal-title-group><journal-title>Journal of Computer and Communications</journal-title></journal-title-group><issn pub-type="epub">2327-5219</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jcc.2017.57011</article-id><article-id pub-id-type="publisher-id">JCC-76359</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  Algorithms of Confidence Intervals of WG Distribution Based on Progressive Type-II Censoring Samples
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohamed</surname><given-names>A. El-Sayed</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fathy</surname><given-names>H. Riad</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>M.</surname><given-names>A. Elsafty</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>Yarub</surname><given-names>A. Estaitia</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Mathematics and Statistics, Faculty of Science, Taif University, Taif, KSA</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Science, Fayoum University, Fayoum, Egypt</addr-line></aff><aff id="aff4"><addr-line>Department of Computer Science, College of Computers and IT, Taif University, Taif, KSA</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics, Faculty of Science, Minia University, Minia, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>drmasayed@yahoo.com(MAE)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>05</month><year>2017</year></pub-date><volume>05</volume><issue>07</issue><fpage>101</fpage><lpage>116</lpage><history><date date-type="received"><day>1,</day>	<month>March</month>	<year>2017</year></date><date date-type="rev-recd"><day>20,</day>	<month>May</month>	<year>2017</year>	</date><date date-type="accepted"><day>23,</day>	<month>May</month>	<year>2017</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 purpose of this article offers different algorithms of Weibull Geometric (WG) distribution estimation depending on the progressive Type II censoring samples plan, spatially the joint confidence intervals for the parameters. The approximate joint confidence intervals for the parameters, the approximate confidence regions and percentile bootstrap intervals of confidence are discussed, and several Markov chain Monte Carlo (MCMC) techniques are also presented. The parts of mean square error (MSEs) and credible intervals lengths, the estimators of Bayes depend on non-informative implement more effective than the maximum likelihood estimates (MLEs) and bootstrap. Comparing the models, the MSEs, average confidence interval lengths of the MLEs, and Bayes estimators for parameters are less significant for censored models.
 
</p></abstract><kwd-group><kwd>Algorithms</kwd><kwd> Simulations</kwd><kwd> Point Estimation</kwd><kwd> Confidence Intervals</kwd><kwd> Bootstrap</kwd><kwd> Approximate Bayes Estimators</kwd><kwd> MCMC</kwd><kwd> MLEs</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The statistical distributions have a very important location of computer branches because of the great number of their particular applications. Being applied to images using Weibull distribution, the structured masks yield good results for the diagnosis of the early Alzheimer’s disease [<xref ref-type="bibr" rid="scirp.76359-ref1">1</xref>] . The paper [<xref ref-type="bibr" rid="scirp.76359-ref2">2</xref>] explores the relationship between the visible content and the real image statistics sampled by the integrated Weibull distribution. It presents a strong relationship between the brain and the parameters’ values using brain images. Moreover, the study discusses a simulated model of parameters estimated from the producer of EEG responses [<xref ref-type="bibr" rid="scirp.76359-ref3">3</xref>] .</p><p>The Weibull distributions display significant statistics―because of their large number of particular features, and practitioners―due to their efficiency to suit data from several scopes, beginning with real data in life, to observation made in economics, weather data, acceptance sampling, hydrology, biology etc. [<xref ref-type="bibr" rid="scirp.76359-ref4">4</xref>] . The article deals with the Weibull-geometric (WG) distribution.</p><p>The Weibull-geometric (WG), Exponential-Poisson (EP), Weibull-Power-Se- ries (WPS), Complementary-Exponential-geometric (CEG), Exponential-Geo- metric (EG), Generalized-Exponential-Power-Series (GEPS), Exponential Weibull-Poisson (EWP), and Generalized-Inverse-Weibull-Poisson (GIWP) distributions are introduced and presented by Adamidis and Loukas [<xref ref-type="bibr" rid="scirp.76359-ref5">5</xref>] , Kus [<xref ref-type="bibr" rid="scirp.76359-ref6">6</xref>] , Chahkandi and Ganjali [<xref ref-type="bibr" rid="scirp.76359-ref7">7</xref>] , Tahmasbi and Rezaei [<xref ref-type="bibr" rid="scirp.76359-ref8">8</xref>] , Barreto [<xref ref-type="bibr" rid="scirp.76359-ref9">9</xref>] , Morais and Barreto [<xref ref-type="bibr" rid="scirp.76359-ref10">10</xref>] , Barreto and Cribari [<xref ref-type="bibr" rid="scirp.76359-ref11">11</xref>] , Louzada et al. [<xref ref-type="bibr" rid="scirp.76359-ref12">12</xref>] , and Cancho et al. [<xref ref-type="bibr" rid="scirp.76359-ref13">13</xref>] . Hamedani and Ahsanullah [<xref ref-type="bibr" rid="scirp.76359-ref14">14</xref>] studied and discussed many properties of WG, such as moments, hazard functions, and functions of order statistics.</p><p>Barreto-Souza [<xref ref-type="bibr" rid="scirp.76359-ref9">9</xref>] suggested and studied the WG distribution. The modified Weibull geometric distribution introduced by composing the modified Weibull and geometric distributions and studied as class of lifetime distributions [<xref ref-type="bibr" rid="scirp.76359-ref15">15</xref>] . MohieEl-Din et al. [<xref ref-type="bibr" rid="scirp.76359-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.76359-ref17">17</xref>] and Elhag et al. [<xref ref-type="bibr" rid="scirp.76359-ref18">18</xref>] studied the confidence intervals for parameters of inverse Weibull distribution based on MLE and bootstrap.</p><p>The paper is organized as follows: the probability density function and cumulative functions of the WG distribution are presented in Section 2. Section 3 provides Markov chain Monte Carlo’s algorithms. The maximum likelihood estimates of the parameters of the WG distribution, the point and interval estimates of the parameters, as well as the approximate joint confidence region are studied in Section 4. The parametric bootstrap confidence intervals of parameters are discussed in Section 5. Bayes estimation of the model parameters and Gibbs sampling algorithm are provided in Section 6. Data analysis and Monte Carlo simulation results are presented in Section 7. Section 8 concludes the paper.</p></sec><sec id="s2"><title>2. WG Distributions</title><p>It is assumed that there are n groups, independent and separated. Each group contains k items that are put in a lifetime test. Consider that the progressive censored scheme R = { R 1 ,   R 2 , ⋯ ,   R m } such that: R 1 represents a set of groups isolated and deleted from the current test, randomly, when the first failure X 1 ;   m ,   n ,   k R takes place. Similarly, R 2 represents a combination of groups and the group that the second failure is observed is deleted from the current test as soon as the second failure X 2 ;   m ,   n ,   k R occurs randomly. In final R m , groups are randomly deleted from the current test when there is an m-th failure X m ; m , n , k R . Therefore, x 1 ;   m ,   n , k R &lt; x 2 ;   m ,   n , k R &lt; ⋯ &lt; x m ;   m ,   n , k R , are known as progressively 1-failure censoring order statistics, where m is the number of the 1-failures 1 &lt; m ≤ n . The relation of the distribution function F ( x ) and probability density function f ( x ) are founded in the function of joint probability density for X 1 ; m , n , k R , X 2 ; m , n , k R , ⋯ , X m ; m , n , k R . The failure times of the k &#215; n items from a continuous population are defined by: (see Balakrishnan and Sandhu [<xref ref-type="bibr" rid="scirp.76359-ref19">19</xref>] )</p><p>f 1 ,   2 , ⋯ ,   m ( x 1 ;   m ,   n , k R ,   x 2 ;   m ,   n , k R , ⋯ ,   x m ;   m ,   n , k R ) = κ k m ∏ i = 1 m f ( x i ;   m ,   n , k R ) [ 1 − F ( x i ;   m ,   n , k R ) ] k ( R i + 1 ) − 1 , 0 &lt; x 1 ;   m ,   n , k R &lt; x 2 ;   m ,   n , k R &lt; ⋯ &lt; x m ;   m ,   n , k R &lt; ∞ , (1)</p><p>and</p><p>κ = n ( n − R 1 − 1 ) ( n − R 1 − R 2 − 2 ) ⋯ ( n − R 1 − R 2 − ⋯ − R m − 1 − m − 1 ) . (2)</p><p>There are special cases of the progressive first-failure censoring scheme of Equation (1) as follows:</p><p>1) When R = { 0 ,   0 , ⋯ ,   0 } , the first-failure censoring scheme is obtained.</p><p>2) When k = 1 , the censoring order statistics of progressive Type II is found.</p><p>3) When R = { 0 ,   0 , ⋯ ,   0 } and k = 1 , sampling case in the complete form is obtained.</p><p>Generally, the progressively first-failure censoring order statistics X 1 ;   m ,   n ,   k R ,   X 2 ;   m ,   n ,   k R , ⋯ ,   X m ;   m ,   n ,   k R can be represented as a censoring order statistics of progressive Type II from the size of a population with function of distribution 1 − ( 1 − F ( x ) ) k . Hence, the results of progressive type II can be expanded to progressive first-failure censoring order statistic easily. The testing time in the progressive first-failure-censoring plan is reduced with n &#215; k items, which contains only m failures.</p><p>The probability density function (pdf) of the WG distribution is represented by the following equation:</p><p>f ( x ) = α β ( 1 − p ) ( β x ) α − 1 e − ( β x ) α / ( 1 − p e − ( β x ) α ) 2 , x &gt; 0 , (3)</p><p>and the cumulative distribution function (cdf) of the WG distribution is shown by:</p><p>F ( x ) = ( 1 − e − ( β x ) α ) / ( 1 − p e − ( β x ) α ) , x ≥ 0 , (4)</p><p>where α &gt; 0 ;   β &gt; 0 and p ( 0 &lt; p &lt; 1 ) are parameters. The parameters α and β stand for the shape and scale while p stands for the mixing parameters, respectively.</p><p>The WG distribution in Equation (3) produces some special models as follows:</p><p>1) Weibull distribution, when p = 0 .</p><p>2) WG distribution tends to a distribution that is degenerated in zero, when p → 1 .</p><p>Hence, the parameter p can be explained as a focus parameter or concentration parameter. <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> show the density and cumulative plots</p><p>respectively, with β = 0.9 and α = 5 for the various rates of p. The EG distribution related to two-parameter with decreasing failure rate is introduced by Adamidis and Loukas [<xref ref-type="bibr" rid="scirp.76359-ref5">5</xref>] . When α = 1 and 0 &lt; p &lt; 1 , the exponential geometric (EG) distribution is obtained, and at α = 1 for any p &lt; 1 the EEG distribution is achieved. Therefore, the EEG distribution expands the EG distribution. The Weibull W ( α , β ) distribution is obtained when p goes to zero. <xref ref-type="fig" rid="fig1">Figure 1</xref> plots the WG density for some values of the vector φ = ( β , α ) when p = − 2 , − 0. 5 , 0 , 0. 5 , 0. 9 . For all values of parameters, the density tends to zero as x → ∞ . The density functions of WG are shown. It is noted that the WG density is strictly decreasing when − 1 ≤ p &lt; 1 and α ≤ 1 , and is multimodal when − 1 ≤ p &lt; 1 and α &gt; 1 . The form x 0 = β − 1 u 1 / α is obtained when solution is arrived of the following nonlinear formulation:</p><p>u + p − 1 e u ( u − 1 + 1 / α ) = − 1 + 1 / α (5)</p><p>The WG density can be unimodal when p &lt; − 1 . For instance, when p &lt; − 1 and α = 1 , the EEG distribution is unimodal. The hazard and survival functions of X are:</p><p>h ( t ) = α β ( p − 1 ) ( β t ) α − 1 / ( p e − ( β t ) α − 1 − 1 ) (6)</p><p>and</p><p>S ( t ) = − 1 + ( e − ( β t ) α − 1 ) / ( p e − ( β t ) α − 1 − 1 ) , (7)</p></sec><sec id="s3"><title>3. Markov Chain Monte Carlo Algorithms</title><p>Markov chain Monte Carlo (MCMC) technique has spread widely for Bayesian calculation in compound statistical modeling. In general, it gives a beneficial application for real statistical modeling (Gilks et al. [<xref ref-type="bibr" rid="scirp.76359-ref20">20</xref>] ; Gamerman, [<xref ref-type="bibr" rid="scirp.76359-ref21">21</xref>] ).</p><p>Markov Chain is a randomly determined and stochastic process, having a random probability distribution or pattern that may be resolved statistically in that future cases are independent of previous cases specified the current case.</p><p>Monte Carlo chain is an emulation and simulation, therefore; it used to solve integrals to some extent rather than analyze performance, a procedure named integration of Monte Carlo. In this way, interested quantities of a distribution can be picked from emulated draws and charts from the distribution. Bayesian test needs integration over probably high-dimension of probability distributions to produce predictions or to yield inference and deduction about parameters of model. Basically, Monte Carlo integration is utilized with chains of Markov in MCMC techniques. The patterns of integration draw from the desired distribution, and then form pattern rates to sacrificial expectations (see Geman [<xref ref-type="bibr" rid="scirp.76359-ref22">22</xref>] ; Metropolis et al. [<xref ref-type="bibr" rid="scirp.76359-ref23">23</xref>] ; and Hastings [<xref ref-type="bibr" rid="scirp.76359-ref24">24</xref>] ).</p><sec id="s3_1"><title>3.1. MH Procedure</title><p>The Metropolis-Hastings (MH) procedure is employed by Metropolis et al. [<xref ref-type="bibr" rid="scirp.76359-ref23">23</xref>] . It is assumed that the main target here is to design samples from the distribution f ( τ | x ) = l ℘ ( τ ) , where l is the normal fixed value which may be hard to calculate or found. MH procedure gives a method of sampling from f ( τ | x ) without the need to inform l . Suppose that ℏ ( τ ( b ) | τ ( a ) ) is an optional transition kernel, where the probability of jumping, or moving, from existing case τ ( a ) to τ ( b ) , known as the suggestion or proposal distribution. The MH Algorithm generates values sequence τ ( 1 ) ,   τ ( 2 ) , ⋯ form a Markov chain with stable distribution given by f ( τ | x ) .</p><p>When the proposal distribution is symmetric, so ℏ ( τ | η ) = ℏ ( η | τ ) for all</p><p>possible η and τ then, in particular, the result is ℏ ( τ ( t − 1 ) | τ ∗ ) = ℏ ( τ ∗ | τ ( t − 1 ) ) ,</p><p>so that the acceptance probability (5) is given by</p><p>χ ( τ ( t − 1 ) ,   τ ∗ ) = min [ 1 ,   f ( τ ∗ | x ) f ( τ ( t − 1 ) | x ) ] . (9)</p></sec><sec id="s3_2"><title>3.2. GS Procedure</title><p>Gibbs’ sampler (GS) procedure is a straightforward branch of MCMC algorithms. This procedure was implemented by Geman [<xref ref-type="bibr" rid="scirp.76359-ref22">22</xref>] . The significance of Gibbs’ procedure for area of issues in Bayesian analysis is explained by Gelfand and Smith [<xref ref-type="bibr" rid="scirp.76359-ref25">25</xref>] . The complete conditional distribution forms the transition kernel, so Gibbs sampler procedure is a MCMC planner.</p><p>The three unknown parameters of WG distribution will be studied through the various algorithms of estimation based on progressive Type-II censoring. The MCMC procedures are used with Bayesian technique to produce from the posterior distributions.</p></sec></sec><sec id="s4"><title>4. MLE of WG Distribution</title><p>This section determines the maximum likelihood estimates (MLEs) of the WG distribution parameters. Let’s assume that X i = X i ;   m ,   n R ,   i = 1 ,   2 , ⋯ ,   m are the progressive first-failure censoring order statistics from a WG distribution, with censoring plane R. Using Equations (1)-(3), the function of likelihood is shown by:</p><p>L ( α ,   β ,   p | x _ ) = κ α m β α m ( 1 − p ) n &#215; exp ( ( α − 1 ) ∑ i = 1 m log x i − ∑ i = 1 m ( β x i ) α ( R i + 1 ) )     &#215; ∏ i = 1 m [ 1 − p exp ( − ( β x i ) α ) ] − ( R i + 2 ) (10)</p><p>where κ is given in (2). The logarithm of the function of likelihood may be obtained as follow:</p><p>l ( α ,   β ,   p | x _ ) = m log α + m α log β + n log ( 1 − p )     + ( α − 1 ) ∑ i = 1 m log x i − ∑ i = 1 m ( β x i ) α ( R i + 1 )     − ∑ i = 1 m ( R i + 2 ) log ( 1 − p exp ( − ( β x i ) α ) ) . (11)</p><p>Compute the derivatives ∂ l ∂ α , ∂ l ∂ β and ∂ l p α , then put each equation equal</p><p>to zero, the likelihood equations can be obtained in the following:</p><p>∂ l ( α , β , p | x _ ) ∂ α = m α + m log β + ∑ i = 1 m log x i − ∑ i = 1 m ( R i + 1 ) ( β x i ) α log ( β x i )                                               − p ∑ i = 1 m ( R i + 2 ) ( β x i ) α log ( β x i ) exp ( − ( β x i ) α ) 1 − p exp ( − ( β x i ) α ) = 0 , (12)</p><p>∂ l ( α ,   β ,   p | x _ ) ∂ β = m α β − α ∑ i = 1 m ( R i + 1 ) x i ( β x i ) α − 1                                             − p α ∑ i = 1 m ( R i + 2 ) x i ( β x i ) α − 1 exp ( − ( β x i ) α ) 1 − p exp ( − ( β x i ) α ) = 0 (13)</p><p>and</p><p>∂ l ( α ,   β ,   p | x _ ) ∂ p = − n 1 − p + ∑ i = 1 m ( R i + 2 ) exp ( − ( β x i ) α ) 1 − p exp ( − ( β x i ) α ) = 0 , (14)</p><p>The analytical solution of α ^ ,   β ^ and p ^ in Equations (12)-(14) is very difficult. Hence, some numerical techniques like Newton’s method may be used.</p><p>From the function of log-likelihood in (11), the Fisher information matrix I ( α ,   β ,   p ) is obtained by taking expectation of minus Equations (12)-(14). Under some mild regularity conditions, ( α ^ , β ^ , p ^ ) are approximately normal bivariate with the means ( α ,   β ,   p ) and covariance matrix I − 1 ( α ,   β ,   p ) . Commonly, in practice, I − 1 ( α ,   β ,   p ) is estimated by I − 1 ( α ^ ,   β ^ ,   p ^ ) . This procedure is simpler and valid to employ the approximation.</p><p>( α ^ ,   β ^ ,   p ^ ) → N ( ( α ,   β ,   p ) ,   I 0 − 1 ( α ^ ,   β ^ ,   p ^ ) ) , (15)</p><p>where I 0 ( α ,   β ,   p ) is observed as information matrix.</p><p>I 0 − 1 ( α ^ ,   β ^ ,   p ^ ) = [ − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ α 2 − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ α ∂ β − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ α ∂ p − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ β ∂ α − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ β 2 − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ β ∂ p − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ p ∂ α − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ p ∂ β − ∂ 2 l ( x _ ; α ,   β ,   p ) ∂ p 2 ] ( α ^ ,   β ^ , p ^ ) − 1 = [ var ( α ^ ) cov ( α ^ ,   β ^ ) cov ( α ^ ,   p ^ ) cov ( β ^ ,   α ^ ) var ( β ^ ) cov ( β ^ ,   p ^ ) cov ( p ^ ,   α ^ ) cov ( p ^ ,   β ^ ) var ( p ^ ) ] . (16)</p><p>Confidence intervals can be calculated approximately for α , β and p to be bivariate normal distributed with the means ( α ,   β ,   p ) and covariance matrix I 0 − 1 ( α ^ ,   β ^ ,   p ^ ) . Hence, the 100 ( 1 − α ) % confidence intervals approximately for α , β and p are</p><p>α ^ &#177; z α 2 v 11   , β ^ &#177; z α 2 v 22 and p ^ &#177; z α 2 v 33 (17)</p><p>respectively, where the values v 11 , v 22 and v 33 are on the major diagonal of the covariance matrix I 0 − 1 ( α ^ ,   β ^ ,   p ^ ) and z α 2 is the percentage of the standard</p><p>normal distribution with right-tail probability α 2 .</p></sec><sec id="s5"><title>5. Intervals of Bootstrap Confidence</title><p>The bootstrap technique is used for resampling in statistical inference cases. It is usually utilized to evaluate confidence regions and it can be applied to evaluate bias and variance of a calibrator or estimator assumption tests. Additional scanning of the parametric and nonparametric bootstrap technique is applied, see Davison and Hinkley [<xref ref-type="bibr" rid="scirp.76359-ref26">26</xref>] , and Elhag et al. [<xref ref-type="bibr" rid="scirp.76359-ref27">27</xref>] . The parametric bootstrap technique of the two confidence intervals is suggested. The algorithm for evaluating the confidence intervals of parameters uses both Efron and Tibshirani procedures [<xref ref-type="bibr" rid="scirp.76359-ref28">28</xref>] , and bootstrap-t Hall procedure [<xref ref-type="bibr" rid="scirp.76359-ref20">20</xref>] . The Bootstrap sampling algorithm for estimating the confidence intervals of parameters is illustrated below.</p><p>Percentile bootstrap confidence interval: Assume that G ( y ) = P ( φ ^ j ∗ ≤ y ) is the cumulative distribution function of φ ^ j ∗ . Determine φ ^ j b o o t ∗ = G − 1 ( y ) for the given y. The bootstrap confidence interval approximately with 100 ( 1 − γ ) % of φ ^ j ∗ may be obtained as follows:</p><p>[ φ ^ j b o o t ∗ ( γ 2 ) ,   φ ^ j b o o t ∗ ( 1 − γ 2 ) ] . (18)</p><p>First, locate the sort statistics δ j ∗ [ 1 ] &lt; δ j ∗ [ 2 ] &lt; ⋯ &lt; δ j ∗ [ N ] , wherever</p><p>δ k ∗ [ i ] = φ ^ j ∗ [ i ] − φ ^ j var ( φ ^ j ∗ [ i ] ) ,   i = 1 ,   2 , ⋯ ,   N ,   j = 1 ,   2 ,   3 , (19)</p><p>and φ ^ 1 = α ^ , φ ^ 2 = β ^ , φ ^ 3 = p ^ .</p><p>Consider that H ( y ) = P ( δ j ∗ &lt; y ) is the cumulative distribution function of δ j ∗ . If y is given, then</p><p>φ ^ j b o o t − t = φ ^ j + var ( φ ^ j ) H − 1 ( y ) . (20)</p></sec><sec id="s6"><title>6. Bayes Estimation of the Model Parameters</title><p>In the consideration that each of the parameters α , β and p are unknown, it may be considered that the joint prior density is a product of gamma density of α and β uniform prior of p, where</p><p>π 1 ( α ) = b a Γ ( a ) α a − 1 exp ( − b α ) ,   α &gt; 0 ,   ( a , b &gt; 0 ) , (21)</p><p>π 2 ( β ) = d c Γ ( c ) β c − 1 exp ( − d β ) ,   β &gt; 0 ,   ( c ,   d &gt; 0 ) , (22)</p><p>and</p><p>π 3 ( p ) = 1 (23)</p><p>By multiplying π 1 ( α ) by π 2 ( β ) and π 3 ( p ) , we get the joint prior density of α , β and p computed by</p><p>π ( α ,   β ,   p ) = b a d c Γ ( a ) Γ ( c ) α a − 1 β c − 1 exp ( − ( b α + d β ) ) ,   ( α ,   β &gt; 0 and 0 ≤ p ≤ 1 ) . (24)</p><p>Based on the prior of joint distribution of α , β and p the posterior of joint density function of α , β and p known as the data, indicated by π ∗ ( α ,   β ,   p | x _ ) can be expressed as follows:</p><p>π ∗ ( α ,   β ,   p | x _ ) = L ( α ,   β ,   p | x _ ) &#215; π ( α ,   β ,   p ) ∫ 0 ∞ ∫ 0 ∞ ∫ 0 ∞ L ( α ,   β ,   p | x _ ) &#215; π ( α ,   β ,   p ) d α d β d p . (25)</p><p>Hence, using squared error loss function (SEL) of any function φ ( α ,   β ,   p ) , the Bayes estimate of α , β and p can be expressed as</p><p>φ ^ ( α ,   β ,   p ) = E α ,   β ,   p | x _ ( φ ( α ,   β ,   p ) ) = ∫ 0 ∞ ∫ 0 ∞ ∫ 0 ∞ φ ( α ,   β ,   p ) L ( α ,   β ,   p | x _ ) &#215; π ( α ,   β ,   p ) d α d β d p ∫ 0 ∞ ∫ 0 ∞ ∫ 0 ∞ L ( α ,   β ,   p | x _ ) &#215; π ( α ,   β ,   p ) d α d β d p (26)</p><p>In general, the value of two integrals specified by (26) cannot be acquired in a cleared and closed format. In this situation, the MCMC procedure is used to create patterns from the posterior distributions and; therefore, is calculated the Bayes estimator of φ ( α ,   β ,   p ) along with the function of SEL. A wide diversity of MCMC techniques is available and can be troublesome to select any of them. A significant type of MCMC technique is Gibbs samplers and widespread Metropolis within-Gibbs samplers.</p><p>The MCMC procedure has the advantage over the MLE procedure that we can permanently gain an appropriate estimation of intervals of the parameters by building the probability intervals and using the experimental posterior distribution.</p><p>This, sometimes, is not obtainable in MLE. The samples of MCMC can be utilized to fully brief the uncertainty of posterior about the parameters α , β and p , by using a kernel estimation of the posterior distribution.</p><p>The function of joint posterior density of α , β and p may be described as</p><p>π ∗ ( α ,   β ,   p | x _ ) ∝ α m + a − 1 β α m + c − 1 ( 1 − p ) n exp { − b α − d β + α ∑ i = 1 m log x i     − ∑ i = 1 m ( R i + 2 ) log [ 1 − p exp ( − ( β x i ) α ) ] − ∑ i = 1 m ( R i + 1 ) ( β x i ) α } . (27)</p><p>The conditional posterior PDF’s of α , β and p are shown as</p><p>π 1 ∗ ( α | β ,   p ,   x _ ) ∝ α m + a − 1 exp { α ( m log β − b + ∑ i = 1 m log x i )                                                 − ∑ i = 1 m ( R i + 2 ) log [ 1 − p exp ( − ( β x i ) α ) ] − ∑ i = 1 m ( R i + 1 ) ( β x i ) α } , (28)</p><p>π 2 ∗ ( β | α ,   p ,   x _ ) ∝ β α m + c − 1 exp { − d β − ∑ i = 1 m ( R i + 2 ) log [ 1 − p exp ( − ( β x i ) α ) ]                                               − ∑ i = 1 m ( R i + 1 ) ( β x i ) α } , (29)</p><p>and</p><p>π 3 ∗ ( p | α ,   β ,   x _ ) ∝ ( 1 − p ) n exp { − ∑ i = 1 m ( R i + 2 ) log [ 1 − p exp ( − ( β x i ) α ) ] } . (30)</p><p>The Metropolis-Hastings procedure [<xref ref-type="bibr" rid="scirp.76359-ref23">23</xref>] with normal proposal distribution under the Gibbs sampler algorithm is described as follows:</p></sec><sec id="s7"><title>7. Illustrative Example and Simulation Studies</title><p>To explain the procedures evolved of estimation in this paper, gamma distribution for given hybrid parameters ( a = 1.5 , b = 1 ) is used and produce sample of</p><p>space 10, randomly (21), the average of the sample α ≅ 1 10 ∑ i = 1 10   α i , is computed</p><p>and supposed as the real population rate of α = 1.5 . So that they are obtained to</p><p>verify E ( α ) = b a ≅ α with the past parameters is nearly the average of gamma</p><p>distribution. Similarly, when the valued c = 2 and d = 1 are given, create π 2 ( β ) based on the last β = 2 , from gamma distribution (22). The previously</p><p>parameters selected to verify E ( β ) = d c ≅ β , are nearly the average of gamma</p><p>distribution. A progressive Type II samples are created by employing the procedures of Balakrishnan and Sandhu [<xref ref-type="bibr" rid="scirp.76359-ref19">19</xref>] from WG distribution with the available data: 0.0409, 0.0552, 0.0561, 0.0726, 0.0776, 0.0840, 0.0906, 0.1108, 0.1291, 0.1502, 0.1513, 0.1540, 0.1624, 0.1691, 0.1930, 0.2175, 0.2188, 0.2700, 0.2709, 0.2994, 0.3219, 0.3342, 0.4065, 0.4396, 0.5385, and under the parameters; ( α = 1.5 , p = 0.6 , β = 2 , m = n = 50 and R = { 2 , 0 , 2 , 0 , 1 , 0 , 2 , 0 , 0 , 3 , 0 , 0 , 2 , 0 , 2 , 0 , 1 , 0 , 3 , 0 , 3 , 0 , 2 , 0 , 2 } ).</p><p>The approximate bootstrap, Bayes estimates and MLEs are calculated of α , β , and p under these data utilizing MCMC algorithm outputs are explained in <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>. <xref ref-type="table" rid="table2">Table 2</xref> yield the 95%, approximate confidence intervals of two bootstrap, approximate credible and MLE under the MCMC samples. Studies of simulation have been executed employing Mathematica ver. 9.0 for explaining the theoretic outcomes of estimates issue. The accomplishment of the performing estimators of the parameters has been supposed in valued of their mean square error (MSE) and average (AVG), where</p><p>φ ^ k &#175; = 1 M ∑ i = 1 M     φ ^ k ( i ) ,   ( φ 1 = α ,   φ 2 = β ,   φ 3 = p ) , (34)</p><p>and</p><p>MSE = 1 M ∑ i = 1 M ( φ ^ k ( i ) − φ k ) 2 . (35)</p><p>In studies of simulation, the researchers assume that the population parameter rates ( α = 0.5 ,   β = 1.5 ,   p = 0.1 ) , various sample values n, different effected sample size m and different censored scheme R . For computing Bayes estimators, without loss of generality using non-informative priors, ( a = 0.0001 , b = 0.0001 , c = 0.0001 , d = 0.0001 ). Under function of squared error loss, the researchers calculate the Bayes estimations. The estimations of Bayes and 95% credible intervals using 11,000 sets of MCMC are also calculated. The mean Bayes estima-</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Show the parameters estimation of WG distribution</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Procedure</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x231.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x232.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x233.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >(.)<sub>ML</sub></td><td align="center" valign="middle" >1.6178</td><td align="center" valign="middle" >1.9614</td><td align="center" valign="middle" >0.4566</td></tr><tr><td align="center" valign="middle" >(.)<sub>Boot</sub></td><td align="center" valign="middle" >1.8122</td><td align="center" valign="middle" >2.2451</td><td align="center" valign="middle" >0.7724</td></tr><tr><td align="center" valign="middle" >(.)<sub>MCMC</sub></td><td align="center" valign="middle" >1.6299</td><td align="center" valign="middle" >1.9787</td><td align="center" valign="middle" >0.4727</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Show the CIs using Bootstrap, Bootstrap-t and MLE according to 500 times</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Procedure</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x234.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x235.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x236.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >(.)ML</td><td align="center" valign="middle" >(1.1424, 2.0931)</td><td align="center" valign="middle" >(1.3282, 2.5946)</td><td align="center" valign="middle" >(0.4654, 0.9210)</td></tr><tr><td align="center" valign="middle" >(.)Boot</td><td align="center" valign="middle" >(1.0004, 2.3599)</td><td align="center" valign="middle" >(1.1012, 2.5840)</td><td align="center" valign="middle" >(0.4655, 0.8821)</td></tr><tr><td align="center" valign="middle" >(.)Boot-t</td><td align="center" valign="middle" >(1.1235, 2.0147)</td><td align="center" valign="middle" >(0.8561, 2.6523)</td><td align="center" valign="middle" >(0.1361, 0.8111)</td></tr><tr><td align="center" valign="middle" >(.)MCMC</td><td align="center" valign="middle" >(1.1444, 1.9440)</td><td align="center" valign="middle" >(0.9569, 2.5709)</td><td align="center" valign="middle" >(0.0361, 0.7768)</td></tr></tbody></table></table-wrap><p>tions, MSEs, coverage percentages, and average lengths of confidence interval based on 500 times are reported.</p><p>Comparatively, the MLEs with the 95% confidence intervals are calculated based on the observation of Fisher information matrix and two bootstrap confidences. <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref> report the outputs based on MLEs and the Bayes estimations utilizing both the Gibbs sampling algorithm and MH algorithm:</p><p>1) From <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref>, in parts of MSEs and credible intervals lengths, the estimators of Bayes depend on non-informative implement more effective than the MLEs and bootstrap.</p><p>2) From <xref ref-type="table" rid="table3">Table 3</xref> and <xref ref-type="table" rid="table4">Table 4</xref>, comparing the models, the MSEs, average confidence interval lengths of the MLEs, and Bayes estimators for parameters are less significant for censored models ( n − m ,   0 , ⋅ ⋅ ⋅ ,   0 ) .</p><p>3) The MSE and average confidence interval lengths nearly reduce the estimators in whole situations when the performance sample rate n / m raises.</p></sec><sec id="s8"><title>8. Conclusion</title><p>Several algorithms of estimation of WG distribution, based on the progressive Type II censored sampling plan, are discussed. The joint confidence intervals for the parameters are also studied. The approximate confidence regions, percentile bootstrap confidence intervals, as well as approximate joint confidence region</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Show the various estimators average values and the identical MSEs when α = 0.5 , β = 1.5 and p = 0.1 </title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >m (scheme)</th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x241.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x242.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x243.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x244.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x245.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x246.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x247.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x248.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x249.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x250.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x251.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x252.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (15, 14<sup>0</sup>)</td><td align="center" valign="middle" >0.6245</td><td align="center" valign="middle" >1.6664</td><td align="center" valign="middle" >0.1021</td><td align="center" valign="middle" >0.7241</td><td align="center" valign="middle" >1.4217</td><td align="center" valign="middle" >0.1539</td><td align="center" valign="middle" >0.5241</td><td align="center" valign="middle" >1.4399</td><td align="center" valign="middle" >0.1597</td></tr><tr><td align="center" valign="middle" >0.1234</td><td align="center" valign="middle" >0.4736</td><td align="center" valign="middle" >0.0664</td><td align="center" valign="middle" >0.2235</td><td align="center" valign="middle" >0.4840</td><td align="center" valign="middle" >0.1021</td><td align="center" valign="middle" >0.1200</td><td align="center" valign="middle" >0.1914</td><td align="center" valign="middle" >0.1056</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (15<sup>1</sup>)</td><td align="center" valign="middle" >0.6754</td><td align="center" valign="middle" >1.6828</td><td align="center" valign="middle" >0.1016</td><td align="center" valign="middle" >0.6788</td><td align="center" valign="middle" >1.4027</td><td align="center" valign="middle" >0.1482</td><td align="center" valign="middle" >0.5751</td><td align="center" valign="middle" >1.4194</td><td align="center" valign="middle" >0.1533</td></tr><tr><td align="center" valign="middle" >0.2101</td><td align="center" valign="middle" >0.5398</td><td align="center" valign="middle" >0.0614</td><td align="center" valign="middle" >0.2479</td><td align="center" valign="middle" >0.5438</td><td align="center" valign="middle" >0.0906</td><td align="center" valign="middle" >0.1101</td><td align="center" valign="middle" >0.4530</td><td align="center" valign="middle" >0.0936</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (14<sup>0</sup>, 15)</td><td align="center" valign="middle" >0.5364</td><td align="center" valign="middle" >1.7667</td><td align="center" valign="middle" >0.1001</td><td align="center" valign="middle" >0.5388</td><td align="center" valign="middle" >1.3614</td><td align="center" valign="middle" >0.1554</td><td align="center" valign="middle" >0.5064</td><td align="center" valign="middle" >1.3977</td><td align="center" valign="middle" >0.1621</td></tr><tr><td align="center" valign="middle" >0.2351</td><td align="center" valign="middle" >0.7337</td><td align="center" valign="middle" >0.0707</td><td align="center" valign="middle" >0.3331</td><td align="center" valign="middle" >0.8748</td><td align="center" valign="middle" >0.1069</td><td align="center" valign="middle" >0.1111</td><td align="center" valign="middle" >0.5925</td><td align="center" valign="middle" >0.1105</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (10, 19<sup>0</sup>)</td><td align="center" valign="middle" >0.6200</td><td align="center" valign="middle" >1.6165</td><td align="center" valign="middle" >0.1023</td><td align="center" valign="middle" >0.7070</td><td align="center" valign="middle" >1.4327</td><td align="center" valign="middle" >0.1432</td><td align="center" valign="middle" >0.5205</td><td align="center" valign="middle" >1.4424</td><td align="center" valign="middle" >0.1471</td></tr><tr><td align="center" valign="middle" >0.1088</td><td align="center" valign="middle" >0.3890</td><td align="center" valign="middle" >0.0623</td><td align="center" valign="middle" >0.1282</td><td align="center" valign="middle" >0.3347</td><td align="center" valign="middle" >0.0874</td><td align="center" valign="middle" >0.0988</td><td align="center" valign="middle" >0.3389</td><td align="center" valign="middle" >0.0596</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (1, 0, ・・・, 1, 0)</td><td align="center" valign="middle" >0.6151</td><td align="center" valign="middle" >1.6173</td><td align="center" valign="middle" >0.1024</td><td align="center" valign="middle" >0.6999</td><td align="center" valign="middle" >1.4234</td><td align="center" valign="middle" >0.1404</td><td align="center" valign="middle" >0.5151</td><td align="center" valign="middle" >1.4322</td><td align="center" valign="middle" >0.1439</td></tr><tr><td align="center" valign="middle" >0.1901</td><td align="center" valign="middle" >0.4028</td><td align="center" valign="middle" >0.057</td><td align="center" valign="middle" >0.2220</td><td align="center" valign="middle" >0.4500</td><td align="center" valign="middle" >0.0793</td><td align="center" valign="middle" >0.1102</td><td align="center" valign="middle" >0.3543</td><td align="center" valign="middle" >0.0511</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (19<sup>0</sup>, 10)</td><td align="center" valign="middle" >0.6164</td><td align="center" valign="middle" >1.6782</td><td align="center" valign="middle" >0.0968</td><td align="center" valign="middle" >0.7162</td><td align="center" valign="middle" >1.4204</td><td align="center" valign="middle" >0.1400</td><td align="center" valign="middle" >0.5146</td><td align="center" valign="middle" >1.4375</td><td align="center" valign="middle" >0.1443</td></tr><tr><td align="center" valign="middle" >0.2225</td><td align="center" valign="middle" >0.5091</td><td align="center" valign="middle" >0.0577</td><td align="center" valign="middle" >0.2335</td><td align="center" valign="middle" >0.6194</td><td align="center" valign="middle" >0.0813</td><td align="center" valign="middle" >0.1325</td><td align="center" valign="middle" >0.4272</td><td align="center" valign="middle" >0.0537</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (30, 29<sup>0</sup>)</td><td align="center" valign="middle" >0.5777</td><td align="center" valign="middle" >1.7881</td><td align="center" valign="middle" >0.0974</td><td align="center" valign="middle" >0.7357</td><td align="center" valign="middle" >1.4828</td><td align="center" valign="middle" >0.1297</td><td align="center" valign="middle" >0.5577</td><td align="center" valign="middle" >1.4934</td><td align="center" valign="middle" >0.1320</td></tr><tr><td align="center" valign="middle" >0.1100</td><td align="center" valign="middle" >0.7534</td><td align="center" valign="middle" >0.054</td><td align="center" valign="middle" >0.2102</td><td align="center" valign="middle" >0.7296</td><td align="center" valign="middle" >0.0707</td><td align="center" valign="middle" >0.0985</td><td align="center" valign="middle" >0.6377</td><td align="center" valign="middle" >0.0518</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (1<sup>30</sup>)</td><td align="center" valign="middle" >0.6360</td><td align="center" valign="middle" >1.9606</td><td align="center" valign="middle" >0.094</td><td align="center" valign="middle" >0.5399</td><td align="center" valign="middle" >1.5464</td><td align="center" valign="middle" >0.1233</td><td align="center" valign="middle" >0.6355</td><td align="center" valign="middle" >1.5575</td><td align="center" valign="middle" >0.1254</td></tr><tr><td align="center" valign="middle" >0.1840</td><td align="center" valign="middle" >1.0418</td><td align="center" valign="middle" >0.0447</td><td align="center" valign="middle" >0.1990</td><td align="center" valign="middle" >0.9999</td><td align="center" valign="middle" >0.0570</td><td align="center" valign="middle" >0.1000</td><td align="center" valign="middle" >0.8539</td><td align="center" valign="middle" >0.0480</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (29<sup>0</sup>, 30)</td><td align="center" valign="middle" >0.6321</td><td align="center" valign="middle" >2.1049</td><td align="center" valign="middle" >0.0950</td><td align="center" valign="middle" >0.6355</td><td align="center" valign="middle" >1.4381</td><td align="center" valign="middle" >0.1320</td><td align="center" valign="middle" >0.6333</td><td align="center" valign="middle" >1.4661</td><td align="center" valign="middle" >0.1351</td></tr><tr><td align="center" valign="middle" >0.2114</td><td align="center" valign="middle" >1.5074</td><td align="center" valign="middle" >0.0548</td><td align="center" valign="middle" >0.2554</td><td align="center" valign="middle" >1.5381</td><td align="center" valign="middle" >0.0741</td><td align="center" valign="middle" >0.2000</td><td align="center" valign="middle" >1.2615</td><td align="center" valign="middle" >0.0758</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Show the coverage percentages and average confidence interval, when α = 0.5 , β = 1.5 and p = 0.1 </title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >m (scheme)</th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x255.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x256.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="3"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x257.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x258.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x259.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x260.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x261.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x262.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x263.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x264.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x265.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1730585x266.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (15, 14<sup>0</sup>)</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.923</td><td align="center" valign="middle" >0.87</td><td align="center" valign="middle" >0.892</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.86</td><td align="center" valign="middle" >0.9021</td><td align="center" valign="middle" >0.916</td><td align="center" valign="middle" >0.936</td></tr><tr><td align="center" valign="middle" >0.7502</td><td align="center" valign="middle" >1.6373</td><td align="center" valign="middle" >0.2507</td><td align="center" valign="middle" >0.9840</td><td align="center" valign="middle" >1.8201</td><td align="center" valign="middle" >0.3503</td><td align="center" valign="middle" >0.7001</td><td align="center" valign="middle" >1.5616</td><td align="center" valign="middle" >0.3504</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (15<sup>1</sup>)</td><td align="center" valign="middle" >0.901</td><td align="center" valign="middle" >0.923</td><td align="center" valign="middle" >0.874</td><td align="center" valign="middle" >0.9011</td><td align="center" valign="middle" >0.963</td><td align="center" valign="middle" >0.894</td><td align="center" valign="middle" >0.910</td><td align="center" valign="middle" >0.952</td><td align="center" valign="middle" >0.952</td></tr><tr><td align="center" valign="middle" >0.8821</td><td align="center" valign="middle" >1.9465</td><td align="center" valign="middle" >0.2358</td><td align="center" valign="middle" >0.9991</td><td align="center" valign="middle" >2.012</td><td align="center" valign="middle" >0.4458</td><td align="center" valign="middle" >0.8111</td><td align="center" valign="middle" >1.8784</td><td align="center" valign="middle" >0.3231</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >15 (14<sup>0</sup>, 15)</td><td align="center" valign="middle" >0.880</td><td align="center" valign="middle" >0.908</td><td align="center" valign="middle" >0.886</td><td align="center" valign="middle" >0.874</td><td align="center" valign="middle" >0.918</td><td align="center" valign="middle" >0.896</td><td align="center" valign="middle" >0.891</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.939</td></tr><tr><td align="center" valign="middle" >0.9921</td><td align="center" valign="middle" >2.5915</td><td align="center" valign="middle" >0.3571</td><td align="center" valign="middle" >1.001</td><td align="center" valign="middle" >2.5313</td><td align="center" valign="middle" >0.4574</td><td align="center" valign="middle" >0.8821</td><td align="center" valign="middle" >2.4269</td><td align="center" valign="middle" >0.3695</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (10, 19<sup>0</sup>)</td><td align="center" valign="middle" >0.911</td><td align="center" valign="middle" >0.945</td><td align="center" valign="middle" >0.883</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.947</td><td align="center" valign="middle" >0.890</td><td align="center" valign="middle" >0.924</td><td align="center" valign="middle" >0.943</td><td align="center" valign="middle" >0.936</td></tr><tr><td align="center" valign="middle" >0.7001</td><td align="center" valign="middle" >1.4041</td><td align="center" valign="middle" >0.2222</td><td align="center" valign="middle" >0.8801</td><td align="center" valign="middle" >1.3331</td><td align="center" valign="middle" >0.3332</td><td align="center" valign="middle" >0.3001</td><td align="center" valign="middle" >1.3522</td><td align="center" valign="middle" >0.2932</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (1, 0, ・・・, 1, 0)</td><td align="center" valign="middle" >0.905</td><td align="center" valign="middle" >0.962</td><td align="center" valign="middle" >0.895</td><td align="center" valign="middle" >0.915</td><td align="center" valign="middle" >0.920</td><td align="center" valign="middle" >0.905</td><td align="center" valign="middle" >0.932</td><td align="center" valign="middle" >0.958</td><td align="center" valign="middle" >0.943</td></tr><tr><td align="center" valign="middle" >0.7721</td><td align="center" valign="middle" >1.5183</td><td align="center" valign="middle" >0.2133</td><td align="center" valign="middle" >0.8723</td><td align="center" valign="middle" >1.6683</td><td align="center" valign="middle" >0.2442</td><td align="center" valign="middle" >0.7028</td><td align="center" valign="middle" >1.4749</td><td align="center" valign="middle" >0.2778</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >20 (19<sup>0</sup>, 10)</td><td align="center" valign="middle" >0.891</td><td align="center" valign="middle" >0.963</td><td align="center" valign="middle" >0.857</td><td align="center" valign="middle" >0.901</td><td align="center" valign="middle" >0.980</td><td align="center" valign="middle" >0.889</td><td align="center" valign="middle" >0.901</td><td align="center" valign="middle" >0.968</td><td align="center" valign="middle" >0.965</td></tr><tr><td align="center" valign="middle" >0.9823</td><td align="center" valign="middle" >1.9051</td><td align="center" valign="middle" >0.2237</td><td align="center" valign="middle" >0.9977</td><td align="center" valign="middle" >1.9352</td><td align="center" valign="middle" >0.2299</td><td align="center" valign="middle" >0.7023</td><td align="center" valign="middle" >1.8133</td><td align="center" valign="middle" >0.302</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (30, 29<sup>0</sup>)</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.943</td><td align="center" valign="middle" >0.855</td><td align="center" valign="middle" >0.906</td><td align="center" valign="middle" >0.955</td><td align="center" valign="middle" >0.921</td><td align="center" valign="middle" >0.935</td><td align="center" valign="middle" >0.945</td><td align="center" valign="middle" >0.946</td></tr><tr><td align="center" valign="middle" >0.6002</td><td align="center" valign="middle" >2.4938</td><td align="center" valign="middle" >0.1935</td><td align="center" valign="middle" >0.6880</td><td align="center" valign="middle" >2.8888</td><td align="center" valign="middle" >0.1991</td><td align="center" valign="middle" >0.5001</td><td align="center" valign="middle" >1.4563</td><td align="center" valign="middle" >0.2011</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (1<sup>30</sup>)</td><td align="center" valign="middle" >0.925</td><td align="center" valign="middle" >0.946</td><td align="center" valign="middle" >0.873</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.920</td><td align="center" valign="middle" >0.913</td><td align="center" valign="middle" >0.965</td><td align="center" valign="middle" >0.959</td><td align="center" valign="middle" >0.975</td></tr><tr><td align="center" valign="middle" >0.7522</td><td align="center" valign="middle" >3.4213</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.7588</td><td align="center" valign="middle" >1.4211</td><td align="center" valign="middle" >0.118</td><td align="center" valign="middle" >0.6122</td><td align="center" valign="middle" >1.4142</td><td align="center" valign="middle" >0.223</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >30 (29<sup>0</sup>, 30)</td><td align="center" valign="middle" >0.901</td><td align="center" valign="middle" >0.945</td><td align="center" valign="middle" >0.855</td><td align="center" valign="middle" >0.921</td><td align="center" valign="middle" >0.944</td><td align="center" valign="middle" >0.952</td><td align="center" valign="middle" >0.933</td><td align="center" valign="middle" >0.956</td><td align="center" valign="middle" >0.956</td></tr><tr><td align="center" valign="middle" >0.7923</td><td align="center" valign="middle" >1.1995</td><td align="center" valign="middle" >0.1061</td><td align="center" valign="middle" >0.8925</td><td align="center" valign="middle" >1.1997</td><td align="center" valign="middle" >0.1880</td><td align="center" valign="middle" >0.6982</td><td align="center" valign="middle" >1.0515</td><td align="center" valign="middle" >0.260</td></tr></tbody></table></table-wrap><p>for the parameters are expanded and developed. Some numerical examples with actual data set and simulated data are used to compare the proposed joint confidence regions. The parts of MSEs and credible intervals lengths, the estimators of Bayes depend on non-informative implement more effective than the MLEs and bootstrap. Comparing the models, the MSEs, average confidence interval lengths of the MLEs, and Bayes estimators for parameters are less significant for censored models.</p></sec><sec id="s9"><title>Cite this paper</title><p>El-Sayed, M.A., Riad, F.H., Elsafty, M.A. and Estaitia, Y.A. (2017) Algorithms of Confidence Intervals of WG Distribution Based on Progressive Type-II Censoring Samples. Journal of Computer and Communications, 5, 101- 116. https://doi.org/10.4236/jcc.2017.57011</p></sec></body><back><ref-list><title>References</title><ref id="scirp.76359-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Al-jibory, W.K.S. and EI-Zaart, A. 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