<?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">ENG</journal-id><journal-title-group><journal-title>Engineering</journal-title></journal-title-group><issn pub-type="epub">1947-3931</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/eng.2017.96032</article-id><article-id pub-id-type="publisher-id">ENG-77032</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Inference and Properties of Mixture Two Extreme Lower Bound Distributions
 
</article-title></title-group><contrib-group><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="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Faculty of Science, Minia University, Minya, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>21</day><month>06</month><year>2017</year></pub-date><volume>09</volume><issue>06</issue><fpage>517</fpage><lpage>523</lpage><history><date date-type="received"><day>May</day>	<month>3,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>June</month>	<year>18,</year>	</date><date date-type="accepted"><day>June</day>	<month>21,</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>
 
 
  In this paper, we discuss the mixture model of two extreme lower bound distributions. First, some properties we obtain of the model with hazard function are discussed. In addition, the estimates of the unknown parameters via the EM algorithm are obtained. The performance of the findings in the paper is showed by demonstrating some numerical illustrations through Monte Carlo simulation.
 
</p></abstract><kwd-group><kwd>Mixture Extreme Lower Bound Distribution</kwd><kwd> Reliability</kwd><kwd> Estimation</kwd><kwd> EM Algorithm</kwd><kwd> Monte Carlo Simulation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Recently, the extreme value distribution is becoming increasingly important in engineering statistics as a suitable model to represent phenomena with usually large maximum observations. In engineering circles, this distribution is often called the extreme lower bound model. It is one of the pioneers of extreme value statistics. The extreme lower bound distribution is one of the probability distributions used to model extreme events. The generalization of the standard extreme lower bound distribution has been introduced by Nadarajah and Kotz [<xref ref-type="bibr" rid="scirp.77032-ref1">1</xref>] and Abd-Elfattah [<xref ref-type="bibr" rid="scirp.77032-ref2">2</xref>] . There are over fifty applications ranging from accelerated life testing through to earthquakes, floods, rain fall, queues in supermarkets, sea currents, wind speeds and track race records, see Kotz and Nadarajah [<xref ref-type="bibr" rid="scirp.77032-ref3">3</xref>] . Mixture models play an important role in many practical applications. For example, direct applications of finite mixture models are in fisheries research, economics, medicine, psychology, palaeoanthropology, botany, agriculture, zoology, life testing and reliability. Direct applications include outliers, Gaussian sums, cluster analysis, latent structure models, modeling prior densities, empirical Bayes method and nonparametric density estimation. In many applications, the available data can be considered as data coming from a mixture population of two or more distributions. This data enables us to mix statistical distributions to get a new distribution which has the properties of its components. For an excellent survey of estimation techniques, discussion and applications, mixture distribution have been considered extensively by many authors, see Titterington [<xref ref-type="bibr" rid="scirp.77032-ref4">4</xref>] , Maclachlan and Basford [<xref ref-type="bibr" rid="scirp.77032-ref5">5</xref>] , Lindsay [<xref ref-type="bibr" rid="scirp.77032-ref6">6</xref>] , Maclachlan and Krishnan [<xref ref-type="bibr" rid="scirp.77032-ref7">7</xref>] and Maclachlan and Peel [<xref ref-type="bibr" rid="scirp.77032-ref8">8</xref>] . Recently, there are many authors [<xref ref-type="bibr" rid="scirp.77032-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.77032-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.77032-ref10">10</xref>] who discuss the mixture models, Mohie El-Din et al. [<xref ref-type="bibr" rid="scirp.77032-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.77032-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.77032-ref13">13</xref>] . In this paper, we discuss some important measures of two extreme lower bound distributions. Also, we estimate the vector of unknown parameters of a mixture model via the EM algorithm proposed by Dempster et al. [<xref ref-type="bibr" rid="scirp.77032-ref9">9</xref>] . Further, we carry out some simulated illustrations using Monte Carlo method.</p></sec><sec id="s2"><title>2. Description of the Model</title><p>The mixture of two extreme lower bound distributions has its pdf as</p><disp-formula id="scirp.77032-formula50"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x2.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x3.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x4.png" xlink:type="simple"/></inline-formula>, the density func- tion of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x5.png" xlink:type="simple"/></inline-formula> component, is given by</p><disp-formula id="scirp.77032-formula51"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x6.png"  xlink:type="simple"/></disp-formula><p>The cdf of the mixture of two extreme lower bound distributions is given by</p><disp-formula id="scirp.77032-formula52"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x7.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x8.png" xlink:type="simple"/></inline-formula>, the cdf <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x9.png" xlink:type="simple"/></inline-formula> component, is given by</p><disp-formula id="scirp.77032-formula53"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x10.png"  xlink:type="simple"/></disp-formula><p>Such that, We study this case, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x11.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x12.png" xlink:type="simple"/></inline-formula> are the parameters unknown and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x13.png" xlink:type="simple"/></inline-formula> is the parameter known.</p></sec><sec id="s3"><title>3. Properties</title><p>In this section we obtain some properties for two extreme lower bound distri- bution by extending the corresponding results of the two parameters extreme lower bound distribution where (2.3) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x14.png" xlink:type="simple"/></inline-formula>is known as follow.</p><sec id="s3_1"><title>3.1. The Expected Value and Variance</title><p>The expected value of the pdf of the two extreme lower bound distribution obtain in (2.1) and (2.3) is</p><disp-formula id="scirp.77032-formula54"><label>(3.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x15.png"  xlink:type="simple"/></disp-formula><p>and the variance is given by</p><disp-formula id="scirp.77032-formula55"><label>(3.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x16.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Mode and Median</title><p>The mode of the mixture of two extreme lower bound distribution is obtained by solving the following nonlinear equation with respect to x</p><disp-formula id="scirp.77032-formula56"><label>(3.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x17.png"  xlink:type="simple"/></disp-formula><p>By using (2.4) and (3.5), the median of the mixture of two extreme lower bound distribution is obtained by solving the following nonlinear equation with respect to x</p><disp-formula id="scirp.77032-formula57"><label>(3.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x18.png"  xlink:type="simple"/></disp-formula><p>From <xref ref-type="table" rid="table1">Table 1</xref>, we obtain the median and the mode of the mixture two extreme lower bound distribution based on different choices of the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x20.png" xlink:type="simple"/></inline-formula> for each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x21.png" xlink:type="simple"/></inline-formula> from this table we observe that the mode is slightly affected by the variation in the values of the mixing proportion<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x22.png" xlink:type="simple"/></inline-formula>, while one mode is stable in the bimodal case. In addition, for unimodal case, the median increases when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x23.png" xlink:type="simple"/></inline-formula> increases. From the bimodal case, we observe that the median decreases when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x24.png" xlink:type="simple"/></inline-formula> icreases.</p></sec><sec id="s3_3"><title>3.3. Reliability and Failure Rate Function</title><p>The reliability function of the mixture two extreme lower bound distribution is given by</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The median and the mode of the mixture of two extreme lower bound distribution</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Bimodel case</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x25.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >(0.2, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >(0.4, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >(0.6, 2.5, 2, 1, 2.9)</td></tr><tr><td align="center" valign="middle" >Median</td><td align="center" valign="middle" >1.0286</td><td align="center" valign="middle" >0.9201</td><td align="center" valign="middle" >0.7852</td></tr><tr><td align="center" valign="middle" >Mode</td><td align="center" valign="middle" >0.326, 0.885</td><td align="center" valign="middle" >0.326, 0.863</td><td align="center" valign="middle" >0.326, 0.798</td></tr><tr><td align="center" valign="middle" >Unimodel case</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x26.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >(0.2, 1, 2, 2, 3)</td><td align="center" valign="middle" >(0.4, 1, 2, 2, 3)</td><td align="center" valign="middle" >(0.6, 1, 2, 2, 3)</td></tr><tr><td align="center" valign="middle" >Median</td><td align="center" valign="middle" >0.635</td><td align="center" valign="middle" >0.733</td><td align="center" valign="middle" >0.882</td></tr><tr><td align="center" valign="middle" >Mode</td><td align="center" valign="middle" >0.459</td><td align="center" valign="middle" >0.469</td><td align="center" valign="middle" >0.882</td></tr></tbody></table></table-wrap><disp-formula id="scirp.77032-formula58"><label>(3.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x27.png"  xlink:type="simple"/></disp-formula><p>By using (2.4) and (3.5) it can be seen the failure rate function (hazard rate function) of the mixture two extreme lower bound distribution is given by</p><disp-formula id="scirp.77032-formula59"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x28.png"  xlink:type="simple"/></disp-formula><p>Which can be written as</p><disp-formula id="scirp.77032-formula60"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x29.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.77032-formula61"><graphic  xlink:href="http://html.scirp.org/file/1-8102606x30.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.77032-formula62"><graphic  xlink:href="http://html.scirp.org/file/1-8102606x31.png"  xlink:type="simple"/></disp-formula><p>The failure rate function of the mixture two extreme lower bound distribution given in (3. 10) satisfies the following limits</p><disp-formula id="scirp.77032-formula63"><label>(3.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x32.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s4"><title>4. Estimation via EM Algorithm</title><p>The EM algorithm provides a simple computational method for fitting mixture models. We use the EM algorithm to estimate the parameters of the pdf of the mixture two extreme lower bound distribution which given in (2.1) and (2.3). We focus in this section, the Maximum likelihood fitting of two extreme lower bound distributions mixture via the EM algorithm. Maclachlan and Peel [<xref ref-type="bibr" rid="scirp.77032-ref9">9</xref>] , the essential nature of the algorithm is the alternation of expectation and maximization steps.</p><disp-formula id="scirp.77032-formula64"><label>(4.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x33.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.77032-formula65"><label>(4.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x34.png"  xlink:type="simple"/></disp-formula><p>then, Concerning the E-step on the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x35.png" xlink:type="simple"/></inline-formula> iteration, the updated estimate of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x36.png" xlink:type="simple"/></inline-formula> mixing proportion <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x37.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.77032-formula66"><label>(4.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x38.png"  xlink:type="simple"/></disp-formula><p>From (4.13) we obtain the M-step of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x39.png" xlink:type="simple"/></inline-formula> iteration, the updated estimates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x41.png" xlink:type="simple"/></inline-formula> for each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x42.png" xlink:type="simple"/></inline-formula> are obtained, respectively, by solving the following systems of equations</p><disp-formula id="scirp.77032-formula67"><label>(4.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x43.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.77032-formula68"><label>(4.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x44.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.77032-formula69"><label>(4.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8102606x45.png"  xlink:type="simple"/></disp-formula><p>The estimates of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x46.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x47.png" xlink:type="simple"/></inline-formula> are obtained by solving (4.15), (4.17) and (4.18). Equations (4.15) and (4.17) are written explicitly but Equation (4.18) has to be solved numerically with random choices of the initial values.</p></sec><sec id="s5"><title>5. Numerical Illustration</title><p>In order to calculate the estimates of the five parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x48.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x49.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x50.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x51.png" xlink:type="simple"/></inline-formula> are known that appear in the pdf of the mixture two extreme lower bound distribution given in (2.1) and (2.3) by using EM algorithm in a Monte Carlo simulation as follows:</p><p>Generate random sample of size <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x52.png" xlink:type="simple"/></inline-formula> and 100 from the mixture two extreme lower bound distribution distribution with for each choice of the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x53.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x54.png" xlink:type="simple"/></inline-formula>. Some of choices caver the unimodal case and other caver the bimodal case.</p><p>The random samples of the mixtures are generated with respect to two uniform variables <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula>. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x57.png" xlink:type="simple"/></inline-formula>, then use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x58.png" xlink:type="simple"/></inline-formula> to generate a random variable x from the mixture two extreme lower bound distribution by using (3.5) as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x59.png" xlink:type="simple"/></inline-formula>, but if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x60.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x61.png" xlink:type="simple"/></inline-formula>.</p><p>The bias and the mean square errors of the estimates are calculated based on 10,000 Monte Carlo simulation and the results are illustrated in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="table" rid="table3">Table 3</xref>. We see that in most of the considered cases, the mean square errors of the estimated parameters decrease as n increase.</p></sec><sec id="s6"><title>6. Conclusion</title><p>In this paper, the behaviors of the mode and median of the mixture two extreme</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Bais of the estimate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x62.png" xlink:type="simple"/></inline-formula> based on EM algorithm</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Bimodal</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x63.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x64.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x65.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x66.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x67.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x68.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x69.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >(0.2, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >−0.116</td><td align="center" valign="middle" >−1.204</td><td align="center" valign="middle" >−0.313</td><td align="center" valign="middle" >0.299</td><td align="center" valign="middle" >−1.203</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >−0.056</td><td align="center" valign="middle" >−1.189</td><td align="center" valign="middle" >−0.333</td><td align="center" valign="middle" >0.313</td><td align="center" valign="middle" >−1.242</td></tr><tr><td align="center" valign="middle" >(0.4, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >−0.068</td><td align="center" valign="middle" >−0.770</td><td align="center" valign="middle" >−0.411</td><td align="center" valign="middle" >0.729</td><td align="center" valign="middle" >−1.309</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >−0.001</td><td align="center" valign="middle" >−0.757</td><td align="center" valign="middle" >−0.421</td><td align="center" valign="middle" >0.743</td><td align="center" valign="middle" >−1.333</td></tr><tr><td align="center" valign="middle" >(0.6, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >−0.614</td><td align="center" valign="middle" >−0.398</td><td align="center" valign="middle" >0.894</td><td align="center" valign="middle" >−1.270</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.015</td><td align="center" valign="middle" >−0.611</td><td align="center" valign="middle" >−0.379</td><td align="center" valign="middle" >0.886</td><td align="center" valign="middle" >−1.295</td></tr><tr><td align="center" valign="middle" >Unimodal</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x70.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x71.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x72.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x73.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x74.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x75.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x76.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >(0.2, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >−0.042</td><td align="center" valign="middle" >0.864</td><td align="center" valign="middle" >0.487</td><td align="center" valign="middle" >−0.136</td><td align="center" valign="middle" >−0.514</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >−0.025</td><td align="center" valign="middle" >0.850</td><td align="center" valign="middle" >0.423</td><td align="center" valign="middle" >−0.131</td><td align="center" valign="middle" >−0.542</td></tr><tr><td align="center" valign="middle" >(0.4, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >0.565</td><td align="center" valign="middle" >−0.019</td><td align="center" valign="middle" >−0.483</td><td align="center" valign="middle" >−1.025</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >0.569</td><td align="center" valign="middle" >−0.015</td><td align="center" valign="middle" >−0.438</td><td align="center" valign="middle" >−0.101</td></tr><tr><td align="center" valign="middle" >(0.6, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.024</td><td align="center" valign="middle" >0.465</td><td align="center" valign="middle" >−0.089</td><td align="center" valign="middle" >−0.613</td><td align="center" valign="middle" >−1.170</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >0.494</td><td align="center" valign="middle" >−0.074</td><td align="center" valign="middle" >−0.573</td><td align="center" valign="middle" >−1.132</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> MSE of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x77.png" xlink:type="simple"/></inline-formula> based on EM algorithm</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Unimodal</th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x78.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x79.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x80.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x81.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x82.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x83.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x84.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >(0.2, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.025</td><td align="center" valign="middle" >1.0002</td><td align="center" valign="middle" >0.1003</td><td align="center" valign="middle" >0.098</td><td align="center" valign="middle" >1.003</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >1.0001</td><td align="center" valign="middle" >0.120</td><td align="center" valign="middle" >0.095</td><td align="center" valign="middle" >1.0001</td></tr><tr><td align="center" valign="middle" >(0.4, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.202</td><td align="center" valign="middle" >1.127</td><td align="center" valign="middle" >0.1003</td><td align="center" valign="middle" >0.200</td><td align="center" valign="middle" >2.005</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.309</td><td align="center" valign="middle" >1.0007</td><td align="center" valign="middle" >0.1001</td><td align="center" valign="middle" >0.199</td><td align="center" valign="middle" >2.002</td></tr><tr><td align="center" valign="middle" >(0.6, 2.5, 2, 1, 2.9)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >0.377</td><td align="center" valign="middle" >0.108</td><td align="center" valign="middle" >0.798</td><td align="center" valign="middle" >2.002</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.369</td><td align="center" valign="middle" >0.1008</td><td align="center" valign="middle" >0.789</td><td align="center" valign="middle" >2.000</td></tr><tr><td align="center" valign="middle" >Unimodal</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x85.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x86.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x87.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x88.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x89.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x90.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8102606x91.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >(0.2, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.0021</td><td align="center" valign="middle" >0.7002</td><td align="center" valign="middle" >0.2384</td><td align="center" valign="middle" >0.0189</td><td align="center" valign="middle" >0.2005</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.0005</td><td align="center" valign="middle" >0.7003</td><td align="center" valign="middle" >0.1798</td><td align="center" valign="middle" >0.0183</td><td align="center" valign="middle" >0.2004</td></tr><tr><td align="center" valign="middle" >(0.4, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.0084</td><td align="center" valign="middle" >0.5987</td><td align="center" valign="middle" >0.0725</td><td align="center" valign="middle" >0.0482</td><td align="center" valign="middle" >0.5000</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.0024</td><td align="center" valign="middle" >0.5169</td><td align="center" valign="middle" >0.0248</td><td align="center" valign="middle" >0.0430</td><td align="center" valign="middle" >0.5023</td></tr><tr><td align="center" valign="middle" >(0.6, 1, 2, 2, 3)</td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >0.0020</td><td align="center" valign="middle" >0.2145</td><td align="center" valign="middle" >0.0083</td><td align="center" valign="middle" >0.3001</td><td align="center" valign="middle" >1.000</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >0.0002</td><td align="center" valign="middle" >0.2003</td><td align="center" valign="middle" >0.0061</td><td align="center" valign="middle" >0.3000</td><td align="center" valign="middle" >0.9998</td></tr></tbody></table></table-wrap><p>lower bound distribution are investigated, based on different choices of the parameters. Also, the behaviors of the failure rate function are discussed through some different graphs. In addition, the estimation of the unknown parameters is obtained using the EM algorithm. Finally, a Monte Carlo simulation based on 10,000 runs is carried out.</p></sec><sec id="s7"><title>Cite this paper</title><p>Riad, F.A. (2017) Inference and Properties of Mixture Two Extreme Lower Bound Distributions. Engineering, 9, 517-523. https://doi.org/10.4236/eng.2017.96032</p></sec></body><back><ref-list><title>References</title><ref id="scirp.77032-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Abd-Elfattah, A.M. and Omima, A.M. (2009) Estimation of the Unknown Parameters of the Generalized Frechet Distribution. Journal of Applied Sciences Research, 5, 1398-1408.</mixed-citation></ref><ref id="scirp.77032-ref2"><label>2</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Dempster</surname><given-names> A. 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