<?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">IIM</journal-id><journal-title-group><journal-title>Intelligent Information Management</journal-title></journal-title-group><issn pub-type="epub">2160-5912</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/iim.2016.82003</article-id><article-id pub-id-type="publisher-id">IIM-65015</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>
 
 
  Semi-Markovian Model of Two-Line Queuing System with Losses
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uriy</surname><given-names>E. Obzherin</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Higher Mathematics, Sevastopol State University, University STR, Sevastopol, 
Russian Federation</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>vmsevntu@mail.ru</email></corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>03</month><year>2016</year></pub-date><volume>08</volume><issue>02</issue><fpage>17</fpage><lpage>26</lpage><history><date date-type="received"><day>18</day>	<month>January</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>22</month>	<year>March</year>	</date><date date-type="accepted"><day>25</day>	<month>March</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In the present paper, to build model of two-line queuing system with losses GI/G/2/0, the approach introduced by V.S. Korolyuk and A.F. Turbin, is used. It is based on application of the theory of semi-Markov processes with arbitrary phase space of states. This approach allows us to omit some restrictions. The stationary characteristics of the system have been defined, assuming that the incoming flow of requests and their service times have distributions of general form. The particular cases of the system were considered. The used approach can be useful for modeling systems of various purposes.
 
</p></abstract><kwd-group><kwd>Two-Line Queuing System with Losses</kwd><kwd> Semi-Markov Process</kwd><kwd> Stationary Distribution of  Embedded Markov Chain</kwd><kwd> Stationary Characteristics of System</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A large number of works, in particular [<xref ref-type="bibr" rid="scirp.65015-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] , have been dedicated to the queuing systems (QS) with losses. Building of QS models and determining their characteristics are simplified, if it is assumed that the incoming flow of requests or their service times are exponentially distributed. The rejection of this assumption leads to a considerable complication of the models. In this paper, the model of two-line QS with losses was built on the assumption that the incoming flow of requests and their service times have distributions of general form. For building QS model and determining its stationary characteristics, the theory of semi-Markov processes with arbitrary phase state space [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.65015-ref10">10</xref>] was used.</p></sec><sec id="s2"><title>2. System Description and Building of the Semi-Markov Model</title><p>Two-line QS with losses GI/G/2/0 is being considered. It is assumed that the system receives requests, and the time between their arrival is a random variable (RV) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x6.png" xlink:type="simple"/></inline-formula>with the distribution function (DF)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x7.png" xlink:type="simple"/></inline-formula>. A received request, with equal probability, starts to be served by one of the available servers or gets lost, if no servers are available. The service time of request by the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x8.png" xlink:type="simple"/></inline-formula> server-RV <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x9.png" xlink:type="simple"/></inline-formula> with DF<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x10.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x11.png" xlink:type="simple"/></inline-formula>. It is assumed that RV<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x12.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x13.png" xlink:type="simple"/></inline-formula>are independent, and have densities<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x14.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x15.png" xlink:type="simple"/></inline-formula>, finite mathematical expectations and variances.</p><p>To describe the QS operation, the semi-Markov process [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.65015-ref7">7</xref>] <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x16.png" xlink:type="simple"/></inline-formula>with the following set of states is used:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x17.png" xlink:type="simple"/></inline-formula>.</p><p>The meaning of state codes is the following:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x18.png" xlink:type="simple"/></inline-formula>: first (second) server started serving the received request, and second (first) server is available;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x19.png" xlink:type="simple"/></inline-formula>: first (second) server became available; second (first) server is available; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x20.png" xlink:type="simple"/></inline-formula>is the time until the arrival of the next request;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x21.png" xlink:type="simple"/></inline-formula>: first (second) server started serving the received request; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x22.png" xlink:type="simple"/></inline-formula>is the time until the end of the request service by second (first) server;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x23.png" xlink:type="simple"/></inline-formula>: first (second) server became available; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x24.png" xlink:type="simple"/></inline-formula>is the time until the end of the request service by second (first) server; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x25.png" xlink:type="simple"/></inline-formula>is the time until the arrival of the next request;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x26.png" xlink:type="simple"/></inline-formula>: the received request was lost; the times until the end of the request service by first (second) servers are respectively equal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x27.png" xlink:type="simple"/></inline-formula>.</p><p>The time diagram of the system is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>Let us define the sojourn times in states of the system. For instance, the sojourn time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x28.png" xlink:type="simple"/></inline-formula>, in the state <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x29.png" xlink:type="simple"/></inline-formula> is determined by three factors: the time x left until the end of request service by the first server, the time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x30.png" xlink:type="simple"/></inline-formula> of request service by the second server, and the time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x31.png" xlink:type="simple"/></inline-formula> between the request arrivals.</p><p>Therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x32.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x33.png" xlink:type="simple"/></inline-formula> is the minimum sign. Similarly, the sojourn times in other states are determined as follows:</p><disp-formula id="scirp.65015-formula202"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x34.png"  xlink:type="simple"/></disp-formula><p>We define the transition probabilities of the embedded Markov chain (EMC) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x35.png" xlink:type="simple"/></inline-formula>for states <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x36.png" xlink:type="simple"/></inline-formula>, in the context of other states, they are determined similarly.</p><disp-formula id="scirp.65015-formula203"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x37.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The time diagram of the system functioning</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-8701387x38.png"/></fig></sec><sec id="s3"><title>3. Definition of the Stationary Distribution of the Embedded Markov Chain</title><p>We will find the stationary distribution of EMC<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula>. Let us denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula> the values of stationary distribution in states <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x41.png" xlink:type="simple"/></inline-formula> and assume the existence of stationary densities <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x42.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x43.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x44.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x45.png" xlink:type="simple"/></inline-formula>.</p><p>Introduce the notations:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x46.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x47.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x48.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x50.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x51.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x52.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x53.png" xlink:type="simple"/></inline-formula>.</p><p>Using (2), set up a system of integral equations to determine the stationary distribution:</p><disp-formula id="scirp.65015-formula204"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x54.png"  xlink:type="simple"/></disp-formula><p>The last equation in the system (3) is the normalization requirement.</p><p>Next, for the sake of simplicity, a homogenous case is considered, and a inhomogeneous case leads to lengthy transformations and results. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x55.png" xlink:type="simple"/></inline-formula>. Then, due to the symmetry of states, we get that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x56.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x57.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x58.png" xlink:type="simple"/></inline-formula>.</p><p>The system (3) is reduced to the following system of equations:</p><disp-formula id="scirp.65015-formula205"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x59.png"  xlink:type="simple"/></disp-formula><p>Let us introduce the following functions, which are used to record the stationary distribution of EMC:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x60.png" xlink:type="simple"/></inline-formula>―is the density of the renewal function [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x61.png" xlink:type="simple"/></inline-formula>of the renewal process generated by RV<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x62.png" xlink:type="simple"/></inline-formula>;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x63.png" xlink:type="simple"/></inline-formula>―is the density of the direct residual time distribution [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] for the renewal process generated by RV<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x64.png" xlink:type="simple"/></inline-formula>;</p><disp-formula id="scirp.65015-formula206"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x65.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x66.png" xlink:type="simple"/></inline-formula>―is the density of the renewal function, renewal process generated by RV with the distribution density<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x67.png" xlink:type="simple"/></inline-formula>;</p><disp-formula id="scirp.65015-formula207"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x68.png"  xlink:type="simple"/></disp-formula><p>Using the method of successive approximations [<xref ref-type="bibr" rid="scirp.65015-ref12">12</xref>] , we can show that the system (4) has the following solution:</p><disp-formula id="scirp.65015-formula208"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x69.png"  xlink:type="simple"/></disp-formula><p>The constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x70.png" xlink:type="simple"/></inline-formula> is found by means of normalization requirement; its explicit form is not used when finding the QS stationary characteristics.</p><p>The system of equations, which is almost identical to the system (3), and its solution method are covered in [<xref ref-type="bibr" rid="scirp.65015-ref13">13</xref>] .</p></sec><sec id="s4"><title>4. Definition of Stationary Characteristics of System</title><p>Let us turn to the determination of the stationary characteristics of the QS. Using Formulas (1), we will define the average sojourn times in states of the system:</p><disp-formula id="scirp.65015-formula209"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x71.png"  xlink:type="simple"/></disp-formula><p>We divide the set of states E into three following subsets:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x72.png" xlink:type="simple"/></inline-formula>―all servers are available;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x73.png" xlink:type="simple"/></inline-formula>―one server is in service;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x74.png" xlink:type="simple"/></inline-formula>―two servers are in service;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x75.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x76.png" xlink:type="simple"/></inline-formula>.</p><p>We will introduce the transition probabilities of the semi-Markov processes<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x77.png" xlink:type="simple"/></inline-formula>:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x78.png" xlink:type="simple"/></inline-formula>,</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x79.png" xlink:type="simple"/></inline-formula>―stationary probabilities,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x80.png" xlink:type="simple"/></inline-formula>.</p><p>We will show that the stationary probabilities of QS <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x81.png" xlink:type="simple"/></inline-formula> are defined by the following formulas:</p><disp-formula id="scirp.65015-formula210"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x82.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.65015-formula211"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x83.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x84.png" xlink:type="simple"/></inline-formula>―is the renewal function [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] ;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x85.png" xlink:type="simple"/></inline-formula>―is DF of the direct residual time [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] ; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x86.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x87.png" xlink:type="simple"/></inline-formula>―is the mathematical expectation of the direct residual time [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] .</p><p>The proof. As is known [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.65015-ref6">6</xref>] , the following equalities are true:</p><disp-formula id="scirp.65015-formula212"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x88.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x89.png" xlink:type="simple"/></inline-formula>―is the average sojourn time of SMP <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x90.png" xlink:type="simple"/></inline-formula> in state<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x91.png" xlink:type="simple"/></inline-formula>;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x92.png" xlink:type="simple"/></inline-formula>―is the stationary distribution of EMC<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x93.png" xlink:type="simple"/></inline-formula>.</p><p>Let us calculate the integrals entering into the right side of equalities (10). Using (6), (7), we get:</p><disp-formula id="scirp.65015-formula213"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x94.png"  xlink:type="simple"/></disp-formula><p>In the transformations, the following formula was used:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x95.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.65015-formula214"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65015-formula215"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x97.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65015-formula216"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x98.png"  xlink:type="simple"/></disp-formula><p>By substituting the determined expressions in Formulas (10), we get Formulas (8).</p><p>Let us define the stationary probability of request loss. We will consider the subset of states:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x99.png" xlink:type="simple"/></inline-formula>―a received request was lost.</p><p>We will find <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x100.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.65015-formula217"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x101.png"  xlink:type="simple"/></disp-formula><p>Therefore, the stationary probability of request loss equals:</p><disp-formula id="scirp.65015-formula218"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x102.png"  xlink:type="simple"/></disp-formula><p>Important characteristics of the QS under consideration are average stationary sojourn times <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x103.png" xlink:type="simple"/></inline-formula> of the system in the selected subsets of states<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x104.png" xlink:type="simple"/></inline-formula>. To determine them we will use Formulas [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.65015-ref6">6</xref>] :</p><disp-formula id="scirp.65015-formula219"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x105.png"  xlink:type="simple"/></disp-formula><p>Let us find the values of the expressions in the denominators of Formulas (14).</p><disp-formula id="scirp.65015-formula220"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x106.png"  xlink:type="simple"/></disp-formula><p>The transformations used the following formula:</p><disp-formula id="scirp.65015-formula221"><label>, (16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x107.png"  xlink:type="simple"/></disp-formula><p>which results from the first equation of the system (4),</p><disp-formula id="scirp.65015-formula222"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x108.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.65015-formula223"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x109.png"  xlink:type="simple"/></disp-formula><p>In the derivations of equalities (17), (18) Formula (16) was used in the same way.</p><p>Having placed the determined values of the denominators into Formulas (14), we obtain:</p><disp-formula id="scirp.65015-formula224"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-8701387x110.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x111.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x112.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>5. Particular Cases of QS GI/G/2/0</title><p>Let us look at particular cases of QS GI/G/2/0.</p><p>1) We find the stationary characteristics of QS<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x113.png" xlink:type="simple"/></inline-formula>. In this case,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x114.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x115.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x116.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x117.png" xlink:type="simple"/></inline-formula>,</p><p><img data-original="http://html.scirp.org/file/1-8701387x120.png" /><img data-original="http://html.scirp.org/file/1-8701387x119.png" /><img data-original="http://html.scirp.org/file/1-8701387x118.png" /></p><p><img data-original="http://html.scirp.org/file/1-8701387x123.png" /><img data-original="http://html.scirp.org/file/1-8701387x122.png" /><img data-original="http://html.scirp.org/file/1-8701387x121.png" /></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x124.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x125.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x126.png" xlink:type="simple"/></inline-formula>,</p><p><img data-original="http://html.scirp.org/file/1-8701387x128.png" /><img data-original="http://html.scirp.org/file/1-8701387x127.png" /></p><p><img data-original="http://html.scirp.org/file/1-8701387x130.png" /><img data-original="http://html.scirp.org/file/1-8701387x129.png" /></p><p>Using Formulas (8), (13), (19), we obtain:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x131.png" xlink:type="simple"/></inline-formula>.</p><p>2) Let us examine QS M/G/2/0, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x138.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x139.png" xlink:type="simple"/></inline-formula>.</p><p>The direct substitution into the system (4) can show that the stationary distribution of EMC is determined by the formulas:</p><disp-formula id="scirp.65015-formula225"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x140.png"  xlink:type="simple"/></disp-formula><p>Functions (5) in this case are as follows:</p><disp-formula id="scirp.65015-formula226"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x141.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x142.png" xlink:type="simple"/></inline-formula>―is the density of function 1: of renewals [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] ;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x143.png" xlink:type="simple"/></inline-formula>―is the density of function 0: of renewals [<xref ref-type="bibr" rid="scirp.65015-ref11">11</xref>] ;</p><disp-formula id="scirp.65015-formula227"><graphic  xlink:href="http://html.scirp.org/file/1-8701387x144.png"  xlink:type="simple"/></disp-formula><p>Consequently,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x145.png" xlink:type="simple"/></inline-formula>.</p><p>Using Formulas (8), (13), (19), we obtain that the stationary characteristics of QS M/G/2/0 are written as:</p><p><img data-original="http://html.scirp.org/file/1-8701387x147.png" /><img data-original="http://html.scirp.org/file/1-8701387x146.png" /></p><p><img data-original="http://html.scirp.org/file/1-8701387x149.png" /><img data-original="http://html.scirp.org/file/1-8701387x148.png" /></p><p><img data-original="http://html.scirp.org/file/1-8701387x152.png" /><img data-original="http://html.scirp.org/file/1-8701387x151.png" /><img data-original="http://html.scirp.org/file/1-8701387x150.png" /></p><p>Thus, in this case, as shown in [<xref ref-type="bibr" rid="scirp.65015-ref4">4</xref>] , stationary probabilities <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x153.png" xlink:type="simple"/></inline-formula> are invariant under the laws of distribution of service time.</p><p>The semi-Markov model of QS <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x154.png" xlink:type="simple"/></inline-formula> is considered in [<xref ref-type="bibr" rid="scirp.65015-ref14">14</xref>] .</p><p>In the paper [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] , a similar approach to the building of QS model under consideration is used. To find the stationary distribution of EMC, a method based on the usage of taboo-probabilities is applied.</p><p>In monograph [<xref ref-type="bibr" rid="scirp.65015-ref13">13</xref>] , the semi-Markov model of QS <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x155.png" xlink:type="simple"/></inline-formula> is considered and stationary characteristics are defined.</p><p>Using built semi-Markov model, limiting theorems and Markov renewal equations [<xref ref-type="bibr" rid="scirp.65015-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.65015-ref7">7</xref>] , one can find other stationary and non-stationary characteristics of QS<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-8701387x156.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s6"><title>Cite this paper</title><p>Yuriy E. Obzherin, (2016) Semi-Markovian Model of Two-Line Queuing System with Losses. Intelligent Information Management,08,17-26. doi: 10.4236/iim.2016.82003</p></sec></body><back><ref-list><title>References</title><ref id="scirp.65015-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kleinrock, L. (1975) Queueing Systems. Volume 1: Theory. Wiley-Inter Science, New York.</mixed-citation></ref><ref id="scirp.65015-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Gnedenko, B.V. and Kovalenko, I.N. (1987) Introduction to Queueing Theory. Nauka, Moscow.</mixed-citation></ref><ref id="scirp.65015-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Ivchenko, G.I., Kashtanov, V.A. and Kovalenko, I.N. (1982) The Queueing Theory. Vyssh Shk, Moscow.</mixed-citation></ref><ref id="scirp.65015-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Kopp, V.Y., Obzherin, Y.E. and Peschansky, A.I. (2011) Stationary Characteristics of Queueing System GI/M/2/0. Collection of Scientific Papers of Sevastopol National University of Nuclear Energy and Industry, 4, 191-197.</mixed-citation></ref><ref id="scirp.65015-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Obzherin, Y.E. and Boyko, E.G. (2015) Semi-Markov Models: Control of Restorable Systems with Latent Failures. Elsevier Academic Press, London.</mixed-citation></ref><ref id="scirp.65015-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Kantorovich, L.V. and Akilov, G.P. (1977) Functional Analysis. Nauka, Moscow.</mixed-citation></ref><ref id="scirp.65015-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Beichelt, F. and Franken, P. (1988) Reliability and Maintenance. Mathematical Method. Radio I Svyaz Press, Moscow.</mixed-citation></ref><ref id="scirp.65015-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Grabski, F. (2014) Semi-Markov Processes: Applications in System Reliability and Maintenance. Elsevier, Amsterdam.</mixed-citation></ref><ref id="scirp.65015-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Janssen, J. and Raimondo, M. (2006) Applied Semi-Markov Processes. Springer Science and Business Media, New York.</mixed-citation></ref><ref id="scirp.65015-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Janssen, J. and Limnios, N. (1999) Semi-Markov Models and Applications. Kluwer Academic Publishers, Dordrecht.  
http://dx.doi.org/10.1007/978-1-4613-3288-6</mixed-citation></ref><ref id="scirp.65015-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Limnios, N. and Oprisan, G. (2001) Semi-Markov Processes and Reliability. Springer Science and Business Media, New York.</mixed-citation></ref><ref id="scirp.65015-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Koroluk, V.S. and Turbin, A.F. (1982) Markovian Restoration Processes in the Problems of System Reliability. Naukova Dumka, Kiev.</mixed-citation></ref><ref id="scirp.65015-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Korlat, A.N., Kuznetsov, V.N. and Turbin, A.F. (1991) Semi-Markovian Models of Restorable and Service Systems. Shtiintsa, Kishinev.</mixed-citation></ref><ref id="scirp.65015-ref14"><label>14</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Sevastyanov</surname><given-names> B.A. </given-names></name>,<etal>et al</etal>. (<year>1957</year>)<article-title>Ergodic Theorem for Markov Processes and Its Application to Telephone Systems with Rejections</article-title><source> Teor Veroyatnost i Primenen</source><volume> 2</volume>,<fpage> 106</fpage>-<lpage>116</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref></ref-list></back></article>