<?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">OJOp</journal-id><journal-title-group><journal-title>Open Journal of Optimization</journal-title></journal-title-group><issn pub-type="epub">2325-7105</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojop.2012.12006</article-id><article-id pub-id-type="publisher-id">OJOp-26134</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><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Investigation of Probability Generating Function in an Interdependent &lt;i&gt;M/M/&lt;/i&gt;1:(∞; GD) Queueing Model with Controllable Arrival Rates Using Rouche’s Theorem
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ishwa</surname><given-names>Nath Maurya</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>Shekhawati Engineering College, Rajasthan Technical University, Kota, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>prof.drvnmaurya@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>12</month><year>2012</year></pub-date><volume>01</volume><issue>02</issue><fpage>34</fpage><lpage>38</lpage><history><date date-type="received"><day>September</day>	<month>28,</month>	<year>2012</year></date><date date-type="rev-recd"><day>November</day>	<month>2,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>14,</month>	<year>2012</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>
 
 
  Present paper deals a M/M/1:(∞; GD) queueing model with interdependent controllable arrival and service rates
   where
  - 
  in customers arrive in the system according to 
  p
  oisson distribution with two different arrivals rates-slower and faster as per controllable arrival policy. Keeping in view the general trend of interdependent arrival and service processes, it is presumed that random variables of arrival and service processes follow a bivariate 
  p
  oisson distribution and the server provides his services under general discipline of service rule in an infinitely large waiting space. In this paper, our cen
  tral attention is to explore the probability generating functions using Rouche’s theorem in both cases of slower and faster arrival rates of the queueing model taken into consideration; which may be helpful for mathematicians and re
  searchers for establishing significant performance measures of the model. Moreover, for the purpose of high-lighting the application aspect of our investigated result, very recently Maurya [1] has derived successfully the expected busy periods of the server in both cases of slower and faster arrival rates, which have also been presented by the end of this paper. 
     
 
</p></abstract><kwd-group><kwd>Interdependent Queueing Model; Bivariate Poisson Process; Controllable Arrival Rates; Probability Generating Function; Laplace Transform; Rouche’s Theorem; Performance Measures</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The probability generating function approach plays a vital role in the study of queueing problems as it is crucially useful in performance analysis of a wide range of queueing models. As an example, the probability generating function approach facilitates to determine the expected busy and idle periods and system size distribution. In the queueing literature, it has been enthusiastically observed that most of the previous researchers [2-7] and references therein have presumed that the parameters of arrival and service rates in the queueing systems are independent to each other. However, it is not so in general because we find many queueing situations in our real life where the arrival and service rates are correlated with an elevated extent. We remark here that the arrival rate of a variety of queueing systems is usually controlled in order to reduce the queue length. Queueing models with controllable arrival rates have been studied by a few noteworthy researchers [3,8-10] which reveals the fact that there is still an increasing demand of analyzing an interdependent queueing models with controllable arrival rates. Srinivasa Rao et al. [<xref ref-type="bibr" rid="scirp.26134-ref8">8</xref>] have confined to obtain the average system size and average waiting time of an</p><p><img src="4-2730005\c329dc0a-7c7e-424b-af57-db473506f321.jpg" />interdependent queueing model with controllable arrival rates under steady state conditions. Of late, Pal [<xref ref-type="bibr" rid="scirp.26134-ref4">4</xref>] considered the same queueing model which was already examined by Srinivasa Rao et al. [<xref ref-type="bibr" rid="scirp.26134-ref8">8</xref>] with a version of its limited waiting space and he succeeded to investigate the cost per unit time of a served customer in the system. Recently, Thiagarajan M. and Srinivasan A. [<xref ref-type="bibr" rid="scirp.26134-ref9">9</xref>] focused their attention to explore the <img src="4-2730005\7e53fe62-6bc7-400b-b16e-17e8790e8019.jpg" /> interdependent queueing model with bulk arrivals and controllable arrival rates. In this sequential work, we consider here an interdependent <img src="4-2730005\930d1dc8-5456-45d5-9976-a38beb625d8f.jpg" /> queueing model incorporating bivariate Poisson process and controllable arrival rates in order to investigate the probability generating functions in faster and slower arrival rates.</p></sec><sec id="s2"><title>2. Description of the Model</title><p>In the present study, we consider an interdependent <img src="4-2730005\4e1328e2-eb5a-4238-aa2d-fcc2df26b9a0.jpg" /> queueing model with bivariate Poisson process and controllable arrival rates. The arrival pattern of customers are controlled by the system that it allows two arrival rates <img src="4-2730005\d35d6d07-83b6-4d80-8830-e14a498872c8.jpg" /> and<img src="4-2730005\a6767348-7e9e-49a7-881a-d1cab0e252a1.jpg" />;<img src="4-2730005\16045dba-42cc-473f-94f1-a31f4df04c99.jpg" />. Without loss of generality we assume that whenever the system size attains a fixed number S, the arrival rate reduces to <img src="4-2730005\4e81f4fc-a465-4f12-ab7d-8319e36c415c.jpg" /> from <img src="4-2730005\d11753a9-4c31-4c81-92f6-b740d5b7adfe.jpg" /> and the arrival rate <img src="4-2730005\bbf88107-e448-4f6d-87cb-2b1569d68cff.jpg" /> remains unchanged till the system size is greater than<img src="4-2730005\b52a20b8-ffa2-4685-985f-ad5233f99b1e.jpg" />. But as soon as the system size reduces to R, the arrival rate <img src="4-2730005\0af08edc-3a90-4a6d-9ce2-3815a540c5a3.jpg" /> changes back to <img src="4-2730005\e31eb33a-0f23-4724-850e-adf78f84daef.jpg" /> and the same pattern of change of arrival rates is repeated during the complete busy period of the system. Moreover, we assume that both <img src="4-2730005\570c2824-65db-4867-95be-b683dac9ceea.jpg" /> and <img src="4-2730005\7d107ce4-3f85-4e10-97ac-d605ea9a8f43.jpg" /> representing respectively the arrival and service processes are interdependent and these discrete random variables follow a bivariate Poisson distribution [<xref ref-type="bibr" rid="scirp.26134-ref11">11</xref>] with their probability mass function <img src="4-2730005\01bdf2a3-3399-46c2-a7e5-1433bf3d0e16.jpg" /> defined as given below</p><p><img src="4-2730005\bd5789ee-61ee-43d0-85ff-f16c862f15b7.jpg" /></p><p>with following feasible conditions:</p><p><img src="4-2730005\d0cd1821-678d-42d5-8ef0-7694a885f7ce.jpg" /></p><p>and<img src="4-2730005\9f831589-b5f9-4e1a-82f4-5a18f9606839.jpg" />.</p><p>Here <img src="4-2730005\947e3bf1-f8f2-4851-ac69-d1d1af22c986.jpg" /> is the mean service rate and <img src="4-2730005\683798a1-d990-4300-b30e-b24c3a7ee1f9.jpg" /> is the covariance between arrival and service processes.</p></sec><sec id="s3"><title>3. Postulates of the Model</title><p>In addition to our assumptions in previous section-2 of the model, we have here underlying postulates for the purpose of our current study and analysis:</p><p>Postulate 3.1: The probability that there is one arrival and no service completion during a small interval of time <img src="4-2730005\1a6ecad0-ee54-409f-8be8-cf2e7ff28c96.jpg" /> is<img src="4-2730005\5141c8fd-d425-46b0-a61c-7f9abe562209.jpg" />; when the system has arrival rate<img src="4-2730005\8d2bac09-c3bf-4e28-b240-d21ec1a1e53b.jpg" />.</p><p>Postulate 3.2: The probability that there is neither arrival and nor service completion during a small interval of time <img src="4-2730005\879c3b5b-94fd-4f0b-b735-56f27270e74e.jpg" /> is<img src="4-2730005\a7bb2bed-baa3-4158-beec-c2c0a3303956.jpg" />, when the system has arrival rate<img src="4-2730005\599c9162-d056-4ac3-8499-00bf3f3254e4.jpg" />.</p><p>Postulate 3.3: The probability that there is no arrival and one service completion during a small interval of time <img src="4-2730005\9aa26bcf-16d4-4bcb-9899-47170f86b481.jpg" /> is<img src="4-2730005\6ec8df69-c415-4926-ae87-0d8e85c1404a.jpg" />, whatever be the arrival rate<img src="4-2730005\d8cb89e6-b7a9-4aeb-ae12-d2dc8649e8e9.jpg" />.</p><p>Postulate 3.4: The probability that there is one arrival and one service completion during a small interval of time <img src="4-2730005\daf4ae19-18f6-42f5-a9b3-b851426720aa.jpg" /> is<img src="4-2730005\d8b16b07-d12e-4fb2-86f9-74e0ec4a458e.jpg" />; whatever be the arrival rate<img src="4-2730005\b06f2f88-172c-487c-90aa-54bdd1708ef8.jpg" />.</p></sec><sec id="s4"><title>4. Differential-Difference Equations</title><p>Before proceeding further, we use symbol <img src="4-2730005\d30db887-ee39-4b6d-a0f4-ec5542da5f90.jpg" /> be the probability that there are n customers in the system at time <img src="4-2730005\c332cfda-a561-422f-8431-e8680033012b.jpg" /> when system allows the arrival rate<img src="4-2730005\3ac079b3-123d-42cf-8361-24137d72b5db.jpg" />.</p><p>Now it is fairly easy to observe that <img src="4-2730005\a7446954-a139-4355-b025-e862fc661ccc.jpg" /> exists when <img src="4-2730005\861300b7-d19c-44d2-ad8b-d421280ff8bb.jpg" /> however both <img src="4-2730005\3f1d3ea7-1f5a-4d5b-9f66-c3d9b9934a23.jpg" /> and <img src="4-2730005\2d194323-137b-4fce-9907-cc441d3b6605.jpg" /> exist when<img src="4-2730005\3d8e2e1b-cb1a-4de0-8c7e-bbf652824677.jpg" />; but only <img src="4-2730005\3d50281e-7ffb-4145-83f6-d7609d67d84d.jpg" /> exists when <img src="4-2730005\c3ddfa5e-1f50-4547-8510-20e267627ef4.jpg" /></p><p>We further assume that the initial system size is 1 and R + 1 respectively when system has arrival rate<img src="4-2730005\b975bde8-f541-41f9-bda2-badbdc4f52f0.jpg" />. Let <img src="4-2730005\ec51afec-0dd1-4473-9839-e22ebdf8ae5a.jpg" /> and <img src="4-2730005\caf2b3e8-29bd-4c22-82a3-5709d92053d3.jpg" /> be the busy period density respectively when the system has arrival rate<img src="4-2730005\98a3bbbf-bc36-4545-ab3f-d4383db82d79.jpg" />.</p><p>Now in view of an absorbing barrier at empty system during its faster arrival rate <img src="4-2730005\a1169b0c-3794-4b83-b5da-c75f53c07478.jpg" /> the governing differential difference equations of the system size for the model are as following:</p><disp-formula id="scirp.26134-formula95120"><label>(4.1)</label><graphic position="anchor" xlink:href="4-2730005\f6327302-5788-48ac-82e6-4a64e3b908f5.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95121"><label>(4.2)</label><graphic position="anchor" xlink:href="4-2730005\7b49e420-54fd-49d8-a5ce-39fccbb0a8cc.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95122"><label>(4.3)</label><graphic position="anchor" xlink:href="4-2730005\b3ba1f70-7b6c-4872-96a6-f46a42ea7abe.jpg"  xlink:type="simple"/></disp-formula><p>The differential difference equation for the system size <img src="4-2730005\7b6883ed-9403-4b83-b82e-23a766a8ad4b.jpg" /> is as following:</p><disp-formula id="scirp.26134-formula95123"><label>(4.4)</label><graphic position="anchor" xlink:href="4-2730005\c1530476-9eee-42b9-a708-2c1a1200e8db.jpg"  xlink:type="simple"/></disp-formula><p>Moreover, the differential difference equations for the system size <img src="4-2730005\18ce215d-f534-41a2-b748-c3a3117f6403.jpg" /> are as following:</p><disp-formula id="scirp.26134-formula95124"><label>(4.5)</label><graphic position="anchor" xlink:href="4-2730005\18e3d7b7-caae-4709-a1ca-52b5a32b53f8.jpg"  xlink:type="simple"/></disp-formula><p>And the differential difference equation governing the state <img src="4-2730005\afede502-4e4f-4ddb-b3cc-62257678fa7b.jpg" /> is as follows</p><disp-formula id="scirp.26134-formula95125"><label>(4.6)</label><graphic position="anchor" xlink:href="4-2730005\0e865277-7c75-4c0e-bfed-7fcbc6f7ebe1.jpg"  xlink:type="simple"/></disp-formula><p>Similarly, in view of an absorbing barrier at <img src="4-2730005\ee7e3cb1-93b5-4df6-98bd-d46a816bce05.jpg" /> system size during its slower arrival rate<img src="4-2730005\76560bb9-c56d-44d1-a6dd-d1d1c3484435.jpg" />, we have the differential difference equations governing for the system size <img src="4-2730005\909da5d2-fb14-4600-8d74-f3a364ee8266.jpg" />as following:</p><disp-formula id="scirp.26134-formula95126"><label>(4.7)</label><graphic position="anchor" xlink:href="4-2730005\876bc6cc-b1cd-4435-ba2a-4d2315771d1e.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95127"><label>(4.8)</label><graphic position="anchor" xlink:href="4-2730005\d38384cd-fbfd-4c89-b1d3-eba6ce31e4fb.jpg"  xlink:type="simple"/></disp-formula><p>As in the earlier case of faster arrival rate, it is fairly easy to obtain the differential difference equations governing the states for <img src="4-2730005\2d2b8794-6b43-45b3-9182-3420f865d549.jpg" /> in slower arrival rate of the model which are given as following</p><disp-formula id="scirp.26134-formula95128"><label>(4.9)</label><graphic position="anchor" xlink:href="4-2730005\db13583a-2e33-4901-9fd8-bc3f921c4e75.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95129"><label>(4.10)</label><graphic position="anchor" xlink:href="4-2730005\bddb6aff-3963-4edd-9451-63c807785db9.jpg"  xlink:type="simple"/></disp-formula><p>Moreover, the differential difference equations governing the states of the system for<img src="4-2730005\78f8f8e9-ae41-4f41-b071-1302f775fcaf.jpg" />. in slower arrival rate are as follows</p><disp-formula id="scirp.26134-formula95130"><label>(4.11)</label><graphic position="anchor" xlink:href="4-2730005\24f1a96c-0e08-44ed-983b-529657d082bb.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Determination of Probability Generating Function in Faster Arrival Rate</title><p>We define following probability generating function for the busy period of server in faster arrival rate: <sup></sup></p><disp-formula id="scirp.26134-formula95131"><label>(5.1)</label><graphic position="anchor" xlink:href="4-2730005\a1310dad-30e0-4b24-8b4c-dbe256c17795.jpg"  xlink:type="simple"/></disp-formula><p>and we use symbol<sup> <img src="4-2730005\f29d1f44-ee5d-411f-a8a2-338236351909.jpg" /> </sup>for the Laplace transform of<img src="4-2730005\c20b2ab2-b5ea-42ab-8a0e-8342d77c037e.jpg" />in following equation:</p><disp-formula id="scirp.26134-formula95132"><label>(5.2)</label><graphic position="anchor" xlink:href="4-2730005\b24e62a0-d5fc-4626-8fa3-df7a9ebe3ea0.jpg"  xlink:type="simple"/></disp-formula><p>Multiplying by <img src="4-2730005\c39f1f69-b9f2-4132-ac58-7ad946c6cb11.jpg" />for <img src="4-2730005\9f156391-4809-46d9-b0c0-d0cd713c6634.jpg" />in respective differential difference Equations (4.1) to (4.6) and then summing over k and simplifying we obtain following partial differential equation</p><disp-formula id="scirp.26134-formula95133"><label>(5.3)</label><graphic position="anchor" xlink:href="4-2730005\2a9f4952-b525-429e-aa09-06fcf70ef649.jpg"  xlink:type="simple"/></disp-formula><p>Taking Laplace transform of both sides of partial differential difference Equation (5.3), it is fairly easy to obtain</p><disp-formula id="scirp.26134-formula95134"><label>(5.4)</label><graphic position="anchor" xlink:href="4-2730005\c38e592d-cd7e-4720-bebd-46cd3401c60d.jpg"  xlink:type="simple"/></disp-formula><p>As we know the fact that the<img src="4-2730005\f6d51a31-8853-4bba-8c15-3fe9fa403883.jpg" />converges in the region of the unit circle; <img src="4-2730005\6b85ddf3-0f61-4ef4-b670-878c02699f16.jpg" />and <img src="4-2730005\49fd1a39-aa55-4b8e-b9d7-7ae7ddbe0c19.jpg" /> whenever the denominator of RHS of equation (5.4) has zeros in the unit circle;<img src="4-2730005\74e9b76d-c498-4e8d-a930-23ca8e247669.jpg" />.</p><p>The two zeros of the denominators are as following:</p><disp-formula id="scirp.26134-formula95135"><label>(5.5)</label><graphic position="anchor" xlink:href="4-2730005\fc661452-85ce-4b94-8875-b0ddc8e91f97.jpg"  xlink:type="simple"/></disp-formula><p>From Equation (5.5), we can observe here that</p><p><img src="4-2730005\ddea8c34-c2f0-4a3b-a358-503b59fa566c.jpg" /></p><p>Moreover, we have</p><disp-formula id="scirp.26134-formula95136"><label>(5.6)</label><graphic position="anchor" xlink:href="4-2730005\8f8976c8-c187-4819-81ee-9088b0203769.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95137"><label>(5.7)</label><graphic position="anchor" xlink:href="4-2730005\6482e6cd-9571-4e43-aca0-0f26bf38219f.jpg"  xlink:type="simple"/></disp-formula><p>On making use of Rouche’s theorem in Equation (5.4), it is fairly easy to evaluate <img src="4-2730005\b1be8731-cf13-48a4-8857-7f3d8080e367.jpg" /> as following:</p><disp-formula id="scirp.26134-formula95138"><label>(5.8)</label><graphic position="anchor" xlink:href="4-2730005\0f156df2-1ba5-4e9b-8e87-526795454eb6.jpg"  xlink:type="simple"/></disp-formula><p>In view of Equation (5.8), <img src="4-2730005\5edf9bf5-1a04-483d-9aaa-5ab1d6b55a6e.jpg" />from<sup> </sup>Equation (5.5) yields as following:</p><disp-formula id="scirp.26134-formula95139"><label>(5.9)</label><graphic position="anchor" xlink:href="4-2730005\8f23725a-77c3-46e0-a200-05c16d0b336b.jpg"  xlink:type="simple"/></disp-formula><p>Equation (5.9) can be used in view of Gross and Harris [<xref ref-type="bibr" rid="scirp.26134-ref12">12</xref>] to explore the expected busy periods <img src="4-2730005\e4a8b5ff-e6f0-446d-a989-2be3bebd83ca.jpg" />in faster arrival rate as discussed by Maurya [<xref ref-type="bibr" rid="scirp.26134-ref1">1</xref>] and it is expressed as following:</p><disp-formula id="scirp.26134-formula95140"><label>(5.10)</label><graphic position="anchor" xlink:href="4-2730005\0a17f7a4-3cb1-4433-9c75-397583c52c66.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. Determination of Probability Generating Function in Slower Arrival Rate</title><p>In this section, we define following probability generating function for the busy period of slower arrival rate:</p><disp-formula id="scirp.26134-formula95141"><label>(6.1)</label><graphic position="anchor" xlink:href="4-2730005\6ed9b04b-48e0-4e3b-85d4-6b48ee75f688.jpg"  xlink:type="simple"/></disp-formula><p>and we use symbol <sup>&#160;<img src="4-2730005\e3d386bf-dfa8-498b-ab9e-7459a7db67c1.jpg" /></sup><sup> </sup>for the Laplace transform of <img src="4-2730005\0b747fc0-49b1-47bd-959e-ede1fdba15e9.jpg" /> in following equation:</p><disp-formula id="scirp.26134-formula95142"><label>(6.2)</label><graphic position="anchor" xlink:href="4-2730005\eb3c46a5-7986-4ea8-932b-24a3a2ae2389.jpg"  xlink:type="simple"/></disp-formula><p>Multiplying through differential difference Equations (4.7) to (4.11) by appropriate power of <img src="4-2730005\6f9b77ba-fd28-4434-8b97-7a35289d5a3c.jpg" />for <img src="4-2730005\a843e59e-5a73-47f8-b538-04eb59170f9e.jpg" />and then summing over k and proceeding as in earlier case of faster arrival rate<img src="4-2730005\7cd616ab-e383-405e-b341-d0a1f3e7ffb3.jpg" />, it is fairly easy to obtain <img src="4-2730005\367161a0-534c-4ff3-b237-841e1b4427a4.jpg" />as following:</p><disp-formula id="scirp.26134-formula95143"><label>(6.3)</label><graphic position="anchor" xlink:href="4-2730005\3830289f-9c82-4b55-a492-d56a89742fd7.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-2730005\c139b0a5-fe25-4472-8acc-dfa03b980c1f.jpg" />is given by following equation:</p><disp-formula id="scirp.26134-formula95144"><label>(6.4)</label><graphic position="anchor" xlink:href="4-2730005\eaf2ee28-49ed-4346-898e-9874194ea38f.jpg"  xlink:type="simple"/></disp-formula><p>It is remarkable that <img src="4-2730005\4e680ad0-7a8c-461f-95fb-928e35b63aed.jpg" />in Equation (6.4) possesses following three properties:</p><disp-formula id="scirp.26134-formula95145"><label>(6.5)</label><graphic position="anchor" xlink:href="4-2730005\0c996bc9-ab15-4815-bd3e-19f9cafa0e85.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95146"><label>(6.6)</label><graphic position="anchor" xlink:href="4-2730005\1914f998-9c86-473e-9e8b-dfd06484c7e4.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26134-formula95147"><label>(6.7)</label><graphic position="anchor" xlink:href="4-2730005\04c893e3-eed3-4e15-aae2-27a6e0d9b2f1.jpg"  xlink:type="simple"/></disp-formula><p>Applying Rouche’s theorem in Equation (6.3), we may have <img src="4-2730005\d9f46c8f-b82e-4c31-b897-83447e6ef398.jpg" />as following:</p><disp-formula id="scirp.26134-formula95148"><label>(6.8)</label><graphic position="anchor" xlink:href="4-2730005\7fd10f6a-39b2-4a70-99d6-640e373ba415.jpg"  xlink:type="simple"/></disp-formula><p>We remark here that using equation (6.8) in the light of Gross and Harris [<xref ref-type="bibr" rid="scirp.26134-ref12">12</xref>], Maurya [<xref ref-type="bibr" rid="scirp.26134-ref1">1</xref>] succeeded to evaluate<img src="4-2730005\2b0c973c-592f-4b5c-8e60-15c949c35ab4.jpg" />; the expected busy period in slower arrival rate which is expressed as following:</p><disp-formula id="scirp.26134-formula95149"><label>(6.9)</label><graphic position="anchor" xlink:href="4-2730005\38f4c793-7543-482f-901b-1cf999357731.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s7"><title>7. Conclusions</title><p>The probability generating function is the most important mathematical technique to examine the transient and steady state behavior of queueing models, particularly to explore many significant performance measures in study of wide range of queueing models which has been been evidenced by recent work of Maurya [1,6,7] and references therein and therefore it plays considerably a vital role in analyzing queueing problems. In the present paper, we have successfully investigated the probability generating functions for two different cases of slower and faster arrival rates of an interdependent <img src="4-2730005\ca96f402-db95-4f0c-b5d6-2fb38678a43f.jpg" /> queueing model with controllable arrival rates taking into account that the two parameters of arrival and service rates follow the bivariate Poisson process. In order to emphasize the application aspect of the investigated result in the present paper, it is much relevant to remark here that by using the probability generating function approach, recently Maurya [<xref ref-type="bibr" rid="scirp.26134-ref1">1</xref>] considered the same queueing model and explored the expected busy periods of the server in both cases of faster and slower arrival rates. Moreover, we remark here that cost per unit time in both cases of faster and slower arrival rates of the queueing model taken into present consideration can be determined. In addition to this, it is highly expected that the research of the present investigation can be further extended by incorporating the concept of some other versions of control policies, server breakdown and multi-phase services.</p></sec><sec id="s8"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.26134-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">V. N. Maurya, “Determination of Expected Busy Periods in Faster and Slower Arrival Rates of an Interdependent  Queueing Model with Controllable Arrival Rates,” International Journal of Engineering Research &amp; Technology, Vol. 1, No. 5, 2012, pp. 1-5.</mixed-citation></ref><ref id="scirp.26134-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">I. J. B. F. Adan and J. 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