<?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">CWEEE</journal-id><journal-title-group><journal-title>Computational Water, Energy, and Environmental Engineering</journal-title></journal-title-group><issn pub-type="epub">2168-1562</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cweee.2016.52005</article-id><article-id pub-id-type="publisher-id">CWEEE-65608</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject><subject> Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Poisson Process and Its Application to the Storm Water Overflows
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>alick</surname><given-names>Baldeh</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chris</surname><given-names>Samba</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kenneth</surname><given-names>Tuffour</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Assane</surname><given-names>Boya</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Gaston Berger University, Saint-Louis, Senegal</addr-line></aff><aff id="aff1"><addr-line>Facility Solution Technology, Inc., Bakau, The Gambia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>kennethtuffour@outlook.com(KT)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>03</month><year>2016</year></pub-date><volume>05</volume><issue>02</issue><fpage>47</fpage><lpage>53</lpage><history><date date-type="received"><day>21</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>16</month>	<year>April</year>	</date><date date-type="accepted"><day>19</day>	<month>April</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>
 
 
  The homogenous Poisson process is often used to describe the event arrivals. Such Poisson process has been applied in various areas. This study focuses on the arrival pattern of storm water overflows. A set of overflow data was obtained from the storm water pipeline of a municipality. The aim is to verify the overflow arrival pattern and check whether the Poisson process can be applied. The adopted method is the analysis over the inter-arrival times. The exponential distribution test is conducted on the annual data set as well as the entire data set. The results show that all data sets follow the exponential distribution. With the verification of Poisson process, specific examples are also given to show how the Poisson process properties can be used in the management of storm water pipeline management. For other data that are featured with various heterogeneities, the homogenous Poisson process might not be able to be verified and used. Under such circumstances, non-homogenous survival model can be used to simulate the arrival process.
 
</p></abstract><kwd-group><kwd>Storm Water Overflow</kwd><kwd> Poisson Process</kwd><kwd> Exponential Distribution</kwd><kwd> Weibull Distribution</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The storm drain is designed to divert excess rain and ground water from impervious surfaces. Those impervious surfaces include paved streets, car parks, parking lots, footpaths, and roofs. There are two types of system that diverts storm water: combined sewer system (CSS) and separate storm system. The former has been the system for many municipalities. The CSS was developed to convey both sanitary sewage and storm water in one piping system. When it rains, storm water is collected into the sewer system and is sent to the treatment facility center. One disadvantage of the CSS is that there is an increased volume of sewage to the treatment plant. To address this issue, some municipalities have two independent piping systems, one for sanitary system, and the other is for storm water system. The separate storm water is designed to drain the storm water into rivers or streams.</p><p>For both combined and separate piping system, overflows are the common issue that needs to be addressed. Overflows cause damages to surrounding properties and pollute the environment. Usually, the pipe system is designed according to the capacity requirement. In terms of separate storm water system, the piping is designed to convey storm from a specific rainfall intensity, such as a 10 year rainfall. When rains are extremely heavy, overflows will probably occur. In addition, issues such as sediment accumulation, pipe condition deterioration, would cause overflows as well. The arrivals of such events are usually regarded random, which is featured with a constant rate. The failure rate is a great indicator of the systems performance. It is very meaningful to explore the true arrival pattern of the overflows.</p><p>In the facility management, pipeline system has been studied in various focuses by using different methods. One popular research topic is the pipe condition deterioration. Modeling has been applied extensively in this research effort. For example, Wirahadikusumah et al. discussed multiple challenging issues in predicting the condition using the Markov chains model [<xref ref-type="bibr" rid="scirp.65608-ref1">1</xref>] . To address certain such issues, Jin and Mukherjee further proposed methods to estimate the condition transition probabilities [<xref ref-type="bibr" rid="scirp.65608-ref2">2</xref>] . They also investigated uncertainty of the Markov chains model with the assistance of simulation in Matlab [<xref ref-type="bibr" rid="scirp.65608-ref3">3</xref>] . Another research topic is the life cycle analysis of the pipeline system. For example, Piratla et al. estimated the life cycle CO<sub>2</sub> emissions of a potable water pipeline project [<xref ref-type="bibr" rid="scirp.65608-ref4">4</xref>] . Emissions from multiple phases in the entire life cycle were quantified. Jin explored both the life cycle cost and life cycle assessment of the sewer pipeline system [<xref ref-type="bibr" rid="scirp.65608-ref5">5</xref>] . Methods proposed can be applied in the life cycle analysis of other pipeline system as well. The third research topic could be system’s reliability analysis by focusing on the failure data. For example, Jin and Mukherjee analyzed blockage failures in sewer systems to support maintenance decision making [<xref ref-type="bibr" rid="scirp.65608-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.65608-ref7">7</xref>] . Pelletier et al. applied the survival analysis on three case studies to evaluate the reliability of the water system [<xref ref-type="bibr" rid="scirp.65608-ref8">8</xref>] . The fourth research topic is the hydraulic evaluation of the pipeline system. For example, Li et al. simulated the mixed flow in storm water [<xref ref-type="bibr" rid="scirp.65608-ref9">9</xref>] . Basically, the hydraulic fundamentals, such as Bernoulli’s equation, are used in evaluate the system’s performance [<xref ref-type="bibr" rid="scirp.65608-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.65608-ref11">11</xref>] . Other relevant studies can be found in [<xref ref-type="bibr" rid="scirp.65608-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.65608-ref15">15</xref>] . All such research efforts are for the purpose of managing the facility systems efficiently [<xref ref-type="bibr" rid="scirp.65608-ref16">16</xref>] .</p><p>This research is similar to Jin and Mukherjee’s work [<xref ref-type="bibr" rid="scirp.65608-ref6">6</xref>] . Jin and Mukherjee proposed methods to model the sewer blockage failures in an effort to support the system’s management. By using a set of blockage failure data from a city, they used the stochastic approach to characterize the failure arrivals. Methods to verify the process were presented with preliminary data analysis and hypothesis test. The results show that for the annual data set, the arrivals can be best described with a homogeneous Poisson process, while for the entire data set, the non- homogenous factors start to have significant impacts on the fitting. They further conducted the reliability analysis over the data set. Based on the analysis, they proposed a schematic survival curve from the life cycle perspective. The developed methods were also successfully applied on the failure data set of a water pipeline sys- tem.</p><p>This paper focuses on the storm water overflows instead. The aim of this paper is to investigate the underlying arrival pattern of storm water overflows to assist facility management. The data set is obtained from an entire separate storm water system. Very often, those failures are regarded as random arrivals, which are featured with a Poisson process. Such Poisson process has been applied in many areas [<xref ref-type="bibr" rid="scirp.65608-ref17">17</xref>] - [<xref ref-type="bibr" rid="scirp.65608-ref20">20</xref>] . This study explores such arrival pattern of storm water overflows. The results would assist stakeholders in the decision making process.</p></sec><sec id="s2"><title>2. Methodology</title><p>In order to verify if Poisson process can be used to characterize the arrival of overflows. The inter-arrival times of the overflows are used. For a Poisson process, the inter-arrival times between two successive events are exponentially distributed.</p><p>In theory, a discrete random variable X is said to be a Poisson random variable with parameter λ, the probability mass function of X is given by</p><disp-formula id="scirp.65608-formula44"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-2570107x6.png"  xlink:type="simple"/></disp-formula><p>The mean of the Poisson distribution is λ, the variance of the distribution is also λ.</p><p>In a Poisson process with a constant arrival rate of λ, the inter-arrival times between events are exponentially distributed. The proof of this statement can be found in Ross [<xref ref-type="bibr" rid="scirp.65608-ref21">21</xref>] . Therefore, in order to verify whether the arrival of overflows follows a Poisson process, one direct method is to check the distribution of the inter-arrival times.</p><p>Among all the renewal processes, the Poisson process is very unique due to the memoryless property of the exponential distribution. For an exponential, the probability density function is</p><disp-formula id="scirp.65608-formula45"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-2570107x7.png"  xlink:type="simple"/></disp-formula><p>In terms of memory-less property, a random variable X has the memory-less property if for every x ≥ 0 and t ≥ 0, we have</p><disp-formula id="scirp.65608-formula46"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-2570107x8.png"  xlink:type="simple"/></disp-formula><p>Equation (3) can be proved using the definition of conditional probability. By combining Equation (2), we have</p><disp-formula id="scirp.65608-formula47"><graphic  xlink:href="http://html.scirp.org/file/3-2570107x9.png"  xlink:type="simple"/></disp-formula><p>In a time series analysis, X can be interpreted as the waiting time until a given arrival. Equation (3) states that, given that the no arrival occurred by time t, the distribution of the remaining waiting time stays the same. That is, the remaining waiting time has no “memory” of previous waiting. That’s the reason that the inter-arrival times can be used to verify the Poisson process.</p><p>When dealing with non-homogenous Poisson process, the arrival rate is not constant but a function of time. A typical non-homogenous Poisson process (NHPP) is the power law process, which is sometimes called a Weibull process [<xref ref-type="bibr" rid="scirp.65608-ref21">21</xref>] . The Weibull distribution is often used to conduct the reliability analysis. As a distribution, it can also be used to fit data set. In this study, if inter-arrival times are not found of exponential distribution, considering the relationship between an exponential and a Weibull, the Weibull distribution can be used, the standard Weibull distribution has the density function</p><disp-formula id="scirp.65608-formula48"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-2570107x10.png"  xlink:type="simple"/></disp-formula><p>and distribution function</p><disp-formula id="scirp.65608-formula49"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-2570107x11.png"  xlink:type="simple"/></disp-formula><p>where α is the scale parameter, k is the shape parameter. When k = 1, the Weibull distribution is reduced to an exponential distribution [<xref ref-type="bibr" rid="scirp.65608-ref21">21</xref>] .</p><p>In summary, in order to verify the Poisson process, the inter-arrival times are used in the analysis. The Poisson process can be verified if the inter-arrival times follow an exponential distribution. In some cases, when Poisson process cannot be verified, some other more powerful distribution can be used to check the distribution of such inter-arrival data sets. The data used in the study ranges from 2012 to 2014. The inter-arrival times of the annual data sets and the entire data set are analyzed. The Minitab 2016 tool is used for the analysis. The hypothesis test is used to verify the distribution fitting. The null and alternative hypothesis are:</p><p>H<sub>0</sub>: The data set follows a specific distribution.</p><p>H<sub>1</sub>: The data set does not follow the specific distribution.</p><p>Significant level: 0.05.</p></sec><sec id="s3"><title>3. Results and Applications</title><p>Figures 1-3 show the exponential distribution test of the annual data set. It can be that the P values for each data</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Exponential distribution fitting for 2012 data</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2570107x12.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Exponential distribution fitting for 2013 data</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2570107x13.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Exponential distribution fitting for 2014 data</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2570107x14.png"/></fig><p>set are all greater than 0.05. Therefore, the hypothesis that the data set follows an exponential distribution can be accepted. It also means that the arrivals of such overflows follow a Poisson process. <xref ref-type="fig" rid="fig4">Figure 4</xref> displays the exponential distribution fitting for the entire data set. The fitting also passes the rigid hypothesis test with a P value of 0.323. Therefore, the entire data set also follows an exponential distribution. <xref ref-type="table" rid="table1">Table 1</xref> lists the parameters for test results.</p><p>Although the exponential distribution is good fit. The Weibull distribution is also used to fit the same data set. As expected, as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, the Weibull distribution fits the data very well with P value greater than 0.25. Considering that the exponential distribution is a one parameter distribution and Weibull distribution is a more powerful 2-parameter distribution, it is obviously that when an exponential distribution fits the data, the Weibull also fits. Since a simple model does the job well, it is reasonable to accept the fact that the data follows the exponential distribution. For some other data set with more non-homogenous noises, the Weibull distribution could be a good option to test against.</p><p>From the entire data set fitting, we can find that the mean value is 16.16 days. The P value is very decent and it is safe to conclude that the inter-arrival times follow an exponential distribution. Therefore, the failure rate is 0.062 per day. In application, those information can be used to address multiple issues. The following example problems can be solved.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Exponential distribution fitting for the entire data</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2570107x15.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Weibull distribution fitting for the entire data</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-2570107x16.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Parameters of the exponential fitting for each data set</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" >Mean</th><th align="center" valign="middle" >P value</th></tr></thead><tr><td align="center" valign="middle" >2012 data</td><td align="center" valign="middle" >14.20</td><td align="center" valign="middle" >0.896</td></tr><tr><td align="center" valign="middle" >2013 data</td><td align="center" valign="middle" >16.36</td><td align="center" valign="middle" >0.603</td></tr><tr><td align="center" valign="middle" >2014 data</td><td align="center" valign="middle" >16.05</td><td align="center" valign="middle" >0.487</td></tr><tr><td align="center" valign="middle" >Entire data</td><td align="center" valign="middle" >16.16</td><td align="center" valign="middle" >0.323</td></tr></tbody></table></table-wrap><p>Case 1: what is the chance that there are exact 10 failures next year? To address this question, we know that the mean arrival number of overflow per year is 0.062 &#215; 365 = 23, by using Equation (1), we have</p><p>P (X = 10) = exp (−23) &#215; 23^10/10! = 0.0012.</p><p>Case 2: what are the chances that there are at least 10 failures next year?</p><p>The question is actually for the probability when there are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-2570107x17.png" xlink:type="simple"/></inline-formula> failures in a given year. Therefore, it is the sum of all those individual probabilities.</p><p>P (X = 0) = exp (−23) &#215; 23^0/0! = 1.026E−10</p><p>P (X = 1) = exp (−23) &#215; 23^1/1! = 2.360E−9</p><p>P (X = 2) = exp (−23) &#215; 23^2/2! = 2.714E−8</p><p>P (X = 3) = exp (−23) &#215; 23^3/3! = 2.081E−7</p><p>P (X = 4) = exp (−23) &#215; 23^4/4! = 1.200E−6</p><p>P (X = 5) = exp (−23) &#215; 23^5/5! = 5.504E−6</p><p>P (X = 6) = exp (−23) &#215; 23^6/6! = 2.110E−5</p><p>P (X = 7) = exp (−23) &#215; 23^7/7! = 6.933E−5</p><p>P (X = 8) = exp (−23) &#215; 23^8/8! = 1.993E−4</p><p>P (X = 9) = exp (−23) &#215; 23^9/9! = 5.093E−4</p><p>P (X = 10) = exp (−23) &#215; 23^10/10! = 1.172E−3</p><p>The probability for at least 10 failures in the next year is 0.0020.</p><p>Case 3: what is the probability that no overflow was found in a 30 days?</p><p>The probability of no overflow can be found using</p><p>Pr {k = 0} = exp (−30 &#215; 0.062) = 0.156.</p><p>Case 4: what is the expected time for the 20<sup>th</sup> overflow?</p><p>Since it is a Poisson process, the arrival rate is constant. Therefore the expected time for the 20<sup>th</sup> overflow can be found using 20/0.062 = 323 days.</p></sec><sec id="s4"><title>4. Conclusion</title><p>The storm water overflow is an indicator of the pipeline management. The arrivals of such overflows can be regarded as a process. The Poisson process is often used to describe such time series events. This paper explores whether the general homogenous Poisson process can be used to model the arrivals of storm water overflows. In theory, the inter-arrival times of a Poisson process follow an exponential distribution. To verify this, the annual data set and the entire data set are used to fit against an exponential distribution. The results show that for the annual data sets, they fit the exponential distribution very well. Even for the entire data set, the fitting is also decent. Therefore, it can be concluded that for the available storm water overflow data set, the Poisson process can be used to describe the process. Specific examples are shown to demonstrate the applications. It should also be noted that the homogenous Poisson process may not be used for other data sets that are impacted by various non-homogenous factors; the non-homogenous reliability model may be applied on those data sets. Related studies will be conducted in our future research.</p></sec><sec id="s5"><title>Cite this paper</title><p>Malick Baldeh,Chris Samba,Kenneth Tuffour,Assane Boya, (2016) Poisson Process and Its Application to the Storm Water Overflows. Computational Water, Energy, and Environmental Engineering,05,47-53. doi: 10.4236/cweee.2016.52005</p></sec></body><back><ref-list><title>References</title><ref id="scirp.65608-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Wirahadikusumah, R., Abraham, D. and Iseley, T. (2001) Challenging Issues in Modeling Deterioration of Combined Sewers. 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