<?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">AJOR</journal-id><journal-title-group><journal-title>American Journal of Operations Research</journal-title></journal-title-group><issn pub-type="epub">2160-8830</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajor.2016.62021</article-id><article-id pub-id-type="publisher-id">AJOR-64501</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Performance of Stochastically Intermittent Sensors in Detecting a Target Traveling between Two Areas
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ongyun</surname><given-names>Wang</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>Hong</surname><given-names>Zhou</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Applied Mathematics and Statistics, Baskin School of Engineering, University of California, Santa Cruz, CA, USA</addr-line></aff><aff id="aff2"><addr-line>Department of Applied Mathematics, Naval Postgraduate School, Monterey, CA, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hongwang@soe.ucsc.edu(OW)</email>;<email>hzhou@nps.edu(HZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>26</day><month>02</month><year>2016</year></pub-date><volume>06</volume><issue>02</issue><fpage>199</fpage><lpage>212</lpage><history><date date-type="received"><day>6</day>	<month>November</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>11</month>	<year>March</year>	</date><date date-type="accepted"><day>15</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>
 
 
  We study the problem of detecting a target that moves between a hiding area and an operating area over multiple fixed routes. The research is carried out with one or more cookie-cutter sensors with stochastic intermission, which turn on and off stochastically governed by an on-rate and an off-rate. A cookie-cutter sensor, when it is on, can detect the target instantly once the target comes within the detection radius of the sensor. In the hiding area, the target is shielded from being detected. The residence times of the target, respectively, in the hiding area and in the operating area, are exponentially distributed and are governed by rates of transitions between the two areas. On each travel between the two areas and in each travel direction, the target selects a route randomly according to a probability distribution. Previously, we analyzed the simple case where the sensors have no intermission (i.e., they stay on all the time). In the current study, the sensors are stochastically intermittent and are synchronized (i.e., they turn on or off simultaneously). This happens when all sensors are affected by the same environmental factors. We derive asymptotic expansions for the mean time to detection when the on-rate and off-rate of the sensors are large in comparison with the rates of the target traveling between the two areas. Based on the mean time to detection, we evaluate the performance of placing the sensor(s) to monitor various travel route(s) or to scan the operating area.
 
</p></abstract><kwd-group><kwd>Stochastically Intermittent Sensors</kwd><kwd> Moving Target with Constrained Pathways</kwd><kwd> Mean Time to Detection</kwd><kwd> Optimal Search Design</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Search and detection theory has a history of principal importance in operations research. It has fundamental military and civilian applications such as anti-submarine warfare, counter-mine warfare, and search and rescue operations [<xref ref-type="bibr" rid="scirp.64501-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.64501-ref4">4</xref>] .</p><p>Nowadays when combating piracy at sea, detecting and intercepting threat objects (boats) such as terrorists and drug or weapon smugglers, or securing coastlines and trade routes, it is important to understand the behavior of a target and plan a search and detection strategy accordingly. In a recent work [<xref ref-type="bibr" rid="scirp.64501-ref5">5</xref>] we considered the problem of searching for a target that travels between a hiding area and an operating area via multiple routes. By assuming certain behaviors of the moving target, we obtained analytic expressions for the mean time to detection and thereby were able to determine the optimal placement of m cookie-cutter sensors (i.e. how many sensors should we place on which routes and the rest is placed to search the operating area). Interestingly, we found that the optimal placement, sometimes, is not the one suggested by intuition.</p><p>In this paper we would like to extend our earlier study to include stochastically intermittent sensors in detecting a target moving between a hiding area and an operating area.</p></sec><sec id="s2"><title>2. Mathematical Formulation for the Case of Sensors without Intermission</title><p>We consider the search problem in which a target moves between a hiding area and an operating area via constrained pathways, as depicted in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The target can stay in the hiding area where the target is shielded from being detected by the sensors. There are N given routes connecting the hiding area and the operating area. The target can travel along one of these N given routes from the hiding area to the operating area. The target can spend time in the operating area to carry out certain activities/tasks. Afterwards, the target can return to the hiding area via possibly a different route. In the hiding area, the target is not detectable. Outside the hiding area, the target is detectable along the routes and in the operating area if it comes into the detection range of a sensor.</p><p>In the search problem, variable number of synchronized intermittent cookie-cutter sensors are used to detect the target. We will first introduce the mathematical model for the simple case of non-intermittent sensors (i.e., they stay on all the time) and then extend the model to accommodate the stochastic intermission of the sensors.</p><p>We start by specifying the target behavior. The target moves stochastically between the hiding area and the operating area according to the following rules.</p><p>・ The dwell time of the target in the hiding area is exponentially distributed with rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x7.png" xlink:type="simple"/></inline-formula>, the forward rate of the target going from the hiding area to the operating area.</p><p>・ On its travel from the hiding area to the operating area, the target takes route k with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x8.png" xlink:type="simple"/></inline-formula>, which satisfies the constraint <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x9.png" xlink:type="simple"/></inline-formula> where N is the total number of given routes.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A target traveling between two areas. The target may stay in the hiding area where it is not detectable; it may travel from the hiding area to the operating area along one of the N given routes; it may spend time in the operating area before returning to the hiding area via possibly a different route</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x10.png"/></fig><p>・ The dwell time of the target in the operating area is exponentially distributed with rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x11.png" xlink:type="simple"/></inline-formula>, the backward rate of the target going from the operating area back to the hiding area.</p><p>・ On its travel from the operating area back to the hiding area, the target chooses route k with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x12.png" xlink:type="simple"/></inline-formula>, which satisfies the condition<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x13.png" xlink:type="simple"/></inline-formula>.</p><p>・ The travel time between the operating area and the hiding area is negligible in comparison with the dwell times in the hiding area and the operating area. Mathematically, we treat the travel time along a route as zero.</p><p>The target’s travel between the two areas is mathematically described by a Markov process of two states, with</p><p>forward rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x14.png" xlink:type="simple"/></inline-formula> and backward rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x15.png" xlink:type="simple"/></inline-formula>, as illustrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>Next, we describe the interaction between the target and sensors. A non-intermittent cookie-cutter sensor is an ideal sensor which detects the target instantly once the target comes within distance R to the center of the sensor where the radius R is called the detection radius of the sensor. When the target is outside the detection radius, it is not detected. In this study, we assume that the detection radius of sensors is large enough to cover the full width of any one of the given routes. Consequently, if a non-intermittent sensor is assigned to monitor a route and the target happens to move along that route, the target will definitely be detected by the sensor. Of course, the situation will be different for an intermittent sensor that turns on and off stochastically.</p><p>When a sensor is used to search the operating area, when the sensor is on, and when the target is in the operating area, the interaction between the target and the sensor is modeled using a detection rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x16.png" xlink:type="simple"/></inline-formula> (pro- bability of detection per time).</p><disp-formula id="scirp.64501-formula747"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x17.png"  xlink:type="simple"/></disp-formula><p>This detection rate is affected by the size of the operating area, and by the detection radius and the speed of the sensor.</p><p>When one or more non-intermittent sensors are deployed to monitor one or more routes or to search the operating area, the transitions and detection of the target are governed by a 3-state Markov process of the same parameter form as the one shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The values of p, q, and d depend on how many sensors are used and which route(s) and area are monitored/searched. Values of p, q, and d are given below for several cases.</p><p>・ When only one sensor is deployed and it is placed to monitor route k, this gives</p><disp-formula id="scirp.64501-formula748"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x18.png"  xlink:type="simple"/></disp-formula><p>・ When only one sensor is deployed and it is used to search the operating area, this corresponds to</p><disp-formula id="scirp.64501-formula749"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x19.png"  xlink:type="simple"/></disp-formula><p>・ When two sensors are placed to monitor, respectively, routes k and j (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x20.png" xlink:type="simple"/></inline-formula>), it follows that</p><disp-formula id="scirp.64501-formula750"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x21.png"  xlink:type="simple"/></disp-formula><p>・ When two sensors are both used to search the operating area, we find</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Markov transitions of the target between the hiding area and the operating area in the absence of any sensor.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x22.png"/></fig></fig-group><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Markov transitions of the target in the presence of non-intermittent sensor(s). Note that the parameter form of the Markov process is the same for all cases while values of parameter p, q, and d vary from case to case</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x23.png"/></fig><disp-formula id="scirp.64501-formula751"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x24.png"  xlink:type="simple"/></disp-formula><p>・ When one sensor is placed to monitor route k and a second sensor is used to search the operating area, this gives</p><disp-formula id="scirp.64501-formula752"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x25.png"  xlink:type="simple"/></disp-formula><p>To facilitate our analysis, we divide all transition rates by the sum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x26.png" xlink:type="simple"/></inline-formula> to non-dimensionalize the Markov process depicted in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Additionally, we introduce two dimensionless parameters:</p><disp-formula id="scirp.64501-formula753"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x27.png"  xlink:type="simple"/></disp-formula><p>The parameter form of the normalized Markov process is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>In the absence of sensors, at equilibrium, the probabilities of the target being in the hiding area or the operating area are, respectively, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x28.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x29.png" xlink:type="simple"/></inline-formula>. This fact will be used later in the calculation of mean time to detection.</p></sec><sec id="s3"><title>3. Mean Time to Detection in the Case of Sensors without Intermission</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> describes the general model for the case of non-intermittent sensors. It can accommodate arbitrary number of sensors. For mathematical convenience, we label the hiding area as state 1 and the operating area as state 2. We solve for the mean time to detection.</p><p>Let T denote the time to detection (random variable), and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x30.png" xlink:type="simple"/></inline-formula> denote the state of the target at time t. Time 0 is defined as the time when the sensors are deployed. We examine the conditional mean time to detection given that the target is in state j at time 0.</p><disp-formula id="scirp.64501-formula754"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x31.png"  xlink:type="simple"/></disp-formula><p>We derive two equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x32.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x33.png" xlink:type="simple"/></inline-formula> based on the Markov process in <xref ref-type="fig" rid="fig4">Figure 4</xref>. Starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x34.png" xlink:type="simple"/></inline-formula>, the probability distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x35.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.64501-formula755"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x36.png"  xlink:type="simple"/></disp-formula><p>Using the law of total expectation, we have</p><disp-formula id="scirp.64501-formula756"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x37.png"  xlink:type="simple"/></disp-formula><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The normalized Markov process governing the transitions of the target.</title></caption><fig id ="fig4_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x38.png"/></fig></fig-group><p>which, when divided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x39.png" xlink:type="simple"/></inline-formula> and in the limit of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x40.png" xlink:type="simple"/></inline-formula> going to zero, yields</p><disp-formula id="scirp.64501-formula757"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x41.png"  xlink:type="simple"/></disp-formula><p>This is an equation for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x42.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x43.png" xlink:type="simple"/></inline-formula>. Similarly, another equation can be derived starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x44.png" xlink:type="simple"/></inline-formula>. The two equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x45.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x46.png" xlink:type="simple"/></inline-formula> are</p><disp-formula id="scirp.64501-formula758"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x47.png"  xlink:type="simple"/></disp-formula><p>Solving linear system (5), we obtain</p><disp-formula id="scirp.64501-formula759"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x48.png"  xlink:type="simple"/></disp-formula><p>Before the deployment of sensors, the equilibrium distribution of the target is</p><disp-formula id="scirp.64501-formula760"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x49.png"  xlink:type="simple"/></disp-formula><p>Thus, the overall mean time to detection has the expression</p><disp-formula id="scirp.64501-formula761"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x50.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Mathematical Formulation for the Case of Synchronized Stochastically Intermittent Sensors</title><p>We extend above discussions to consider synchronized intermittent sensors that stochastically turn on or off simultaneously. We model the stochastic evolution of sensors as a 2-state Markov process with an on-rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x51.png" xlink:type="simple"/></inline-formula> and an off-rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x52.png" xlink:type="simple"/></inline-formula>, as illustrated in <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>As in the previous section, we divide all rates by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x53.png" xlink:type="simple"/></inline-formula> to normalize the problem. After the non- dimensionalization scaling, we write the on-rate and the off-rate as</p><disp-formula id="scirp.64501-formula762"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x54.png"  xlink:type="simple"/></disp-formula><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The 2-state Markov process governing the intermittent sensors.</title></caption><fig id ="fig5_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x55.png"/></fig></fig-group><disp-formula id="scirp.64501-formula763"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x56.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.64501-formula764"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x57.png"  xlink:type="simple"/></disp-formula><p>Note that the parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x58.png" xlink:type="simple"/></inline-formula> defined above corresponds to the equilibrium probability of sensors being on, which is also the fraction of time that sensors are on. The quantity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x59.png" xlink:type="simple"/></inline-formula> is the equilibrium probability of sensors being off. The choice of notation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x60.png" xlink:type="simple"/></inline-formula> indicates that we will focus on the parameter regime of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x61.png" xlink:type="simple"/></inline-formula>.</p><p>That is, we will focus on the case of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x62.png" xlink:type="simple"/></inline-formula>. Note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x63.png" xlink:type="simple"/></inline-formula> is the rate of sensors relaxing</p><p>to equilibrium between the on- and off-states; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x64.png" xlink:type="simple"/></inline-formula>is the rate of the target relaxing to equilibrium between the hiding area and the operating area. Parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x65.png" xlink:type="simple"/></inline-formula> in (9) measures the ratio of these two relaxation rates.</p><p>We now combine the stochastic travel of the target and the stochastic intermission of the sensors into a 5-state Markov process for the target-sensors system as illustrated in <xref ref-type="fig" rid="fig6">Figure 6</xref>. The normalized version of this 5-state Markov process where all transition rates are divided by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x66.png" xlink:type="simple"/></inline-formula>, is shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. In the model, the sensors’ intermission and the target’s travel between the two areas are independent of each other. The target- sensors system can reside in any of 4 states before the detection. For mathematical convenience, we number the 4 states as follows: (<xref ref-type="fig" rid="fig7">Figure 7</xref>).</p><p>・ State 1: the target is in the hiding area and the sensors are on.</p><p>・ State 2: the target is in the operating area and the sensors are on.</p><p>・ State 3: the target is in the hiding area and the sensors are off.</p><p>・ State 4: the target is in the operating area and the sensors are off.</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> gives the general model for the target-sensors system with synchronized stochastically intermittent sensors. It can accommodate arbitrary number of sensors. We study the mean time to detection in this 5-state Markov process.</p><p>Again, let T represent the time to detection (random variable), and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x67.png" xlink:type="simple"/></inline-formula> denote the state of the target at time t. We consider the conditional mean time to detection</p><disp-formula id="scirp.64501-formula765"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x68.png"  xlink:type="simple"/></disp-formula><p>We derive four equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x69.png" xlink:type="simple"/></inline-formula> based on the 5-state Markov process in <xref ref-type="fig" rid="fig7">Figure 7</xref>. Starting with</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x70.png" xlink:type="simple"/></inline-formula>, the probability distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x71.png" xlink:type="simple"/></inline-formula> is</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The 5-state Markov process governing the target- sensors system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x72.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> The normalized 5-state Markov process governing the target-sensors system. In the non-dimensionalization scaling, all transition rates are divided by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x74.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x73.png"/></fig><disp-formula id="scirp.64501-formula766"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x75.png"  xlink:type="simple"/></disp-formula><p>The law of total expectation gives us</p><disp-formula id="scirp.64501-formula767"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x76.png"  xlink:type="simple"/></disp-formula><p>Dividing both sides by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x77.png" xlink:type="simple"/></inline-formula> and taking the limit as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x78.png" xlink:type="simple"/></inline-formula> going to zero, we arrive at</p><disp-formula id="scirp.64501-formula768"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x79.png"  xlink:type="simple"/></disp-formula><p>This is an equation for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x80.png" xlink:type="simple"/></inline-formula>. Three other equations are derived using the same approach, starting with, respectively, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x81.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x82.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x83.png" xlink:type="simple"/></inline-formula>. Putting together, these four equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x84.png" xlink:type="simple"/></inline-formula> are</p><disp-formula id="scirp.64501-formula769"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x85.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula770"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x86.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula771"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x87.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula772"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x88.png"  xlink:type="simple"/></disp-formula><p>Analytical solutions to the above linear system is hard to obtain. Instead, in the next section, we use this linear system to calculate asymptotic expansions for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x89.png" xlink:type="simple"/></inline-formula> and for the overall mean time to detection when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x90.png" xlink:type="simple"/></inline-formula> is small.</p></sec><sec id="s5"><title>5. Asymptotic Solutions for the Mean Time to Detection in the Case of Synchronized Intermittent Sensors</title><p>We derive asymptotic solutions for the mean time to detection for small<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x91.png" xlink:type="simple"/></inline-formula>. We start by writing the conditional mean time to detection in the asymptotic form of</p><disp-formula id="scirp.64501-formula773"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x92.png"  xlink:type="simple"/></disp-formula><p>Substituting this asymptotic form into Equations (12)-(15) and examining terms of the order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x93.png" xlink:type="simple"/></inline-formula>, which</p><p>are of the largest magnitude, we obtain</p><disp-formula id="scirp.64501-formula774"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x94.png"  xlink:type="simple"/></disp-formula><p>From Equations (12)-(15), we will derive two equations that do not contain any coefficient of the order</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x95.png" xlink:type="simple"/></inline-formula>. These two equations will then be used to calculate the leading coefficients in the asymptotic form: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x96.png" xlink:type="simple"/></inline-formula></p><p>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x97.png" xlink:type="simple"/></inline-formula>. We rewrite Equations (12)-(15) to separate terms with coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x98.png" xlink:type="simple"/></inline-formula> from other terms.</p><disp-formula id="scirp.64501-formula775"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x99.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula776"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x100.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula777"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x101.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula778"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x102.png"  xlink:type="simple"/></disp-formula><p>The two equations are constructed by</p><disp-formula id="scirp.64501-formula779"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x103.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula780"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x104.png"  xlink:type="simple"/></disp-formula><p>The resulting two equations are</p><disp-formula id="scirp.64501-formula781"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula782"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x106.png"  xlink:type="simple"/></disp-formula><p>Substituting asymptotic form (16) into the two equations above, keeping only terms of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x107.png" xlink:type="simple"/></inline-formula>, and using result (17), we arrive at</p><disp-formula id="scirp.64501-formula783"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x108.png"  xlink:type="simple"/></disp-formula><p>System (24) is of the same parameter form as system (5) except that p, q, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x109.png" xlink:type="simple"/></inline-formula> in (5) are replaced by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x110.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x111.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x112.png" xlink:type="simple"/></inline-formula> in (24). The solution of (24) immediately gives us the leading coefficients:</p><disp-formula id="scirp.64501-formula784"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x113.png"  xlink:type="simple"/></disp-formula><p>We introduce quantity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x114.png" xlink:type="simple"/></inline-formula>, which will be useful in the subsequent calculation. Quantity</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x115.png" xlink:type="simple"/></inline-formula>has the expression</p><disp-formula id="scirp.64501-formula785"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x116.png"  xlink:type="simple"/></disp-formula><p>Next, we calculate coefficients<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x117.png" xlink:type="simple"/></inline-formula>. Substituting the asymptotic form (16) into equation (20)- (21), and using the fact that all leading coefficients are already known, we find expressions for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x118.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x119.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.64501-formula786"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x120.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula787"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x121.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula788"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x122.png"  xlink:type="simple"/></disp-formula><p>Substituting the asymptotic form (16) into Equations (22)-(23), collecting all terms of the order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x123.png" xlink:type="simple"/></inline-formula>, and using results (27)-(28), we obtain two equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x124.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x125.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.64501-formula789"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x126.png"  xlink:type="simple"/></disp-formula><p>The solution of (30) gives us expressions for coefficients<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x127.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.64501-formula790"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x128.png"  xlink:type="simple"/></disp-formula><p>Before the sensors are assigned to monitor/search routes, the equilibrium distribution of the target-sensors system is</p><disp-formula id="scirp.64501-formula791"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x129.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula792"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x130.png"  xlink:type="simple"/></disp-formula><p>It follows that the overall mean time to detection has the expression</p><disp-formula id="scirp.64501-formula793"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x131.png"  xlink:type="simple"/></disp-formula><p>Therefore, the overall mean time to detection has the asymptotic expansion</p><disp-formula id="scirp.64501-formula794"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x132.png"  xlink:type="simple"/></disp-formula><p>where the coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x133.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x134.png" xlink:type="simple"/></inline-formula> are given by</p><disp-formula id="scirp.64501-formula795"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x135.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula796"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x136.png"  xlink:type="simple"/></disp-formula><p>The normalized transition rates and parameters (shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>) are related to the physical transition rates (shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>) as follows</p><disp-formula id="scirp.64501-formula797"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x137.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula798"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x138.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula799"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x139.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula800"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1040431x140.png"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. Behaviors of the Mean Time to Capture</title><p>We examine behaviors of the mean time to detection, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x141.png" xlink:type="simple"/></inline-formula>, as a function of parameters<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x142.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x143.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x144.png" xlink:type="simple"/></inline-formula>, p, q, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x145.png" xlink:type="simple"/></inline-formula>.</p><p>Observation 1: t<sup>(0)</sup> is a decreasing function of m.</p><p>We differentiate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x146.png" xlink:type="simple"/></inline-formula> as defined in (33) with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x147.png" xlink:type="simple"/></inline-formula> and find that</p><disp-formula id="scirp.64501-formula801"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x148.png"  xlink:type="simple"/></disp-formula><p>In the derivative above, the right-hand side is negative because factors<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x149.png" xlink:type="simple"/></inline-formula>, p, and q are all positive and bounded by 1. This property of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x150.png" xlink:type="simple"/></inline-formula> is not surprising. Recall that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x151.png" xlink:type="simple"/></inline-formula> is the normalized detection rate in the operating area. For a larger<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x152.png" xlink:type="simple"/></inline-formula>, it is reasonable to expect that the target will be detected sooner.</p><p>Observation 2: t<sup>(0)</sup> is a decreasing function of p and a decreasing function of q.</p><p>We differentiate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x153.png" xlink:type="simple"/></inline-formula>, respectively, with respect to p and q and obtain that</p><disp-formula id="scirp.64501-formula802"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x154.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula803"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x155.png"  xlink:type="simple"/></disp-formula><p>Both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x156.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x157.png" xlink:type="simple"/></inline-formula> are negative, which follows directly from the fact that all terms in the numerators are positive. In particular, it is true that</p><disp-formula id="scirp.64501-formula804"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x158.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64501-formula805"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x159.png"  xlink:type="simple"/></disp-formula><p>This property of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x160.png" xlink:type="simple"/></inline-formula> is also expected. Remember that p and q are, respectively, the probability of the target being detected on its way to the operating area and the probability of being detected on its way back to the hiding area. Increasing either p or q while keeping the other unchanged will speed up the detection of the target.</p><p>Observation 3: While (p + q) keeps fixed, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x161.png" xlink:type="simple"/></inline-formula>becomes an increasing function of (pq).</p><p>In the expression of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x162.png" xlink:type="simple"/></inline-formula>, while the sum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x163.png" xlink:type="simple"/></inline-formula> is fixed, the combination <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x164.png" xlink:type="simple"/></inline-formula> appears only in the denominator.</p><disp-formula id="scirp.64501-formula806"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x165.png"  xlink:type="simple"/></disp-formula><p>When the product <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x166.png" xlink:type="simple"/></inline-formula> is increased, the denominator is decreased, and as a result, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x167.png" xlink:type="simple"/></inline-formula>is increased. This behavior tells us that when evaluating several options with the same value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x168.png" xlink:type="simple"/></inline-formula>, the optimal option is the one with the smallest value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x169.png" xlink:type="simple"/></inline-formula>.</p><p>Observation 4: t<sup>(0)</sup> is a decreasing function of b.</p><p>We differentiate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x170.png" xlink:type="simple"/></inline-formula> with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x171.png" xlink:type="simple"/></inline-formula> to get</p><disp-formula id="scirp.64501-formula807"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x172.png"  xlink:type="simple"/></disp-formula><p>This property of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x173.png" xlink:type="simple"/></inline-formula> is expected. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x174.png" xlink:type="simple"/></inline-formula>is the fraction of time that the sensors are on. Increasing the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x175.png" xlink:type="simple"/></inline-formula> leads to an increase in the probability that the sensors are on at a random time. and thus reduces the time to detection.</p><p>Observation 5: When p = q = 0, t<sup>(0)</sup> is a decreasing function of a.</p><p>When sensors are deployed only to search in the operating area and no sensor is used to monitor any of the routes, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x176.png" xlink:type="simple"/></inline-formula>. In this case, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x177.png" xlink:type="simple"/></inline-formula>has the simple expression</p><disp-formula id="scirp.64501-formula808"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x178.png"  xlink:type="simple"/></disp-formula><p>which is a decreasing function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x179.png" xlink:type="simple"/></inline-formula>. When only the operating area is searched, the target can only be detected in the operating area; the target cannot be detected on its travels between the two areas. Consequently, the detection probability increases with the fraction of time that the target spends in the operating area, which is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x180.png" xlink:type="simple"/></inline-formula>.</p><p>Observation 6: In general, t<sup>(0)</sup> is not necessarily a decreasing function of a.</p><p>When the condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula> is not satisfied, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula>may not be monotonic with respect to variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig8">Figure 8</xref> shows a plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula> vs <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula> while other parameters are fixed at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula>initially decreases as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula> is increased from 0. It attains a minimum around<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula>. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x193.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x194.png" xlink:type="simple"/></inline-formula>appears to be an increasing function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x195.png" xlink:type="simple"/></inline-formula>. It is clear that in general, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x196.png" xlink:type="simple"/></inline-formula>is not monotonic with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x197.png" xlink:type="simple"/></inline-formula>.</p><p>Next we study how the mean time to detection changes with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x198.png" xlink:type="simple"/></inline-formula>, the normalized time scale of sensors relaxing to equilibrium between the on- and off-states. For that purpose, we examine coefficient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x199.png" xlink:type="simple"/></inline-formula> in the asymptotic expansion<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x200.png" xlink:type="simple"/></inline-formula>.</p><p>Observation 7: t<sup>(1)</sup> is always positive.</p><p>We write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x201.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.64501-formula809"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x202.png"  xlink:type="simple"/></disp-formula><p>where h is a function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x203.png" xlink:type="simple"/></inline-formula>, given by</p><disp-formula id="scirp.64501-formula810"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x204.png"  xlink:type="simple"/></disp-formula><p>To prove that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x205.png" xlink:type="simple"/></inline-formula> is always positive, we only need to show <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x206.png" xlink:type="simple"/></inline-formula> is always true.</p><p>As a first step, we establish that h is an increasing function of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x207.png" xlink:type="simple"/></inline-formula>, which is reached by differentiating h with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x208.png" xlink:type="simple"/></inline-formula>.</p><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula> vs <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x213.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x214.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x215.png" xlink:type="simple"/></inline-formula>. Note that in general, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x216.png" xlink:type="simple"/></inline-formula>is not monotonic with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x217.png" xlink:type="simple"/></inline-formula>.</title></caption><fig id ="fig8_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x209.png"/></fig></fig-group><disp-formula id="scirp.64501-formula811"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x218.png"  xlink:type="simple"/></disp-formula><p>Thus, to prove<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x219.png" xlink:type="simple"/></inline-formula>, we only need to show<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x220.png" xlink:type="simple"/></inline-formula>. This can be verified directly:</p><disp-formula id="scirp.64501-formula812"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x221.png"  xlink:type="simple"/></disp-formula><p>In the above, we have used the facts</p><disp-formula id="scirp.64501-formula813"><graphic  xlink:href="http://html.scirp.org/file/9-1040431x222.png"  xlink:type="simple"/></disp-formula><p>Therefore, we conclude that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula> is always positive. It follows that as a function of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x224.png" xlink:type="simple"/></inline-formula> while other para- meters are fixed, the mean time to detection <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x225.png" xlink:type="simple"/></inline-formula> decreases as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x226.png" xlink:type="simple"/></inline-formula> is reduced. In other words, when the fraction of time that sensors are on is fixed (i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x227.png" xlink:type="simple"/></inline-formula>is kept at a constant), and when the normalized time scale of sensors relaxing to equilibrium between the on- and off-states is reduced (i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x228.png" xlink:type="simple"/></inline-formula>is made smaller), the detection performance of sensors is improved (i.e., the mean time to detection is shorter).</p><p>Finally, we demonstrate the accuracy of the asymptotic solution for the mean time to detection. <xref ref-type="fig" rid="fig9">Figure 9</xref> compares an accurate numerical solution and the asymptotic expansion <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula>, in the range of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x231.png" xlink:type="simple"/></inline-formula>. It is clear that the dependence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x232.png" xlink:type="simple"/></inline-formula> on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x233.png" xlink:type="simple"/></inline-formula> is well captured in the asymptotic solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x234.png" xlink:type="simple"/></inline-formula> even at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x235.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s7"><title>7. Conclusion</title><p>We have addressed the performance of stochastically intermittent sensors when used to detect a target that moves between a hiding area and an operating area via multiple routes. We have derived asymptotic expansions for the mean time to detection when the on-rate and off-rate of the sensors are large in comparison with the rates of the target moving between the hiding area and the operating area. Using the mean time to detection, we have evaluated the performance of placing sensor(s) to monitor various travel route(s) or to scan the operating area.</p><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Comparison of an accurate numerical solution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula> and the asymptotic solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x239.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x239.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x240.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x239.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x241.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x239.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x242.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x239.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x240.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x242.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1040431x243.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1040431x236.png"/></fig></sec><sec id="s8"><title>Acknowledgements and Disclaimer</title><p>Hong Zhou would like to thank Naval Postgraduate School Center for Multi-INT Studies for supporting this work. Special thanks go to Professor Jim Scrofani and Deborah Shifflett. The authors also thank Mr. Ed Waltz and Dr. Will Williamson for their inspirational suggestions. The views expressed in this document are those of the authors and do not reflect the official policy or position of the Department of Defense or the U.S. Government.</p></sec><sec id="s9"><title>Cite this paper</title><p>HongyunWang,HongZhou, (2016) Performance of Stochastically Intermittent Sensors in Detecting a Target Traveling between Two Areas. American Journal of Operations Research,06,199-212. doi: 10.4236/ajor.2016.62021</p></sec><sec id="s10"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.64501-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Koopman, B.O. (1999) Search and Screening: General Principles with Historical Applications. 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