<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2016.47123</article-id><article-id pub-id-type="publisher-id">JAMP-67935</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>
 
 
  Dynamics of a Two Species Competitive System with Pure Delays
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Talat</surname><given-names>Tayir</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Rouzimaimaiti</surname><given-names>Mahemuti</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xamxinur</surname><given-names>Abdurahman</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Mathematics and System Sciences, Xinjiang University, Urumqi, China</addr-line></aff><pub-date pub-type="epub"><day>30</day><month>06</month><year>2016</year></pub-date><volume>04</volume><issue>07</issue><fpage>1186</fpage><lpage>1191</lpage><history><date date-type="received"><day>6</day>	<month>May</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>1</month>	<year>July</year>	</date><date date-type="accepted"><day>4</day>	<month>July</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>
 
 
  A class of non-autonomous two species Lotka-Volterra competitive system with pure discrete time delays is discussed. Some sufficient conditions on the boundedness, permanence, periodic solution and global attractivity of the system are established by means of the comparison method and Liapunov functional.
 
</p></abstract><kwd-group><kwd>Lotka-Volterra Competitive System</kwd><kwd> Discrete Time Delay</kwd><kwd> Liapunov Functional</kwd><kwd> Global Attractivity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Population competition systems of Lotka-Volterra type have been investigated extensively in recent years [<xref ref-type="bibr" rid="scirp.67935-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67935-ref5">5</xref>] . The basic and the simplest two species nonautonomous competitive system for Lotka-Volterra type is as following form</p><disp-formula id="scirp.67935-formula770"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x7.png"  xlink:type="simple"/></disp-formula><p>There is an extensive literature concerned with the properties of system (1) that has been discussed by many authors [<xref ref-type="bibr" rid="scirp.67935-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67935-ref4">4</xref>] .</p><p>However, in the real world, the growth rate of a natural species will not often respond immediately to changes in its own population or that of an interacting species, but will rather do so after a time lag [<xref ref-type="bibr" rid="scirp.67935-ref6">6</xref>] . Recently, many people are doing research on the dynamics of population with time delays, which is useful for the control of the population of mankind, animals and the environment. Therefore, it is essential for us to investigate population systems with time delays. In this paper, we investigate the following two species Lotka-Volterra type competitive systems with pure discrete time delays</p><disp-formula id="scirp.67935-formula771"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x8.png"  xlink:type="simple"/></disp-formula><p>By using the technique of comparison method and Liapunov function method, we will establish some sufficient conditions on the boundedness, permanence, existence of positive periodic solution and global attractivity of the system.</p><p>The organization of this paper is as follows. In the next Section, we will present some basic assumptions and main definition and lemmas. In Section 3, conditions for the positivity and boundedness are considered. In the final Section, we considered the conditions for the permanence, existence of positive periodic solution and global attractivity of the system.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>In system (2), we have that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x9.png" xlink:type="simple"/></inline-formula> represent the density of two competitive species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x10.png" xlink:type="simple"/></inline-formula> at time t, respectively; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x11.png" xlink:type="simple"/></inline-formula>represent the intrinsic growth rate of species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x12.png" xlink:type="simple"/></inline-formula> at time t, respectively; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x13.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x14.png" xlink:type="simple"/></inline-formula> represent the intra patch restriction density of species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x15.png" xlink:type="simple"/></inline-formula> at time t, respectively; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x16.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x17.png" xlink:type="simple"/></inline-formula> represent the competitive coefficients between two species <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x18.png" xlink:type="simple"/></inline-formula> at time t, respectively. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x19.png" xlink:type="simple"/></inline-formula>represent the time delay in the model. In this paper, we always assume that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x20.png" xlink:type="simple"/></inline-formula>are positive constants, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x22.png" xlink:type="simple"/></inline-formula>are continuous positive functions.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x23.png" xlink:type="simple"/></inline-formula>are positive constants, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x24.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x25.png" xlink:type="simple"/></inline-formula>are continuous positive ω-peri- odic functions.</p><p>From the viewpoint of mathematical biology, in this paper for system (2) we only consider the solution with the following initial conditions</p><disp-formula id="scirp.67935-formula772"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x26.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x27.png" xlink:type="simple"/></inline-formula> are nonnegative continuous functions defined on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x28.png" xlink:type="simple"/></inline-formula> satisfying <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x29.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x30.png" xlink:type="simple"/></inline-formula>.</p><p>In this paper, for any continuous function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x31.png" xlink:type="simple"/></inline-formula> we denote</p><disp-formula id="scirp.67935-formula773"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x32.png"  xlink:type="simple"/></disp-formula><p>Now, we present some useful definitions.</p><p>Definition 1. (see [<xref ref-type="bibr" rid="scirp.67935-ref7">7</xref>] ) System (2) is said to be permanent if there exists a compact region <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x33.png" xlink:type="simple"/></inline-formula> such that every solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x34.png" xlink:type="simple"/></inline-formula> of system (2) with initial conditions (3) eventually enters and remains in the region D.</p><p>Definition 2. (see [<xref ref-type="bibr" rid="scirp.67935-ref8">8</xref>] ) System (2) is said to be global attractive, if for any two positive solutions</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x35.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x36.png" xlink:type="simple"/></inline-formula> of system (2), one has</p><disp-formula id="scirp.67935-formula774"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x37.png"  xlink:type="simple"/></disp-formula><p>The following two lemmas will be used in the proof of the main results of system (2).</p><p>Lemma 1. (see [<xref ref-type="bibr" rid="scirp.67935-ref9">9</xref>] ) Consider the following equation:</p><disp-formula id="scirp.67935-formula775"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x38.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x39.png" xlink:type="simple"/></inline-formula>, we have</p><p>1) If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x40.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x41.png" xlink:type="simple"/></inline-formula>.</p><p>2) If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x42.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x43.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 2. (see [<xref ref-type="bibr" rid="scirp.67935-ref10">10</xref>] ) Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula> be a nonnegative function defined on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x45.png" xlink:type="simple"/></inline-formula>, such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x46.png" xlink:type="simple"/></inline-formula> is integrable on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x47.png" xlink:type="simple"/></inline-formula> and uniformly continuous on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x48.png" xlink:type="simple"/></inline-formula>. Then,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x49.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Positivity and Boundedness</title><p>In this section, we will obtain positivity and boundedness of system (2). The following Lemma is about the positivity of system (2).</p><p>Lemma 1. Set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x50.png" xlink:type="simple"/></inline-formula> is positively invariant for system (2).</p><p>The proof of Lemma1 is simple, and here we omit it.</p><p>The following theorem is about the boundedness of system (2).</p><p>Theorem 1. Suppose that assumption (H<sub>1</sub>) holds, then there exist positive constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x51.png" xlink:type="simple"/></inline-formula> such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x52.png" xlink:type="simple"/></inline-formula>for any positive solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x53.png" xlink:type="simple"/></inline-formula> of system (2).</p><p>Proof: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x54.png" xlink:type="simple"/></inline-formula> be a solution of system (2). Firstly, it follows from the first equation of system (2) that for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x55.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.67935-formula776"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x56.png"  xlink:type="simple"/></disp-formula><p>We consider the following auxiliary equation</p><disp-formula id="scirp.67935-formula777"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x57.png"  xlink:type="simple"/></disp-formula><p>By Lemma 2, we derive</p><disp-formula id="scirp.67935-formula778"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x58.png"  xlink:type="simple"/></disp-formula><p>By comparison, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x59.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x60.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x61.png" xlink:type="simple"/></inline-formula>.</p><p>Next, by using an argument similar in the above, there exist a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x62.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x63.png" xlink:type="simple"/></inline-formula>, where</p><disp-formula id="scirp.67935-formula779"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x64.png"  xlink:type="simple"/></disp-formula><p>This completes the proof.</p><p>The following theorem is about the global attractivity of system (2). Firstly, for convenience we denote the following functions</p><disp-formula id="scirp.67935-formula780"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x65.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.67935-formula781"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x66.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x67.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x68.png" xlink:type="simple"/></inline-formula> are constants.</p></sec><sec id="s4"><title>4. Permanence, Existence of Positive Periodic Solution and Global Attractivity</title><p>In this section, we will obtain the permanence, existence of positive periodic solution and global attractivity of system (2). First we obtain the global attractivity of system (2).</p><p>Theorem 2. Suppose that (H<sub>1</sub>) and there exists a constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x69.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.67935-formula782"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x70.png"  xlink:type="simple"/></disp-formula><p>Then system (2) has a positive solution which is globally attractive.</p><p>Proof: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x71.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x72.png" xlink:type="simple"/></inline-formula> are any two positive solutions of system (2). From Theorem 1, choose positive constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x73.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.67935-formula783"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x74.png"  xlink:type="simple"/></disp-formula><p>for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x75.png" xlink:type="simple"/></inline-formula>. Let</p><disp-formula id="scirp.67935-formula784"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x76.png"  xlink:type="simple"/></disp-formula><p>Calculating the upper right derivation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x77.png" xlink:type="simple"/></inline-formula> along system (2) for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x78.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.67935-formula785"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x79.png"  xlink:type="simple"/></disp-formula><p>Define</p><disp-formula id="scirp.67935-formula786"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x80.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.67935-formula787"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x81.png"  xlink:type="simple"/></disp-formula><p>Calculating the upper right derivative of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x82.png" xlink:type="simple"/></inline-formula> and from (6), we have</p><disp-formula id="scirp.67935-formula788"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x83.png"  xlink:type="simple"/></disp-formula><p>Define</p><disp-formula id="scirp.67935-formula789"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x84.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.67935-formula790"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x85.png"  xlink:type="simple"/></disp-formula><p>Further, we define a Liapunov function as follows</p><disp-formula id="scirp.67935-formula791"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x86.png"  xlink:type="simple"/></disp-formula><p>Calculating the upper right derivation of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x87.png" xlink:type="simple"/></inline-formula>, from (6) and (7) we finally can obtain for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x88.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.67935-formula792"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x89.png"  xlink:type="simple"/></disp-formula><p>From assumption (H<sub>2</sub>), there exists a constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x90.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x91.png" xlink:type="simple"/></inline-formula> such that for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x92.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.67935-formula793"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x93.png"  xlink:type="simple"/></disp-formula><p>Integrating from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x94.png" xlink:type="simple"/></inline-formula> to t on both sides of (8) and by (9) produces</p><disp-formula id="scirp.67935-formula794"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x95.png"  xlink:type="simple"/></disp-formula><p>hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x96.png" xlink:type="simple"/></inline-formula>bounded on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x97.png" xlink:type="simple"/></inline-formula> and we have</p><disp-formula id="scirp.67935-formula795"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720590x98.png"  xlink:type="simple"/></disp-formula><p>From the boundedness of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x99.png" xlink:type="simple"/></inline-formula> and (11), we can obtain that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x100.png" xlink:type="simple"/></inline-formula> and their derivatives remain bounded on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x101.png" xlink:type="simple"/></inline-formula>. Therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x102.png" xlink:type="simple"/></inline-formula> is uniformly continuous on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x103.png" xlink:type="simple"/></inline-formula>. By Barbalat’s theorem it follows that</p><disp-formula id="scirp.67935-formula796"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x104.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.67935-formula797"><graphic  xlink:href="http://html.scirp.org/file/2-1720590x105.png"  xlink:type="simple"/></disp-formula><p>This completes the proof of Theorem 2.</p><p>From the global attractivity of system (2), we have the following result.</p><p>Corollary 1. Suppose that the conditions of Theorem 2 hold, then system (2) is permanent.</p><p>As a direct corollary of [<xref ref-type="bibr" rid="scirp.67935-ref11">11</xref>] (Theorem 2), from Corollary 1, we have the following result.</p><p>Corollary 2. Suppose that the conditions of Theorem 2 and (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720590x106.png" xlink:type="simple"/></inline-formula>) hold, then system (2) has a positive ω-peri- odic solution which is globally attractive.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by the Natural Science Foundation of Xinjiang University (Starting Fund for Doctors, Grant No. BS130102, BS150202) and the National Natural Science Foundation of China (Grant No. 11401509, 11261056).</p></sec><sec id="s6"><title>Cite this paper</title><p>Talat Tayir,Rouzimaimaiti Mahemuti,Xamxinur Abdurahman, (2016) Dynamics of a Two Species Competitive System with Pure Delays. Journal of Applied Mathematics and Physics,04,1186-1191. doi: 10.4236/jamp.2016.47123</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.67935-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ahmad, S. (1987) Convergence and Ultimate Bounds of the Nonautonomous Volterra-Lotka Competition Equation. Journal of Mathematical Analysis and Applications, 127, 377-387. http://dx.doi.org/10.1016/0022-247X(87)90116-8</mixed-citation></ref><ref id="scirp.67935-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Ahmad, S. (1993) On the Nonautonomous Volterra-Lotka Competition Equations. Proceedings of the American Mathematical Society, 117, 199-204. http://dx.doi.org/10.1090/S0002-9939-1993-1143013-3</mixed-citation></ref><ref id="scirp.67935-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Peng, Q.L. and Chen, L.S. 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