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    <journal-meta>
      <journal-id journal-id-type="publisher">journal-of-dynamical-systems-and-geometric-theories</journal-id>
      <journal-title-group>
        <journal-title>Journal of Dynamical Systems and Geometric Theories</journal-title>
      </journal-title-group>
      <issn publication-format="electronic">2169-0057</issn>
      <issn publication-format="print">1726-037X</issn>
      <publisher>
        <publisher-name>Taru Publications</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.1080/1726037X.2015.1029330</article-id>
      <title-group>
        <article-title>Kaluza-Klein Type Cosmological Model with Ω–Dependent Cosmological Constant and Big Rip Singularity</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name>
            <surname>Wanjari</surname>
            <given-names>Rupali</given-names>
          </name>
          <aff>Department Of Mathematics, Mahatma Jyotiba Phule Educational Campus, Amravati Road, Rashtrasant Tukadoji Maharaj Nagpur University, s:, Nagpur, 440033, India</aff>
        </contrib>
      </contrib-group>
      <volume>13</volume>
      <issue>1</issue>
      <fpage>43</fpage>
      <lpage>50</lpage>
      <pub-date date-type="pub">
        <day>02</day>
        <month>06</month>
        <year>2015</year>
      </pub-date>
      <abstract>
        <p>In this paper by using the modified EOS of the form p=– ρ–f(ρ) we investigate the evolution of the scale factor in Kaluza-Klein type cosmological model in which cosmological constant is given by the scalar arisen by the contraction of the scale energy tensor. It is shown that the big rip singularity occurs at finite time t = tundefined by violating null, weak, strong energy condition and satisfying the dominant energy condition for α &gt; 0. For the general case f(ρ) = αρ(undefined), it is observed that for β= 1/2 &gt;0,R(t), p(t) and H(t) → ∞ are reached at a finite time tundefined = 2/bundefined, where b0 is constant. So again take place big rip singularity at a finite time. However, for β &lt; 0, singularity does not occurs at a finite time in the framework of Kaluza-Klein theory of gravitation.</p>
      </abstract>
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</article>
