<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.79080</article-id><article-id pub-id-type="publisher-id">AM-66811</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>
 
 
  Study of the Influence of Nanoparticles on the Molecular Model of an Ideal Fluid
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ahammadali</surname><given-names>Ahmad oglu Ramazanov</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>Mammad</surname><given-names>Samad oglu Aslanov</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Azerbayjan Technical University, Baku, Azerbaijan</addr-line></aff><aff id="aff1"><addr-line>Baku State University, Baku, Azerbaijan</addr-line></aff><pub-date pub-type="epub"><day>26</day><month>05</month><year>2016</year></pub-date><volume>07</volume><issue>09</issue><fpage>908</fpage><lpage>911</lpage><history><date date-type="received"><day>28</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>24</month>	<year>May</year>	</date><date date-type="accepted"><day>27</day>	<month>May</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>
 
 
  In the article a molecular model of oil with nanoparticles on the basis of the model of ideal fluid is considered. It is assumed that the molecular model of the oil can be represented as a homogenous distribution of identical molecules in space. It is assumed that the central interaction between the oil molecules and nanoparticles, results in a change of the model parameters. It is shown that for an ideal fluid the effect of nanoparticles is reduced to a change of the coefficient at the pressure.
 
</p></abstract><kwd-group><kwd>Ideal Fluid</kwd><kwd> Molecular Model of Oil</kwd><kwd> Nanoparticles</kwd><kwd> Coefficient of Elasticity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>At the present time the development of effective technologies, based on nanotechnology in the fields of oil, automotive, shipbuilding, construction, aviation industries and etc. is highly evaluated. For example, the application of nanotechnology in the oil industry is associated with an increase of the oil recovery factor of high- viscosity oil fields and in this direction was carried out numerous studies [<xref ref-type="bibr" rid="scirp.66811-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.66811-ref7">7</xref>] .</p><p>Developed countries spend significant expenditures on the development of oil science that allows creating cost-effective technologies for the extraction of hard recoverable oil reserves.</p><p>According to the material of the London Forum on oil recovery, applications of already developed advanced technologies allow raising the average recovery factor up to 50% by 2020, which in turn increase oil recovery of the proven world’s oil reserves on 1.4 times [<xref ref-type="bibr" rid="scirp.66811-ref3">3</xref>] .</p><p>It is known that the oil is a complex mixture of hydrocarbons and carbon compounds. Not separated into individual components, it can be accepted as an ideal fluid in a molecular level.</p><p>So, study of the model of an ideal fluid containing nanoparticles is of scientific interest and is very relevant in the nanotechnology field.</p></sec><sec id="s2"><title>2. Formulation of the Problem</title><p>It is known that the liquid has a continuum and when it is at rest or moves as a rigid body, only the normal stress is observed and at the same time there is no shear stress.</p><p>In real fluids shear stresses are not equal to zero, but too small and incomparable to the normal stresses. In such cases, the liquid is taken as the ideal fluid [<xref ref-type="bibr" rid="scirp.66811-ref3">3</xref>] .</p><p>In contrast to the continuum hypothesis when considered liquid system is described on the molecular scale, it is necessary to model the system by molecular dynamics. The essence of this method is as follows: an ensemble of particles formed from atoms and molecules that is individually accepted as material points. It is assumed that the particles containing atoms and molecules interact to each other and can be subjected to external interaction. Interatomic or intermolecular interactions are described by means of van der Waals forces, which are mathematically expressed by Lennard-Jones potential [<xref ref-type="bibr" rid="scirp.66811-ref3">3</xref>] .</p><p>In the nature a real fluid characterised by the physical properties of an incompressible fluid that has constant density and the friction force between the particles. Due to difficulty of describing of hydrodynamic processes in such fluids and in order to simplify the solving of tasks relating them the concept of an ideal fluid is introduced. It is assumed that the viscosity of an ideal fluid is equal zero, i.e., there is no friction between the particles. Despite the fact of ideal fluid does not exist, these assumptions facilitates the study of the mechanical properties of real liquids and solutions of some problems.</p><p>Required to identify the impact of nanoparticles on the molecular model of an ideal fluid.</p></sec><sec id="s3"><title>3. The Solution of the Problem</title><p>Assume that the ideal liquid is the body, wherein the tension in all directions is equal.</p><p>Based on this assumption the molecular model of oil can be represented as uniform distribution of identical molecules in space. There is a central interaction between these molecules. We accept the strength of the interaction <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x6.png" xlink:type="simple"/></inline-formula> elastic and low, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x7.png" xlink:type="simple"/></inline-formula>,</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x8.png" xlink:type="simple"/></inline-formula>―the initial distance, a―the distance between the interacting molecules, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x9.png" xlink:type="simple"/></inline-formula>, c―the coefficient of elasticity (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>For the construction of the defining equation draw the plane. We distinguish molecules with the smallest distance to the plane. Draw a line perpendicular to the plane. Their numbers N,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x10.png" xlink:type="simple"/></inline-formula>. The total force is equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x11.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x12.png" xlink:type="simple"/></inline-formula>―stress. On the other hand</p><disp-formula id="scirp.66811-formula1596"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402843x13.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x14.png" xlink:type="simple"/></inline-formula>; k―the number of planes that do not have contact (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>From (1) we obtain</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x15.png" xlink:type="simple"/></inline-formula>.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Scheme of the interaction between molecules</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-7402843x16.png"/></fig><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x17.png" xlink:type="simple"/></inline-formula> is not dependent on the angle of inclination of the plane, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x18.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.66811-formula1597"><label>. (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402843x19.png"  xlink:type="simple"/></disp-formula><p>From (2) it follows that the voltage in an ideal fluid is, the compressive stress and no slip, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x20.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x22.png" xlink:type="simple"/></inline-formula></p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x23.png" xlink:type="simple"/></inline-formula>―the Kronecker symbol (<xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x24.png" xlink:type="simple"/></inline-formula>, then we get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x25.png" xlink:type="simple"/></inline-formula>.</p><p>The physical meaning of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x26.png" xlink:type="simple"/></inline-formula>―the relative change in volume, i.e. p―depends on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x27.png" xlink:type="simple"/></inline-formula> or p depends of the density (at constant mass the volume change leads to a change in density).</p><p>Addition of nanoparticles leads to a change of the molecular model of oil. Then, the liquid keeps staying ideal, or will become non-ideal. In case the liquid keep staying ideal, then molecular model takes the form (see <xref ref-type="fig" rid="fig4">Figure 4</xref>).</p><p>In the I and II models there are sliding (shear) i.e. these are non-ideal fluids. In the III model the interaction is central.</p><p>Drawing the plane through the liquid medium containing nanoparticles, we get the following model (<xref ref-type="fig" rid="fig5">Figure 5</xref>).</p><p>I row is not considered as the closest row is the row of nanoparticles. Then</p><disp-formula id="scirp.66811-formula1598"><graphic  xlink:href="http://html.scirp.org/file/9-7402843x28.png"  xlink:type="simple"/></disp-formula><p>where index “n” means, that this value refers to nanoparticles.</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The scheme of arrangement of the molecules relatively to the plane separating the liquid medium.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-7402843x29.png"/></fig></fig-group><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The scheme of interactions of atoms in the presence of vacancies</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-7402843x30.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Molecular models of the oil with the addition of nanoparticles</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-7402843x31.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The scheme of arrangement of the nanoparticles relatively to the plane separating the liquid medium</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-7402843x32.png"/></fig><p>Finally, we find that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x33.png" xlink:type="simple"/></inline-formula>.</p><p>Thus, for an ideal fluid the effect of nanoparticles is reduced to a change of the coefficient at pressure.</p><p>Note that non-ideal fluid is a body in which the voltage is a superposition of the voltage of an ideal fluid and shifting, i.e., this ideal fluid is taken with consideration of shear deformation. Hence we can say that non-ideal fluid is the body, which changes its shape, but does not change the volume<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402843x34.png" xlink:type="simple"/></inline-formula>.</p><p>Molecular model of non-ideal fluid is the same that for ideal fluid but the molecules can participate simultaneously in two (or more) of motion, i.e. there is possible shift.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In the article a molecular model of oil with nanoparticles on the basis of the model of ideal fluid is described. It is assumed that the molecular model of the oil can be represented as a homogenous distribution of identical molecules in space. It is assumed that the central interaction between the oil molecules and nanoparticles, results in a change of the model parameters. It is shown that for an ideal fluid the effect of nanoparticles is reduced to a change of the coefficient at the pressure.</p></sec><sec id="s5"><title>Cite this paper</title><p>Mahammadali Ahmad oglu Ramazanov,Mammad Samad oglu Aslanov, (2016) Study of the Influence of Nanoparticles on the Molecular Model of an Ideal Fluid. Applied Mathematics,07,908-911. doi: 10.4236/am.2016.79080</p></sec></body><back><ref-list><title>References</title><ref id="scirp.66811-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Khavkin, A.J. (2008) Nanotechnology in Oil and Gaza. The Campaign Sputnik, 149 p.</mixed-citation></ref><ref id="scirp.66811-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Sergeev, G.B. (2007) Nanochemistry: Textbook. 2nd Edition, KDU, 336 p.</mixed-citation></ref><ref id="scirp.66811-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Abdullayev, S. and Nagiyev, F. 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