<?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">AJCM</journal-id><journal-title-group><journal-title>American Journal of Computational Mathematics</journal-title></journal-title-group><issn pub-type="epub">2161-1203</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajcm.2015.53028</article-id><article-id pub-id-type="publisher-id">AJCM-59430</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>
 
 
  Peristaltic Pumping of a Conducting Sisko Fluid through Porous Medium with Heat and Mass Transfer
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>abit</surname><given-names>Tawfiq Mohamed El-Dabe</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>Ahmed</surname><given-names>Younis Ghaly</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>Sallam</surname><given-names>Nagy Sallam</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>Khaled</surname><given-names>Elagamy</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>Yasmeen</surname><given-names>Mohamed Younis</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Education, Ain Shams University, Cairo, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mastermath2003@gmail.com(ATME)</email>;<email>mastermath2003@gmail.com(AYG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>08</month><year>2015</year></pub-date><volume>05</volume><issue>03</issue><fpage>304</fpage><lpage>316</lpage><history><date date-type="received"><day>2</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>4</month>	<year>September</year>	</date><date date-type="accepted"><day>7</day>	<month>September</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The mathematical model is presented for the flow of peristaltic pumping of a conducting non-Newtonian fluid obeying Sisko model through a porous medium under the effect of magnetic field with heat and mass transfer. The solutions of the system of equations which represent this motion are obtained analytically using perturbation technique after considering the approximation of long wave length. The formula of the velocity with temperature and concentration of the fluid is obtained as a function of the physical parameters of the problem. The effects of these parameters on these solutions are discussed numerically and illustrated graphically through some graphs.
 
</p></abstract><kwd-group><kwd>Peristaltic</kwd><kwd> Sisko Fluid</kwd><kwd> MHD</kwd><kwd> Heat and Mass Transfer</kwd><kwd> Chemical Reaction</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Peristalsis is a form of fluid transport induced by a progressive wave of area contraction or expansion along the walls of distensible duct containing a liquid or mixture. A peristaltic pump is a device for pumping fluids, generally from a region of lower to higher pressure, by means of a contraction wave traveling along a tube like structure. Shapiro et al. [<xref ref-type="bibr" rid="scirp.59430-ref1">1</xref>] explained the basic principles and brought out clearly the significances of the various parameters governing the flow. The non-Newtonian effects in peristaltic motion were included in Kaimal [<xref ref-type="bibr" rid="scirp.59430-ref2">2</xref>] . Later several mathematical and experimental models have been developed to understand the fluid mechanical aspects of peristaltic motion. A large body of work already exists on mathematical and experimental models containing a Newtonian or non-Newtonian fluid in a channel.</p><p>Peristalsis also have industrial and biological applications like sanitary fluid transport blood pumps in heart lungs machines and peristaltic transport of toxic liquid is used in nuclear industries. Some recent investigations made to discuss the mechanism of peristalsis include the works. Radhakrishnamacharya and Srinivasulu [<xref ref-type="bibr" rid="scirp.59430-ref3">3</xref>] studied the influence of wall properties on peristaltic transport with heat transfer. Mekheimer and Abd Elmaboud [<xref ref-type="bibr" rid="scirp.59430-ref4">4</xref>] analyzed the influence of heat transfer and magnetic field on peristaltic transport of Newtonian fluid in a vertical annulus. Hayat et al. [<xref ref-type="bibr" rid="scirp.59430-ref5">5</xref>] studied the effect of heat transfer on the peristaltic flow of an electrically conducting fluid in a porous space. Krishna Kumari et al. [<xref ref-type="bibr" rid="scirp.59430-ref6">6</xref>] studied the peristaltic pumping of a magnetohydrodynamic Casson fluid in an inclined channel. Ravi Kumar et al. [<xref ref-type="bibr" rid="scirp.59430-ref7">7</xref>] considered power-law fluid in the study of peristaltic transport.</p><p>The effect of porous medium on the motion of the fluid has been studied by many authors. Elshehawey et al. [<xref ref-type="bibr" rid="scirp.59430-ref8">8</xref>] studied the effect of porous medium on peristaltic motion of a Newtonian fluid. Eldabe [<xref ref-type="bibr" rid="scirp.59430-ref9">9</xref>] studied magnetohydrodynamic flow through a porous medium fluid at a rear stagnation point. Eldabe et al. [<xref ref-type="bibr" rid="scirp.59430-ref8">8</xref>] studied MHD flow and heat transfer in a viscoelastic incompressible fluid confined between a horizontal stretching sheet and a parallel porous wall. Elshehawey et al. [<xref ref-type="bibr" rid="scirp.59430-ref9">9</xref>] studied the peristaltic motion of a Generalized Newtonian fluid through a porous medium. El-Dabe et al. [<xref ref-type="bibr" rid="scirp.59430-ref10">10</xref>] studied the magnetohydrodynamic flow and heat transfer for a peristaltic motion of Carreau fluid through a porous medium.</p><p>The study of the influence of mass and heat transfer on Newtonian and non-Newtonian fluids has become important in the last few years. This importance is due to a number of industrial processes. Examples are food-processing, biochemical operations and transport in polymers. Eldabe et al. [<xref ref-type="bibr" rid="scirp.59430-ref11">11</xref>] studied the heat and mass transfer in hydromagnetic flow of the non-Newtonian fluid with heat source over an accelerating surface through a porous medium. Srinivas and Kothandapani [<xref ref-type="bibr" rid="scirp.59430-ref12">12</xref>] dealt with peristalsis and heat transfer. Hayat et al. [<xref ref-type="bibr" rid="scirp.59430-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.59430-ref15">15</xref>] analyzed the peristaltic mechanism with heat transfer. Eldabe et al. [<xref ref-type="bibr" rid="scirp.59430-ref16">16</xref>] studied the effect of couple stresses on the MHD of a non-Newtonian unsteady flow between two parallel porous plates. The main aim of this study is to investigate the problem of the peristaltic flow of a conducting Sisko fluid in a porous channel with heat and mass transfer; the system of non-linear partial differential equations which describe this motion with heat and mass transfer subjected to the appropriate boundary conditions is solved analytically by using perturbation method. The expressions of the velocity, the temperature and the concentration are determined. The effects of different parameters on these expressions are discussed through graphs.</p></sec><sec id="s2"><title>2. Basic Equations</title><p>The basic equations governing the flow of an incompressible fluid are expressed as follows:</p><p>The continuity equation</p><disp-formula id="scirp.59430-formula918"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x5.png"  xlink:type="simple"/></disp-formula><p>The momentum equation</p><disp-formula id="scirp.59430-formula919"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x7.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.59430-formula920"><label>, (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x8.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x12.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x13.png" xlink:type="simple"/></inline-formula> are the material parameters of the fluid. Note that for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x14.png" xlink:type="simple"/></inline-formula> the fluid describes shear thinning, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x15.png" xlink:type="simple"/></inline-formula> the fluid describes shear thicking, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x16.png" xlink:type="simple"/></inline-formula> the Newtonian fluid is recovered and for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x17.png" xlink:type="simple"/></inline-formula> the generalized power-law model can be obtained.</p><p>The temperature equation</p><disp-formula id="scirp.59430-formula921"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x18.png"  xlink:type="simple"/></disp-formula><p>The concentration equation</p><disp-formula id="scirp.59430-formula922"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x19.png"  xlink:type="simple"/></disp-formula><p>The dissipation function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x20.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.59430-formula923"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x21.png"  xlink:type="simple"/></disp-formula><p>Maxwell s equations</p><disp-formula id="scirp.59430-formula924"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula925"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x23.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula926"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x24.png"  xlink:type="simple"/></disp-formula><p>Ohm’s equation</p><disp-formula id="scirp.59430-formula927"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x25.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x26.png" xlink:type="simple"/></inline-formula> is the velocity vector, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x27.png" xlink:type="simple"/></inline-formula>is the density, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x28.png" xlink:type="simple"/></inline-formula>is the material time derivative, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x29.png" xlink:type="simple"/></inline-formula>is the permea-</p><p>bility, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x30.png" xlink:type="simple"/></inline-formula>is the current density, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x31.png" xlink:type="simple"/></inline-formula>is the electrical conductivity, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x32.png" xlink:type="simple"/></inline-formula>is the magnetic permeability, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x33.png" xlink:type="simple"/></inline-formula></p><p>is the electric field and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x34.png" xlink:type="simple"/></inline-formula> is the Cauchy stress, T and C are temperature and concentration of the fluid, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x35.png" xlink:type="simple"/></inline-formula>is the thermal conductivity, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x36.png" xlink:type="simple"/></inline-formula>is the specific heat capacity at constant pressure, D is the coefficient of mass diffusivity, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x37.png" xlink:type="simple"/></inline-formula>is the thermal diffusion ratio, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x38.png" xlink:type="simple"/></inline-formula>is the mean fluid temperature and A is the reaction rate constant.</p></sec><sec id="s3"><title>3. Mathematical Formulation</title><p>Consider the two-dimensional motion of an incompressible Sisko fluid in an infinite channel of width<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x39.png" xlink:type="simple"/></inline-formula>, see <xref ref-type="fig" rid="fig1">Figure 1</xref>. In the upper wall we assume an infinite sinusoidal wave train moving ahead with constant velocity c along it while the lower plate is fixed at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x40.png" xlink:type="simple"/></inline-formula>. The wavy surface is defined as</p><disp-formula id="scirp.59430-formula928"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x41.png"  xlink:type="simple"/></disp-formula><p>where b is the wave amplitude, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x42.png" xlink:type="simple"/></inline-formula>is the wave length and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x43.png" xlink:type="simple"/></inline-formula> is the time.</p><p>Now, Equations (2)-(6) can be written in two-dimensional <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x44.png" xlink:type="simple"/></inline-formula> as follows:</p><disp-formula id="scirp.59430-formula929"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x45.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula930"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x46.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Sketch of the problem</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x47.png"/></fig><disp-formula id="scirp.59430-formula931"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x48.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula932"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x49.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula933"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x50.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.59430-formula934"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x51.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula935"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula936"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula937"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x54.png"  xlink:type="simple"/></disp-formula><p>Subjected to the following appropriate boundary conditions:</p><disp-formula id="scirp.59430-formula938"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x55.png"  xlink:type="simple"/></disp-formula><p>Choose the wave frame <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x56.png" xlink:type="simple"/></inline-formula> moving with speed c, where</p><disp-formula id="scirp.59430-formula939"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x57.png"  xlink:type="simple"/></disp-formula><p>In which <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x58.png" xlink:type="simple"/></inline-formula> are components of the velocity in the moving coordinates system.</p><p>Then, the Equations (10)-(19) can be written as:</p><disp-formula id="scirp.59430-formula940"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x59.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula941"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x60.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula942"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x61.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula943"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x62.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula944"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x63.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.59430-formula945"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x64.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula946"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x65.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula947"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x66.png"  xlink:type="simple"/></disp-formula><p>The boundary conditions are:</p><disp-formula id="scirp.59430-formula948"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x67.png"  xlink:type="simple"/></disp-formula><p>In order to simplify the governing equations of the motion, we may introduce the following dimensionless transformations:</p><disp-formula id="scirp.59430-formula949"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x68.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x69.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x70.png" xlink:type="simple"/></inline-formula> are the temperature and the concentration of the fluid at the lower wall of the channel, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x71.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x72.png" xlink:type="simple"/></inline-formula> are the temperature and the concentration of the fluid at the upper wall of the channel.</p><p>Substituting (30) into Equations (21)-(29) we obtain the following non-dimensional equations after dropping the star mark:</p><disp-formula id="scirp.59430-formula950"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x73.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula951"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula952"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula953"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula954"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula955"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula956"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula957"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x80.png"  xlink:type="simple"/></disp-formula><p>The boundary conditions are:</p><disp-formula id="scirp.59430-formula958"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x81.png"  xlink:type="simple"/></disp-formula><p>where, the dimensionless parameters are defined by:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula>is the Wave number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula>is the Reynolds number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula>is the Darcy number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula>is the Magnetic field parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula>is the Non-Newtonian parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x87.png" xlink:type="simple"/></inline-formula>is the Prandtle number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x88.png" xlink:type="simple"/></inline-formula>is the Eckert number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x89.png" xlink:type="simple"/></inline-formula>is the Schmidt number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x90.png" xlink:type="simple"/></inline-formula>is the Soret number and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x91.png" xlink:type="simple"/></inline-formula> is the chemical reaction parameter.</p><p>By using the following definition of stream function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x92.png" xlink:type="simple"/></inline-formula> as:</p><disp-formula id="scirp.59430-formula959"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x93.png"  xlink:type="simple"/></disp-formula><p>The system of Equations (3.30)-(3.38) can be written as:</p><disp-formula id="scirp.59430-formula960"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x94.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula961"><label>(42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x95.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula962"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula963"><label>(44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x97.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula964"><label>(45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x98.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula965"><label>(46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x99.png"  xlink:type="simple"/></disp-formula><p>The boundary conditions for the dimensionless stream function in the moving frame are given by:</p><disp-formula id="scirp.59430-formula966"><label>(47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x100.png"  xlink:type="simple"/></disp-formula><p>The dimensionless form of the surface of the peristaltic wall can be written as:</p><disp-formula id="scirp.59430-formula967"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x101.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x102.png" xlink:type="simple"/></inline-formula> is the amplitude ratio or the occlusion. and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x103.png" xlink:type="simple"/></inline-formula>is the total flux number (48)</p></sec><sec id="s4"><title>4. Solution of the Problem</title><p>According to long wavelength approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x104.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.59430-ref1">1</xref>] , Equations (41)-(46) after eliminating the pressure gradient become:</p><disp-formula id="scirp.59430-formula968"><label>(49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula969"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x106.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula970"><label>(51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x107.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula971"><label>(52)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x108.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula972"><label>(53)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x109.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula973"><label>(54)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x110.png"  xlink:type="simple"/></disp-formula><p>In order to solve the Equations (49)-(51) subjected to the boundary conditions, we suppose the following perturbation for small non-Newtonian parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x111.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.59430-formula974"><label>(55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x112.png"  xlink:type="simple"/></disp-formula><p>Substituting (55) into (49)-(54) and comparing the coefficient of zero and first order of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x113.png" xlink:type="simple"/></inline-formula> we get.</p><sec id="s4_1"><title>4.1. Zero Order System of h</title><disp-formula id="scirp.59430-formula975"><label>(56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x114.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula976"><label>(57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula977"><label>(58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x116.png"  xlink:type="simple"/></disp-formula><p>With the respective boundary conditions</p><disp-formula id="scirp.59430-formula978"><label>(59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x117.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_2"><title>4.2. First Order System of h</title><p>We shall consider the case of Dielatent fluids when n &gt; 1, and we choose (n = 3), then we have the following system of first order of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x118.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.59430-formula979"><label>(60)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x119.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula980"><label>(61)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x120.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula981"><label>(62)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x121.png"  xlink:type="simple"/></disp-formula><p>with the respective boundary conditions</p><disp-formula id="scirp.59430-formula982"><label>(63)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x122.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_3"><title>4.3. Solution for System of Zero Order</title><disp-formula id="scirp.59430-formula983"><label>(64)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x123.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula984"><label>(65)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x124.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula985"><label>(66)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x125.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4_4"><title>4.4. Solution for System of First Order</title><disp-formula id="scirp.59430-formula986"><label>(67)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x126.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula987"><label>(68)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x127.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula988"><label>(69)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1100456x128.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s5"><title>5. Results and Discussions</title><p>The problem of the peristaltic flow of a Sisko fluid through a porous medium with heat and mass transfer has been discussed. The effects of non-Newtonian dissipation and chemical reaction on the fluid flow have been considered. We obtained the solutions of the momentum, heat and mass equations analytically by using the perturbation technique for small non-Newtonian parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x129.png" xlink:type="simple"/></inline-formula> after considering the long wave approximations.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> illustrates the relation between the value of stream function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x130.png" xlink:type="simple"/></inline-formula> and the magnetic parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x131.png" xlink:type="simple"/></inline-formula>, it is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x132.png" xlink:type="simple"/></inline-formula> increases with increasing the magnetic parameter, while it decreases with increasing the permeability parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x133.png" xlink:type="simple"/></inline-formula> which seen through <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref>, the relation between the value of stream function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x134.png" xlink:type="simple"/></inline-formula> and the amplitude ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x135.png" xlink:type="simple"/></inline-formula> has been illustrated. it is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x136.png" xlink:type="simple"/></inline-formula> decreases with the decrease of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x137.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref>, illustrates the relation between the value of temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x138.png" xlink:type="simple"/></inline-formula> and the magnetic parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x139.png" xlink:type="simple"/></inline-formula>, it is clear that increases with increasing the magnetic parameter.</p><p>In <xref ref-type="fig" rid="fig6">Figure 6</xref>, we can observe that the value of temperature increases with increasing the Prandtle number parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x140.png" xlink:type="simple"/></inline-formula>, while in <xref ref-type="fig" rid="fig7">Figure 7</xref>, the relation between the value of temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x141.png" xlink:type="simple"/></inline-formula> and the Eckert number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x142.png" xlink:type="simple"/></inline-formula> has been illustrated. It is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x143.png" xlink:type="simple"/></inline-formula> increases with the increase of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x144.png" xlink:type="simple"/></inline-formula>.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Stream function profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x146.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x147.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x145.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Stream function profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x149.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x150.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x148.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Stream function profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x152.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x153.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x151.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Temperature profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x155.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x156.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x154.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Temperature profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x158.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x159.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x157.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Temperature profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x161.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x162.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x160.png"/></fig><p>In <xref ref-type="fig" rid="fig8">Figure 8</xref>, the relation between the value of concentration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula> and the magnetic parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula>, it is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula> decreases with increasing the magnetic parameter. But we can observe from <xref ref-type="fig" rid="fig9">Figure 9</xref> that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula> decreases with increasing the Schmidt parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x167.png" xlink:type="simple"/></inline-formula>, also in <xref ref-type="fig" rid="fig1">Figure 1</xref>0, the relation between the value of concentration function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x168.png" xlink:type="simple"/></inline-formula> and the Soret value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x169.png" xlink:type="simple"/></inline-formula> has been illustrated. It is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x170.png" xlink:type="simple"/></inline-formula> increases with the increase of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x171.png" xlink:type="simple"/></inline-formula> as in <xref ref-type="fig" rid="fig1">Figure 1</xref>1.</p></sec><sec id="s6"><title>6. Conclusion and Applications</title><p>In this work, we study the peristaltic motion of magneto-hydrodynamics flow with heat and mass transfer for incompressible non-Newtonian fluid through a porous medium. The governing partial differential equations of this problem, subjected to the boundary conditions are solved analytically by using perturbation technique. The</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Concentration profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x173.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x174.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x172.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Concentration profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x176.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x177.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x175.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Concentration profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x179.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x180.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x178.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> Concentration profiles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x182.png" xlink:type="simple"/></inline-formula> for some values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x183.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-1100456x181.png"/></fig><p>analytical forms for the stream distribution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula>, the temperature <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula> and the concentration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula> are obtained. The effects of various physical parameters of the problem on these formulas are discussed and have been shown graphically. It is seen that the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x187.png" xlink:type="simple"/></inline-formula> increases with increasing the magnetic parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x188.png" xlink:type="simple"/></inline-formula>, while it decreases with increasing the permeability parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x189.png" xlink:type="simple"/></inline-formula>. Also it is clear that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x190.png" xlink:type="simple"/></inline-formula> increases with the increase of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1100456x191.png" xlink:type="simple"/></inline-formula>,</p><p>The study of this phenomenon is very important, because the study of flow through porous medium has many applications. It has an important role in agricultural, extracting pure petrol from crude oil and chemical engineering. There are examples of natural porous media such as wood, filter paper, cotton, leather and plastics. As a good biological example on the porous medium, the human lung galls bladder and the walls of vessels. The peristaltic motion has been found to involve in many biological organs such as esophagus, small and large intestine, stomach, the human ureter, lymphatic vessels and small blood vessels. Also, peristaltic transport occurs in many practical applications involving biomechanical systems such as finger pumps.</p></sec><sec id="s7"><title>Cite this paper</title><p>Nabit Tawfiq MohamedEl-Dabe,Ahmed YounisGhaly,Sallam NagySallam,KhaledElagamy,Yasmeen MohamedYounis, (2015) Peristaltic Pumping of a Conducting Sisko Fluid through Porous Medium with Heat and Mass Transfer. American Journal of Computational Mathematics,05,304-316. doi: 10.4236/ajcm.2015.53028</p></sec><sec id="s8"><title>Appendix</title><disp-formula id="scirp.59430-formula989"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x192.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula990"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x193.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula991"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x194.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula992"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x195.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59430-formula993"><graphic  xlink:href="http://html.scirp.org/file/9-1100456x196.png"  xlink:type="simple"/></disp-formula></sec></body><back><ref-list><title>References</title><ref id="scirp.59430-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Shapiro, A.H., Jafferin, M.Y. and Weinberg, S.L. (1969) Peristaltic Pumping with Long Wave Lengths at Low Reynolds Number. Journal Fluid Mechanics, 35, 669-675.</mixed-citation></ref><ref id="scirp.59430-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Kaimal, M.R. (1978) Peristaltic Pumping of Non-Newtonian Fluid at Low Reynolds Number under Long Wave Approximation. Journal of Applied Mechanics, 45, 32. http://dx.doi.org/10.1115/1.3424270</mixed-citation></ref><ref id="scirp.59430-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Radhakrishnamacharya, G. and Srinivasulu, C. (2007) Influence of Wall Properties on Peristaltic Transport with Heat Transfer. Comptes Rendus Mecanique, 335, 369-373. http://dx.doi.org/10.1016/j.crme.2007.05.002</mixed-citation></ref><ref id="scirp.59430-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Hayat, T., Qureshi, M.U. and Hussain, Q. (2009) Effect of Heat Transfer on the Peristaltic Flow of an Electrically Conducting Fluid in a Porous Space. Applied Mathematical Modelling, 33, 1862-1873.  
http://dx.doi.org/10.1016/j.apm.2008.03.024</mixed-citation></ref><ref id="scirp.59430-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Abd Elmaboud, Y. and Mekheimer, Kh.S. (2008) Peristaltic Flow of a Couple Stress Fluid in an Annulus: Application of an Endoscope. Physica A: Statistical Mechanics and Its Applications, 387, 2403-2415.  
http://dx.doi.org/10.1016/j.physa.2007.12.017</mixed-citation></ref><ref id="scirp.59430-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Krishna Kumari.P, S.V.H.N., Ramana Murthy, M.V., Chenna Krishna Reddy, M. and Ravi Kumar, Y.V.K. (2011) Peristaltic Pumping of a Magnetohydrodynamic Casson Fluid in an Inclined Channel. Advances in Applied Science Research, 2, 428-436.</mixed-citation></ref><ref id="scirp.59430-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Ravi Kumar, Y.V.K., Krishna Kumari.P, S.V.H.N., Ramana Murthy, M.V. and Sreenadh, S. (2011) Peristaltic Transport of a Power-Law Fluid in an Assymmetric Channel Bounded by Permeable Walls. Advances in Applied Sciences, 2, 396-340.</mixed-citation></ref><ref id="scirp.59430-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Eldabe, N.T. and Sallam, S.N. (1998) Magenetohydrodynamic Flow and Heat Transfer in a Viscoelastic Incompressible Fluid Confined between a Horizontal Stretching Sheet and a Parallel Porous Wall. Canadian Journal of Physics, 76, 98. http://dx.doi.org/10.1139/cjp-76-12-949</mixed-citation></ref><ref id="scirp.59430-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">El Shehawey, E.F. and El Sebaei, W. (2000) Peristaltic Transport in a Cylindrical Tube through a Porous Medium. International Journal of Mathematics and Mathematical Sciences, 26, 217-230.  
http://dx.doi.org/10.1155/S0161171200004737</mixed-citation></ref><ref id="scirp.59430-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">El-Dabe, N.T.M., Fouad, A. and Hussein, M.M. (2010) Magnetohydrodynamic Flow and Heat Transfer for a Peristaltic Motion of Carreau Fluid through a Porous Medium. Punjab University Journal of Mathematics, 42, 1-16.</mixed-citation></ref><ref id="scirp.59430-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Eldabe, N.T. and Mohamed, M.A.A. (2002) Heat and Mass Transfer in Hydromagnetic Flow of the Non-Newtonian Fluid with Heat Source over an Accelerating Surface through a Porous Medium. Chaos, Solitons and Fractals, 13, 907-917. http://dx.doi.org/10.1016/S0960-0779(01)00066-2</mixed-citation></ref><ref id="scirp.59430-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Srinivas, S. and Kothandapani, M. (2008) Peristaltic Transport in an Asymmetric Channel with Heat Transfer—A Note. International Communications in Heat and Mass Transfer, 35, 514-522.  
http://dx.doi.org/10.1016/j.icheatmasstransfer.2007.08.011</mixed-citation></ref><ref id="scirp.59430-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Hayat, T., Abbasi, F.M. and Alsaedi, A. (2014a) Soret and Dufour Effects on Peristaltic Flow in an Asymmetric Channel. Arabian Journal for Science and Engineering, 39, 4341-4349. http://dx.doi.org/10.1007/s13369-014-1163-y</mixed-citation></ref><ref id="scirp.59430-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Hayat, T., Hina, S., Hendi, A.A. and Asghar, S. (2011) Effect of Wall Properties on the Peristaltic Flow of a Third Grade Fluid in a Curved Channel with Heat and Mass Transfer. International Journal of Heat and Mass Transfer, 54, 5126-5136. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2011.07.036</mixed-citation></ref><ref id="scirp.59430-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Hayat, T., Noreen, S., Alhothuali, M.S., Asghar, S. and Alhomaidan, A. (2012) Peristaltic Flow under the Effects of an Induced Magnetic Field and Heat and Mass Transfer. International Journal of Heat and Mass Transfer, 55, 443-452.  
http://dx.doi.org/10.1016/j.ijheatmasstransfer.2011.09.044</mixed-citation></ref><ref id="scirp.59430-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Eldabe, N.T., Hassan, A.A. and Mohamed, M.A.A. (2003) Effect of Couple Stresses on the MHD of a Non-Newtonian Unsteady Flow between Two Parallel Porous Plates. Zeitschrift für Naturforschung, 58, 204-210.  
http://dx.doi.org/10.1515/zna-2003-0405</mixed-citation></ref></ref-list></back></article>