<?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">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2016.612065</article-id><article-id pub-id-type="publisher-id">APM-72060</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>
 
 
  Local Solutions to a Class of Parabolic System Related to the P-Laplacian
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Qitong</surname><given-names>Ou</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>Huashui</surname><given-names>Zhan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Applied Mathematics, Xiamen University of Technology, Xiamen, China</addr-line></aff><pub-date pub-type="epub"><day>08</day><month>11</month><year>2016</year></pub-date><volume>06</volume><issue>12</issue><fpage>868</fpage><lpage>877</lpage><history><date date-type="received"><day>September</day>	<month>27,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>14,</year>	</date><date date-type="accepted"><day>November</day>	<month>17,</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 this paper, the existence and uniqueness of local solutions to the initial and boundary value problem of a class of parabolic system related to the p-Laplacian are studied. The regularization method is used to construct a sequence of approximation solutions, with the help of monotone iteration technique, then we get the existence of solution of a regularized system. By the use of a standard limiting process, the existence of the local solutions of the system is obtained. Finally, the uniqueness of the solution is also proven.
 
</p></abstract><kwd-group><kwd>Existence</kwd><kwd> Uniqueness</kwd><kwd> Evolution</kwd><kwd> P-Laplacian</kwd><kwd> Parabolic System</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The objective of this paper is to study the existence and uniqueness of local solutions to the initial and boundary value problem of the parabolic system</p><disp-formula id="scirp.72060-formula132"><label>(1.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x2.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula133"><label>(1.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x3.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula134"><label>(1.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x4.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x5.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x6.png" xlink:type="simple"/></inline-formula> is a bounded domain with smooth boundary<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x7.png" xlink:type="simple"/></inline-formula>. The conditions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x8.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x9.png" xlink:type="simple"/></inline-formula> will be given later.</p><p>System (1.1) is popular applied in non-Newtonian fluids [<xref ref-type="bibr" rid="scirp.72060-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.72060-ref2">2</xref>] and nonlinear filtration [<xref ref-type="bibr" rid="scirp.72060-ref3">3</xref>] , etc. In the non-Newtonian fluids theory, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x10.png" xlink:type="simple"/></inline-formula>are all characteristic quantity of the medium. Media with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x11.png" xlink:type="simple"/></inline-formula> are called dilatant fluids and those with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x12.png" xlink:type="simple"/></inline-formula> are called pseudoplastics. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x13.png" xlink:type="simple"/></inline-formula>, they are Newtonian fluids.</p><p>Some authors have studied the global finiteness of the solutions (see [<xref ref-type="bibr" rid="scirp.72060-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.72060-ref5">5</xref>] ) and blow-up properties of the solutions (see [<xref ref-type="bibr" rid="scirp.72060-ref6">6</xref>] ) with various boundary conditions to the systems of evolutionary Laplacian equations. Zhao [<xref ref-type="bibr" rid="scirp.72060-ref7">7</xref>] and Wei-Gao [<xref ref-type="bibr" rid="scirp.72060-ref8">8</xref>] studied the existence and blow-up property of the solutions to a single equation and the systems of two equations. We found that the method of [<xref ref-type="bibr" rid="scirp.72060-ref8">8</xref>] can be extended to the general systems of n equations. For the sake of simplicity, this paper only makes a detailed discussion on n = 3. Since the system is coupled with nonlinear terms, it is in general difficult to study the system. In this paper, we consider some special cases by stating some methods of regularization to construct a sequence of approximation solutions with the help of monotone iteration technique and obtain the existence of solutions to a regularized system of equations. Then we obtain the existence of solutions to the system (1.1)-(1.3) by a standard limiting process. Systems (1.1) degenerates when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x14.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x15.png" xlink:type="simple"/></inline-formula>. In general, there would be no classical solutions and hence we have to study the generalized solutions to the problem (1.1)-(1.3).</p><p>The definition of generalized solutions in this work is the following.</p><p>Definition 1.1. Function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x16.png" xlink:type="simple"/></inline-formula> is called a generalized solution of the system (1.1)-(1.3) if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x17.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x18.png" xlink:type="simple"/></inline-formula>and satisfies</p><disp-formula id="scirp.72060-formula135"><label>(1.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x19.png"  xlink:type="simple"/></disp-formula><p>for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x20.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x21.png" xlink:type="simple"/></inline-formula></p><p>Equations (4) implies that</p><disp-formula id="scirp.72060-formula136"><label>(1.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x22.png"  xlink:type="simple"/></disp-formula><p>The followings are the constrains to the nonlinear functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x23.png" xlink:type="simple"/></inline-formula> involved in this paper.</p><p>Definition 1.2. A function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x24.png" xlink:type="simple"/></inline-formula> is said to be quasimonotone nondecreasing (resp., nonincreasing) if for fixed<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x25.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x26.png" xlink:type="simple"/></inline-formula>is nondecreasing (resp., non- increasing) in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x27.png" xlink:type="simple"/></inline-formula></p><p>Our main existence result is following:</p><p>Theorem 1.3. If there exist nonnegative functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x28.png" xlink:type="simple"/></inline-formula> which are quasimonotonically nondecreasing for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x29.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x30.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x31.png" xlink:type="simple"/></inline-formula>, and a non- negative function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x32.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72060-formula137"><label>(1.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x33.png"  xlink:type="simple"/></disp-formula><p>Then there exists a constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x34.png" xlink:type="simple"/></inline-formula> such that the system (1.1)-(1.3) has a solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x35.png" xlink:type="simple"/></inline-formula> in the sence of Definition 1.1 with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x36.png" xlink:type="simple"/></inline-formula> replaced by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x37.png" xlink:type="simple"/></inline-formula>.</p><p>In Theorem 1.3, we just obtain the existence of local solution. As known to all, when the system degenerates into an equation, as long as some order of growth conditions is added on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x38.png" xlink:type="simple"/></inline-formula>, we can find the global solution, which is the main result of [<xref ref-type="bibr" rid="scirp.72060-ref7">7</xref>] . The existence of the global solution of (1.1)-(1.3) remains to be further studied.</p><p>On the other hand, similar to [<xref ref-type="bibr" rid="scirp.72060-ref8">8</xref>] , we made the assumption of monotonicity to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x39.png" xlink:type="simple"/></inline-formula>. From the current point of view, the condition is relatively strong. It is well worth studying how to reduce <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x40.png" xlink:type="simple"/></inline-formula> monotonicity requirements of the system (1.1)-(1.3).</p></sec><sec id="s2"><title>2. Proof of Theorem 1.3</title><p>To prove the theorem, we consider the following regularized problem</p><disp-formula id="scirp.72060-formula138"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula139"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula140"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x43.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x44.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x45.png" xlink:type="simple"/></inline-formula>are quasimonotone nondecreasing and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x46.png" xlink:type="simple"/></inline-formula> uniformly on bounded subsets of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x47.png" xlink:type="simple"/></inline-formula> also</p><disp-formula id="scirp.72060-formula141"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x48.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x49.png" xlink:type="simple"/></inline-formula>strongly in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x50.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 2.1. The regularized problem (2.1)-(2.3) has a generalized solution.</p><p>Proof. Starting from a suitable initial iteration<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x51.png" xlink:type="simple"/></inline-formula>, we construct a se- quence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x52.png" xlink:type="simple"/></inline-formula> from the iteration process</p><disp-formula id="scirp.72060-formula142"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula143"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula144"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x55.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x56.png" xlink:type="simple"/></inline-formula>. It is clear that for each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x57.png" xlink:type="simple"/></inline-formula> the above system consists of three nondegenerated and uncoupled initial boundary-value problems.</p><p>By classical results (see [<xref ref-type="bibr" rid="scirp.72060-ref9">9</xref>] ) for fixed <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x58.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x59.png" xlink:type="simple"/></inline-formula> the problem (2.5)-(2.7) has a classical solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x60.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x61.png" xlink:type="simple"/></inline-formula> is smooth.</p><p>To ensure that this sequence converges to a solution of (2.1)-(2.3), it is necessary to choose a suitable initial iteration. The choice of this function depends on the type of quasimonotone property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x62.png" xlink:type="simple"/></inline-formula>. In the following, we establish the monotone property of the sequence.</p><p>Set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x63.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x64.png" xlink:type="simple"/></inline-formula> be a classical solution of the following problem.</p><disp-formula id="scirp.72060-formula145"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x65.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula146"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x66.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula147"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x67.png"  xlink:type="simple"/></disp-formula><p>By <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x68.png" xlink:type="simple"/></inline-formula> and the comparison theorem (see [<xref ref-type="bibr" rid="scirp.72060-ref10">10</xref>] ), we have that</p><disp-formula id="scirp.72060-formula148"><label>(2.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x69.png"  xlink:type="simple"/></disp-formula><p>Hence by the quasimonotone nondecreasing property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x70.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72060-formula149"><label>(2.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x71.png"  xlink:type="simple"/></disp-formula><p>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x72.png" xlink:type="simple"/></inline-formula>.</p><p>Using the same argument as above, we can obtain a classical solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x73.png" xlink:type="simple"/></inline-formula> of the problem</p><disp-formula id="scirp.72060-formula150"><label>(2.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula151"><label>(2.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula152"><label>(2.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x76.png"  xlink:type="simple"/></disp-formula><p>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x77.png" xlink:type="simple"/></inline-formula>.</p><p>By the comparison theorem, we have</p><disp-formula id="scirp.72060-formula153"><label>(2.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x78.png"  xlink:type="simple"/></disp-formula><p>By induction method, we obtain a nonincreasing sequence of smooth functions</p><disp-formula id="scirp.72060-formula154"><label>(2.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x79.png"  xlink:type="simple"/></disp-formula><p>In a similar way, by setting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x80.png" xlink:type="simple"/></inline-formula> we can get a solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x81.png" xlink:type="simple"/></inline-formula> of</p><disp-formula id="scirp.72060-formula155"><label>(2.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x82.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula156"><label>(2.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x83.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula157"><label>(2.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x84.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.72060-formula158"><label>(2.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x85.png"  xlink:type="simple"/></disp-formula><p>In the same way as above, we obtain a nondecreasing sequence of smooth functions</p><disp-formula id="scirp.72060-formula159"><label>(2.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x86.png"  xlink:type="simple"/></disp-formula><p>It is obvious that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x87.png" xlink:type="simple"/></inline-formula>. By induction method, we may assume that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x88.png" xlink:type="simple"/></inline-formula>. Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x89.png" xlink:type="simple"/></inline-formula> is quasimonotone nondecreasing, we have</p><disp-formula id="scirp.72060-formula160"><label>(2.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x90.png"  xlink:type="simple"/></disp-formula><p>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x91.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.72060-formula161"><label>(2.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula162"><label>(2.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x93.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula163"><label>(2.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x94.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula164"><label>(2.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x95.png"  xlink:type="simple"/></disp-formula><p>By the comparison principle, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x96.png" xlink:type="simple"/></inline-formula>. Therefore</p><disp-formula id="scirp.72060-formula165"><label>(2.28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x97.png"  xlink:type="simple"/></disp-formula><p>Taking<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x98.png" xlink:type="simple"/></inline-formula>, we get a nondecreasing bounded sequence</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x99.png" xlink:type="simple"/></inline-formula>. Hence there exist functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x100.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72060-formula166"><label>(2.29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x101.png"  xlink:type="simple"/></disp-formula><p>By the continuity of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x102.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.72060-formula167"><label>(2.30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x103.png"  xlink:type="simple"/></disp-formula><p>We now prove that there exist <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x104.png" xlink:type="simple"/></inline-formula> and a constant M (independent of k and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x105.png" xlink:type="simple"/></inline-formula>) such that for all k, we have</p><disp-formula id="scirp.72060-formula168"><label>(2.31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x106.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x107.png" xlink:type="simple"/></inline-formula> be the solutions of the ordinary differential equations</p><disp-formula id="scirp.72060-formula169"><label>(2.32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x108.png"  xlink:type="simple"/></disp-formula><p>By standard results in [<xref ref-type="bibr" rid="scirp.72060-ref11">11</xref>] , there exist<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x109.png" xlink:type="simple"/></inline-formula>, such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x110.png" xlink:type="simple"/></inline-formula> exists on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x111.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x112.png" xlink:type="simple"/></inline-formula> depends only on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x113.png" xlink:type="simple"/></inline-formula>. By the comparison theorem</p><disp-formula id="scirp.72060-formula170"><label>(2.33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x114.png"  xlink:type="simple"/></disp-formula><p>Setting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x115.png" xlink:type="simple"/></inline-formula>, we obtain (2.31).</p><p>We now claim that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x116.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x117.png" xlink:type="simple"/></inline-formula>, in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x118.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x119.png" xlink:type="simple"/></inline-formula> stands for weak convergence,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x120.png" xlink:type="simple"/></inline-formula>.</p><p>Multiplying (2.5) by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x121.png" xlink:type="simple"/></inline-formula> and integrating over<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x122.png" xlink:type="simple"/></inline-formula>, we obtain that</p><disp-formula id="scirp.72060-formula171"><label>(2.34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x123.png"  xlink:type="simple"/></disp-formula><p>Furthermore</p><disp-formula id="scirp.72060-formula172"><label>(2.35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x124.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula173"><label>(2.36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x125.png"  xlink:type="simple"/></disp-formula><p>By (2.12) and the property of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x126.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.72060-formula174"><label>(2.37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x127.png"  xlink:type="simple"/></disp-formula><p>where C is a constant independent of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x128.png" xlink:type="simple"/></inline-formula> and k.</p><p>Multiplying (2.5) by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x129.png" xlink:type="simple"/></inline-formula> and integrating over<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x130.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72060-formula175"><label>(2.38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x131.png"  xlink:type="simple"/></disp-formula><p>By Cauchy inequality and integrating by parts, we obtain</p><disp-formula id="scirp.72060-formula176"><label>(2.39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x132.png"  xlink:type="simple"/></disp-formula><p>Hence</p><disp-formula id="scirp.72060-formula177"><label>(2.40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x133.png"  xlink:type="simple"/></disp-formula><p>By (2.37) and (2.40), we obtain that there exists a subsequence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x134.png" xlink:type="simple"/></inline-formula> converging weakly in the following sense as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x135.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.72060-formula178"><label>(2.41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x136.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula179"><label>(2.42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x137.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula180"><label>(2.43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x138.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x139.png" xlink:type="simple"/></inline-formula> stands for weak convergence,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x140.png" xlink:type="simple"/></inline-formula>.</p><p>From (2.29), (2.30), (2.37), (2.40) and the uniqueness of the weak limits, we have that, as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x141.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72060-formula181"><label>(2.44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x142.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula182"><label>(2.45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x143.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula183"><label>(2.46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x144.png"  xlink:type="simple"/></disp-formula><p>We now claim that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x145.png" xlink:type="simple"/></inline-formula></p><p>Multiplying (2.5) by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x146.png" xlink:type="simple"/></inline-formula> and integrating over <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x147.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x148.png" xlink:type="simple"/></inline-formula> we get</p><disp-formula id="scirp.72060-formula184"><label>(2.47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x149.png"  xlink:type="simple"/></disp-formula><p>Hence</p><disp-formula id="scirp.72060-formula185"><label>(2.48)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x150.png"  xlink:type="simple"/></disp-formula><p>Since the three terms on the right hand side of the above equality converge to 0 as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x151.png" xlink:type="simple"/></inline-formula>. This yields that</p><disp-formula id="scirp.72060-formula186"><label>(2.49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x152.png"  xlink:type="simple"/></disp-formula><p>On the other hand, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x153.png" xlink:type="simple"/></inline-formula>, we have that</p><disp-formula id="scirp.72060-formula187"><label>(2.50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x154.png"  xlink:type="simple"/></disp-formula><p>Note that</p><disp-formula id="scirp.72060-formula188"><label>(2.51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x155.png"  xlink:type="simple"/></disp-formula><p>Following (2.50) and (2.51), we have</p><disp-formula id="scirp.72060-formula189"><label>(2.52)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x156.png"  xlink:type="simple"/></disp-formula><p>Since</p><disp-formula id="scirp.72060-formula190"><label>(2.53)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x157.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72060-formula191"><label>(2.54)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x158.png"  xlink:type="simple"/></disp-formula><p>by H&#246;lder inequality, we have</p><disp-formula id="scirp.72060-formula192"><label>(2.55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x159.png"  xlink:type="simple"/></disp-formula><p>i.e.,</p><disp-formula id="scirp.72060-formula193"><label>(2.56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x160.png"  xlink:type="simple"/></disp-formula><p>Hence</p><disp-formula id="scirp.72060-formula194"><label>(2.57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x161.png"  xlink:type="simple"/></disp-formula><p>This proves that any weak convergence subsequence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x162.png" xlink:type="simple"/></inline-formula> will have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x163.png" xlink:type="simple"/></inline-formula> as its weak limit and hence by a standard argument, we have that as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x164.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72060-formula195"><label>(2.58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x165.png"  xlink:type="simple"/></disp-formula><p>Combining the above results, we have proved that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x166.png" xlink:type="simple"/></inline-formula> is a generalized solution of (2.1)-(2.3).</p><p>Proof of theorem 1.3.</p><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula> satisfy similar estimates as (2.31), (2.37) and (2.40), combining the property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x168.png" xlink:type="simple"/></inline-formula>, we know that there are functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x169.png" xlink:type="simple"/></inline-formula> (as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x170.png" xlink:type="simple"/></inline-formula>) such that for some subsequence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x171.png" xlink:type="simple"/></inline-formula> denoted again by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x172.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72060-formula196"><label>(2.59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x173.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula197"><label>(2.60)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x174.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula198"><label>(2.61)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x175.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula199"><label>(2.62)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x176.png"  xlink:type="simple"/></disp-formula><p>In a similar way as above, we prove that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x177.png" xlink:type="simple"/></inline-formula></p><p>By a standard limiting process, we obtain that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x178.png" xlink:type="simple"/></inline-formula> satisfies the initial and boundary value conditions and the integrating expression. Thus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x179.png" xlink:type="simple"/></inline-formula> is a generalized solution of (1.1)-(1.3).</p></sec><sec id="s3"><title>3. Uniqueness Result to the Solution of the System</title><p>We now prove the uniqueness result to the solution of the system.</p><p>Theorem 3.1. Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x180.png" xlink:type="simple"/></inline-formula> is Lipschitz continuous in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x181.png" xlink:type="simple"/></inline-formula>, then the solution of (1.1)-(1.3) is unique.</p><p>Proof. Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x182.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x183.png" xlink:type="simple"/></inline-formula> are two solutions of (1.1)- (1.3). Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x184.png" xlink:type="simple"/></inline-formula> then following (1.5),</p><disp-formula id="scirp.72060-formula200"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x185.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72060-formula201"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x186.png"  xlink:type="simple"/></disp-formula><p>By (3.1) subtracting (3.2), we get</p><disp-formula id="scirp.72060-formula202"><label>(3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x187.png"  xlink:type="simple"/></disp-formula><p>By the inequality (3.3) and the Lipschitz condition, a simple calculation shows that</p><disp-formula id="scirp.72060-formula203"><label>(3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-5301191x188.png"  xlink:type="simple"/></disp-formula><p>Setting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x189.png" xlink:type="simple"/></inline-formula>, then (3.4) can be written as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x190.png" xlink:type="simple"/></inline-formula>. Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x191.png" xlink:type="simple"/></inline-formula>, by a standard argument, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x192.png" xlink:type="simple"/></inline-formula>, and hence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-5301191x193.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>Cite this paper</title><p>Ou, Q.T. and Zhan, H.S. (2016) Local Solutions to a Class of Parabolic System Related to the P-Lapla- cian. Advances in Pure Mathematics, 6, 868- 877. http://dx.doi.org/10.4236/apm.2016.612065</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72060-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Astrita, G. and Marrucci, G. (1974) Principles of Non-Newtonian Fluid Mechanics. McGraw-Hill, New York.</mixed-citation></ref><ref id="scirp.72060-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Martinson, L.K. and Pavlov, K.B. (1971) Unsteady Shear Flows of a Conducting Fluid with a Rheological Power Law. Magnitnaya Gidrodinamika, 2, 50-58.</mixed-citation></ref><ref id="scirp.72060-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Esteban, J.R. and Vazquez, J.L. (1982) On the Equation of Turbulent Filteration in One-Dimensional Porous Media. Nonlinear Analysis, 10, 1303-1325. http://dx.doi.org/10.1016/0362-546X(86)90068-4</mixed-citation></ref><ref id="scirp.72060-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Constantin, A., Escher, J. and Yin, Z. (2004) Global Solutions for Quasilinear Parabolic System. Journal of Differential Equations, 197, 73-84. http://dx.doi.org/10.1016/S0022-0396(03)00165-7</mixed-citation></ref><ref id="scirp.72060-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Dichstein, F. and Escobedo, M. (2001) A Maximum Principle for Semilinear Parabolic Systems and Application. Nonlinear Analysis, 45, 825-837.  http://dx.doi.org/10.1016/S0362-546X(99)00419-8</mixed-citation></ref><ref id="scirp.72060-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Pierre, M. and Schmidt, D. (1997) Blowup in Reaction-Diffusion Systems with Dissipation of Mass. SIAM Journal on Mathematical Analysis, 28, 259-269.  http://dx.doi.org/10.1137/S0036141095295437</mixed-citation></ref><ref id="scirp.72060-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, J. (1993) Existence and Nonexistence of Solutions for  . Journal of Mathematical Analysis and Applications, 172, 130-146. http://dx.doi.org/10.1006/jmaa.1993.1012</mixed-citation></ref><ref id="scirp.72060-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Wei, Y. and Gao, W. (2007) Existence and Uniqueness of Local Solutions to a Class of Quasilinear Degenerate Parabolic Systems. Applied Mathematics and Computation, 190, 1250-1257. http://dx.doi.org/10.1016/j.amc.2007.02.007</mixed-citation></ref><ref id="scirp.72060-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Ladyzenskaja, O.A., Solonnikov, V.A. and Ural’ceva, N.N. (1968) Linear and Quasilinear Equations of Parabolic Type. American Mathematical Society, Providence, RI.</mixed-citation></ref><ref id="scirp.72060-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Friedman, A. (1964) Partial Differential Equations of Parabilic Type. Prentice-Hall Inc., Englewood Cliffs, NJ.</mixed-citation></ref><ref id="scirp.72060-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Coddingtin, E. and Levinson, N. (1955) Theory of Ordinary Differential Equations. McGraw-Hill, New York.</mixed-citation></ref></ref-list></back></article>