<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.717173</article-id><article-id pub-id-type="publisher-id">AM-72160</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>
 
 
  Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Anna</surname><given-names>Harris</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>Stephen</surname><given-names>Harris</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Danielle</surname><given-names>Rauls</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics and Computer Science, University of Arkansas at Pine Bluff, Pine Bluff, Arkansas, USA</addr-line></aff><aff id="aff2"><addr-line>US Food and Drug Administration, National Center for Toxicology Research, Jefferson, Arkansas, USA</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>11</month><year>2016</year></pub-date><volume>07</volume><issue>17</issue><fpage>2174</fpage><lpage>2182</lpage><history><date date-type="received"><day>September</day>	<month>20,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>19,</year>	</date><date date-type="accepted"><day>November</day>	<month>22,</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>
 
 
  The superconvergence in the finite element method is a phenomenon in which the fi-nite element approximation converges to the exact solution at a rate higher than the optimal order error estimate. Wang proposed and analyzed superconvergence of the conforming finite element method by L2-projections. However, since the conforming finite element method (CFEM) requires a strong continuity, it is not easy to construct such finite elements for the complex partial differential equations. Thus, the nonconforming finite element method (NCFEM) is more appealing computationally due to better stability and flexibility properties compared to CFEM. The objective of this paper is to establish a general superconvergence result for the nonconforming finite element approximations for second-order elliptic problems by L2-projection methods by applying the idea presented in Wang. MATLAB codes are published at https://github.com/annaleeharris/Superconvergence-NCFEM for anyone to use and to study. The results of numerical experiments show great promise for the robustness, reliability, flexibility and accuracy of superconvergence in NCFEM by L2- projections.
 
</p></abstract><kwd-group><kwd>Nonconforming Finite Element Methods</kwd><kwd> Superconvergence</kwd><kwd> L2-Projection</kwd><kwd> Second-Order Elliptic Equation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The conforming finite element method (CFEM) requires a strong continuity; hence it is</p><p>not easy to construct such finite elements for the complex partial differential equations. The nonconforming finite element method (NCFEM) is more appealing computationally due to better stability and flexibility properties compared to CFEM [<xref ref-type="bibr" rid="scirp.72160-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.72160-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.72160-ref3">3</xref>] . The superconvergence in the finite element method is a phenomenon in which the finite element approximation converges to the exact solution at a rate higher than the optimal order error estimate. Wang proposed and analyzed superconvergence of the conforming finite element method by L<sup>2</sup>-projections. The main idea behind the L<sup>2</sup>-projections is to project the finite element solution to another finite element space with a coarse mesh and a higher order of polynomials.</p><p>The objective of this paper is to establish a general superconvergence result for the nonconforming finite element approximations for second-order elliptic problems by L<sup>2</sup>-projection methods by applying the idea presented in Wang [<xref ref-type="bibr" rid="scirp.72160-ref4">4</xref>] .</p><p>This paper is organized as follows. In Section 2, we present a review for the non- conforming finite element method for the second-order elliptic problem. In Section 3, we develop a general theory of superconvergence by following the idea presented in Wang [<xref ref-type="bibr" rid="scirp.72160-ref4">4</xref>] . In Section 4, we perform numerical experiments to support the theoretical results. Numerical experiements of superconvergence of NCFEM are performed in MATLAB and its codes are posted at https://github.com/annaleeharris/Superconvergence-NCFEM for anyone to use and to study.</p></sec><sec id="s2"><title>2. NCFEM for the Second-Order Elliptic Problem</title><p>Consider the second-order elliptic problem with the Dirichlet boundary condition which seeks <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x2.png" xlink:type="simple"/></inline-formula> satisfying</p><disp-formula id="scirp.72160-formula134"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x3.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x4.png" xlink:type="simple"/></inline-formula> is the Laplacian operator, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x5.png" xlink:type="simple"/></inline-formula>is a bounded, connected, and open subset of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x6.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x7.png" xlink:type="simple"/></inline-formula>is a Lipschitz continuous boundary, and a given function f is the external force.</p><p>A variational formulation of (1) seeks <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x8.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72160-formula135"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x9.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72160-formula136"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x10.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x11.png" xlink:type="simple"/></inline-formula> be a quasi-uniform, i.e., it is regular and satisfies the inverse assumption [<xref ref-type="bibr" rid="scirp.72160-ref5">5</xref>] , triangulation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x12.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x13.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x14.png" xlink:type="simple"/></inline-formula> be the space of poly- nomials of degree at most k with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x15.png" xlink:type="simple"/></inline-formula> on K. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x16.png" xlink:type="simple"/></inline-formula> denote the union of the boun- daries of all elements <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x17.png" xlink:type="simple"/></inline-formula> and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x18.png" xlink:type="simple"/></inline-formula> be the collection of all interior edges. Assume that the polynomial space in the construction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x19.png" xlink:type="simple"/></inline-formula> contains <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x20.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x21.png" xlink:type="simple"/></inline-formula>. Define the finite element space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x22.png" xlink:type="simple"/></inline-formula> associated with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x23.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.72160-formula137"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x24.png"  xlink:type="simple"/></disp-formula><p>The finite element space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x25.png" xlink:type="simple"/></inline-formula> is assumed to satisfy the following approximation pro- perty for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x26.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.72160-ref6">6</xref>] :</p><disp-formula id="scirp.72160-formula138"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x27.png"  xlink:type="simple"/></disp-formula><p>The nonconforming finite element approximation problem (2) seeks <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x28.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72160-formula139"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x29.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72160-formula140"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x30.png"  xlink:type="simple"/></disp-formula><p>A well known error estimate for the finite element approximation solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x31.png" xlink:type="simple"/></inline-formula> is the following [<xref ref-type="bibr" rid="scirp.72160-ref7">7</xref>] :</p><disp-formula id="scirp.72160-formula141"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x32.png"  xlink:type="simple"/></disp-formula><p>where C is a constant independent of the mesh size h.</p><p>To apply the superconvergence of finite element approximation, we assume that domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x33.png" xlink:type="simple"/></inline-formula> is so regular that it ensures a<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x34.png" xlink:type="simple"/></inline-formula>, regularity for the solution of (2). In other words, for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x35.png" xlink:type="simple"/></inline-formula> the problem (2) has a unique solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x36.png" xlink:type="simple"/></inline-formula> satisfying the following a priori estimate</p><disp-formula id="scirp.72160-formula142"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x37.png"  xlink:type="simple"/></disp-formula><p>where C is a constant independent of data f.</p></sec><sec id="s3"><title>3. Superconvergence of NCFEM</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x38.png" xlink:type="simple"/></inline-formula> be another finite element partition with coarse mesh size <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x39.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x40.png" xlink:type="simple"/></inline-formula>. Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x41.png" xlink:type="simple"/></inline-formula> and h have the following relation:</p><disp-formula id="scirp.72160-formula143"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x42.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula> be any finite element space consisting of piecewise polynomial of degree r associated with the partition<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x44.png" xlink:type="simple"/></inline-formula>. Define <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x45.png" xlink:type="simple"/></inline-formula> to be the L<sup>2</sup>-projection from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x46.png" xlink:type="simple"/></inline-formula> onto the finite element space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x47.png" xlink:type="simple"/></inline-formula>. The finite element space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x48.png" xlink:type="simple"/></inline-formula> is defined as follows:</p><disp-formula id="scirp.72160-formula144"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x49.png"  xlink:type="simple"/></disp-formula><p>The following lemma will provide an error estimate for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x50.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 1 Assume that the second-order elliptic problem (2) holds (5) with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x51.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x52.png" xlink:type="simple"/></inline-formula>. Then there exists a constant C independent of h and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x53.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72160-formula145"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x54.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x55.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x56.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. Using the definition of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x57.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x58.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72160-formula146"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x59.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72160-formula147"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x60.png"  xlink:type="simple"/></disp-formula><p>Then</p><disp-formula id="scirp.72160-formula148"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x61.png"  xlink:type="simple"/></disp-formula><p>Consider the following problem:</p><disp-formula id="scirp.72160-formula149"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x62.png"  xlink:type="simple"/></disp-formula><p>Multiplying the second-order elliptic Equation (1) by v and integrating it over <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x63.png" xlink:type="simple"/></inline-formula> give</p><disp-formula id="scirp.72160-formula150"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x64.png"  xlink:type="simple"/></disp-formula><p>where n is the unit outward normal.</p><p>Subtract (3) from the above Equation (10) gives</p><disp-formula id="scirp.72160-formula151"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x65.png"  xlink:type="simple"/></disp-formula><p>Multiplying (9) by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x66.png" xlink:type="simple"/></inline-formula>, integrating it over<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x67.png" xlink:type="simple"/></inline-formula>, adding and subtracting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x68.png" xlink:type="simple"/></inline-formula>, and using the result (11) we have</p><disp-formula id="scirp.72160-formula152"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x69.png"  xlink:type="simple"/></disp-formula><p>The line integrals of the above equations are approximated in [<xref ref-type="bibr" rid="scirp.72160-ref6">6</xref>] as follows:</p><disp-formula id="scirp.72160-formula153"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x70.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72160-formula154"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x71.png"  xlink:type="simple"/></disp-formula><p>Using the Cauchy-Schwartz inequality, the approximation property (2), and line integral approximations (12) and (13) we have</p><disp-formula id="scirp.72160-formula155"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x72.png"  xlink:type="simple"/></disp-formula><p>Substituting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x73.png" xlink:type="simple"/></inline-formula> as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x74.png" xlink:type="simple"/></inline-formula> by the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x75.png" xlink:type="simple"/></inline-formula> regularity, applying the inverse in- equality to the term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x76.png" xlink:type="simple"/></inline-formula> and using the definition of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x77.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.72160-formula156"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x78.png"  xlink:type="simple"/></disp-formula><p>Combining the above equation with the Equation (8) we have</p><disp-formula id="scirp.72160-formula157"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x79.png"  xlink:type="simple"/></disp-formula><p>which completes the proof of the lemma.</p><p>The following theorem provides an error estimate for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x80.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 1 Assume that (5) holds true with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x82.png" xlink:type="simple"/></inline-formula>. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x83.png" xlink:type="simple"/></inline-formula> is the finite element approximation of the exact solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x84.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x85.png" xlink:type="simple"/></inline-formula> of (2), then there exists a constant C independent of h and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x86.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.72160-formula158"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x87.png"  xlink:type="simple"/></disp-formula><p>Proof. Since we assume the exact solution u is sufficiently smooth and by the de- finitions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x88.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x89.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72160-formula159"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x90.png"  xlink:type="simple"/></disp-formula><p>Using the triangle inequality and combining (16) and Lemma 1 we obtain</p><disp-formula id="scirp.72160-formula160"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x91.png"  xlink:type="simple"/></disp-formula><p>which completes the error estimate of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x92.png" xlink:type="simple"/></inline-formula>.</p><p>Similarly, we estimate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x93.png" xlink:type="simple"/></inline-formula>.</p><p>Using the inverse inequality and the definitions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x94.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x95.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.72160-formula161"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x96.png"  xlink:type="simple"/></disp-formula><p>Using the triangle inequality and combining (17) and Lemma 1 we have</p><disp-formula id="scirp.72160-formula162"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x97.png"  xlink:type="simple"/></disp-formula><p>Hence the theorem has been proved.</p><p>The optimal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x98.png" xlink:type="simple"/></inline-formula> is selected using Theorem 1 for the error estimates:</p><disp-formula id="scirp.72160-formula163"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x99.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72160-formula164"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x100.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Experiments of Superconvergence of NCFEM by L<sup>2</sup>-Projection Methods</title><p>In this section, we present numerical experiments for second-order elliptic problems to support our theoretical results. Assume that the exact solution of the second-order elliptic problem has the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x101.png" xlink:type="simple"/></inline-formula> regularity for some <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x102.png" xlink:type="simple"/></inline-formula> and for simplicity, assume</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x103.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x104.png" xlink:type="simple"/></inline-formula> which gives <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x105.png" xlink:type="simple"/></inline-formula> using the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x106.png" xlink:type="simple"/></inline-formula> formula (18).</p><p>From the theoretical result (15) we have the following optimal error estimates:</p><disp-formula id="scirp.72160-formula165"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x107.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72160-formula166"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/8-7403381x108.png"  xlink:type="simple"/></disp-formula><p>From the results (19) and (20), theoretically, in L<sup>2</sup> norm the L<sup>2</sup>-projection to the existing numerical approximation does not improve the convergence rate but in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x109.png" xlink:type="simple"/></inline-formula> norm the L<sup>2</sup>-projection to the existing numerical solution provides some superconver- gence.</p><p>The finite element partition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula> is constructed by dividing the domain into an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula> rectangular mesh then dividing the rectangular mesh with the positive slope to form two triangles. The coarse finite element partition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula> is also constructed by dividing the domain into an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula> rectangular mesh then dividing the rectangular mesh with the positive slope to form two triangles. The finite element space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula> con- sists of the space of the linear polynomials <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula> associated with the partition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula> and the dual finite element space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x117.png" xlink:type="simple"/></inline-formula> consists of the space of the quadratic polynomials <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x118.png" xlink:type="simple"/></inline-formula> associated with the partition<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x119.png" xlink:type="simple"/></inline-formula>. The finite element spaces <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x120.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x121.png" xlink:type="simple"/></inline-formula> are defined as follows:</p><disp-formula id="scirp.72160-formula167"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x122.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72160-formula168"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x123.png"  xlink:type="simple"/></disp-formula><p>The numerical approximation is refined as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x124.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x125.png" xlink:type="simple"/></inline-formula>. The length of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x126.png" xlink:type="simple"/></inline-formula> and each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x127.png" xlink:type="simple"/></inline-formula> element contains <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x128.png" xlink:type="simple"/></inline-formula> elements.</p><p>Using the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x129.png" xlink:type="simple"/></inline-formula> Equation (18) and our choice of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x130.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x131.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.72160-formula169"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x132.png"  xlink:type="simple"/></disp-formula><p>Using the difference in mesh size and a higher degree of polynomials we shall produce some superconvergence of NCFEM for the second-order elliptic problems.</p><p>Example 1. Let the domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x133.png" xlink:type="simple"/></inline-formula> and the exact solution is assumed to be as follows:</p><disp-formula id="scirp.72160-formula170"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x134.png"  xlink:type="simple"/></disp-formula><p>From <xref ref-type="table" rid="table1">Table 1</xref> we observe that the L<sup>2</sup>-projection to the existing numerical approxi- mation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula> reduced the error estimates in L<sup>2</sup> norm and in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula> norm. In L<sup>2</sup> norm the convergence rate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula> is similar to the convergence rate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula> which is the same as the theoretical result (19). The convergence rate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x139.png" xlink:type="simple"/></inline-formula> is about 33% faster than the convergence rate of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x140.png" xlink:type="simple"/></inline-formula> in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x141.png" xlink:type="simple"/></inline-formula> norm (see <xref ref-type="fig" rid="fig2">Figure 2</xref>). The surface plots of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x142.png" xlink:type="simple"/></inline-formula> in coarse meshes and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x143.png" xlink:type="simple"/></inline-formula> in fine meshes are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The numerical example 1 clearly supports the theoretical result and confirms the super- convergence of NCFEM for the second-order elliptic problem.</p><p>Example 2. Let the domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x144.png" xlink:type="simple"/></inline-formula> and let the analytical solution be given as</p><disp-formula id="scirp.72160-formula171"><graphic  xlink:href="http://html.scirp.org/file/8-7403381x145.png"  xlink:type="simple"/></disp-formula><p>From <xref ref-type="table" rid="table2">Table 2</xref>, we can see that the numerical example 2 supports the theoretical result (15). See <xref ref-type="fig" rid="fig3">Figure 3</xref>, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x146.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x147.png" xlink:type="simple"/></inline-formula>, we can project 3<sup>2</sup> fine triangle elements onto one coarse triangle element. Thus, as n increases, we can project <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x148.png" xlink:type="simple"/></inline-formula> more fine triangle elements to one coarse triangle element in which the process of refining elements produces better error estimates. The L<sup>2</sup>-projection to the existing numerical approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x149.png" xlink:type="simple"/></inline-formula> produced some superconvergence in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x150.png" xlink:type="simple"/></inline-formula> norm and did not affect the convergence rate in L<sup>2</sup> norm (see <xref ref-type="fig" rid="fig4">Figure 4</xref>). The numerical example 2 also</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Numerical error approximation results using NCFEM in Example 1,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x151.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" >iter</th><th align="center" valign="middle" >h</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x152.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x153.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x154.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x155.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2<sup>−3</sup></td><td align="center" valign="middle" >0.1388e−1</td><td align="center" valign="middle" >0.3909e−3</td><td align="center" valign="middle" >0.8184e−2</td><td align="center" valign="middle" >0.3920e−3</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3<sup>−3</sup></td><td align="center" valign="middle" >0.4138e−2</td><td align="center" valign="middle" >0.3443e−4</td><td align="center" valign="middle" >0.1635e−2</td><td align="center" valign="middle" >0.3431e−4</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4<sup>−3</sup></td><td align="center" valign="middle" >0.1747e−2</td><td align="center" valign="middle" >0.6104e−5</td><td align="center" valign="middle" >0.5190e−3</td><td align="center" valign="middle" >0.6104e−5</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >5<sup>−3</sup></td><td align="center" valign="middle" >0.8944e−3</td><td align="center" valign="middle" >0.1600e−5</td><td align="center" valign="middle" >0.2127e−3</td><td align="center" valign="middle" >0.1600e−5</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >6<sup>−3</sup></td><td align="center" valign="middle" >0.5176e−3</td><td align="center" valign="middle" >0.5358e−6</td><td align="center" valign="middle" >0.1026e−3</td><td align="center" valign="middle" >0.5359e−6</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x156.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.9981</td><td align="center" valign="middle" >2.000</td><td align="center" valign="middle" >1.3287</td><td align="center" valign="middle" >2.0010</td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Surface plots of approximation using NCFEM in Example 1,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula>. (L): Surface plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x160.png" xlink:type="simple"/></inline-formula>. (M): Surface of plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x161.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x162.png" xlink:type="simple"/></inline-formula>. (R): Surface plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x163.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x164.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/8-7403381x157.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Error convergence rates using NCFEM in Example 1,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x166.png" xlink:type="simple"/></inline-formula>. (L): L<sup>2</sup> norm error; (R): <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x167.png" xlink:type="simple"/></inline-formula>norm error</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/8-7403381x165.png"/></fig><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Numerical error approximation results using NCFEM in Example 2, <img data-original="http://html.scirp.org/file/8-7403381x168.png" /></title></caption><table><tbody><thead><tr><th align="center" valign="middle" >iter</th><th align="center" valign="middle" >h</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x169.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x170.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x171.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x172.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2<sup>−3</sup></td><td align="center" valign="middle" >0.3933e−1</td><td align="center" valign="middle" >0.8429e−3</td><td align="center" valign="middle" >0.2214e−1</td><td align="center" valign="middle" >0.8453e−3</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3<sup>−3</sup></td><td align="center" valign="middle" >0.1189e−1</td><td align="center" valign="middle" >0.7404e−4</td><td align="center" valign="middle" >0.4387e−2</td><td align="center" valign="middle" >0.7408e−4</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4<sup>−3</sup></td><td align="center" valign="middle" >0.5019e−2</td><td align="center" valign="middle" >0.1317e−4</td><td align="center" valign="middle" >0.1392e−2</td><td align="center" valign="middle" >0.1318e−4</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >5<sup>−3</sup></td><td align="center" valign="middle" >0.2570e−2</td><td align="center" valign="middle" >0.3454e−5</td><td align="center" valign="middle" >0.5708e−3</td><td align="center" valign="middle" >0.3455e−5</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >6<sup>−3</sup></td><td align="center" valign="middle" >0.1487e−2</td><td align="center" valign="middle" >0.1156e−5</td><td align="center" valign="middle" >0.2754e−3</td><td align="center" valign="middle" >0.1157e−5</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x173.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.9983</td><td align="center" valign="middle" >1.9998</td><td align="center" valign="middle" >1.3311</td><td align="center" valign="middle" >2.0006</td></tr></tbody></table></table-wrap><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Surface plots of approximation using NCFEM in Example 2, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula>(L): Surface plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x177.png" xlink:type="simple"/></inline-formula>. (M): Surface of plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x178.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x179.png" xlink:type="simple"/></inline-formula>. (R): Surface plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x180.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x181.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/8-7403381x174.png"/></fig><p>supports the theoretical result and confirms the superconvergence of NCFEM for the second-order elliptic problem.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The L<sup>2</sup>-projection to the existing numerical approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x182.png" xlink:type="simple"/></inline-formula> produced some super- convergence in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x183.png" xlink:type="simple"/></inline-formula> norm, convergence rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x184.png" xlink:type="simple"/></inline-formula>, but did not affect the convergence</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Error convergence rates using NCFEM in Example 2, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x186.png" xlink:type="simple"/></inline-formula>(L): L<sup>2</sup> norm error; (R): <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/8-7403381x187.png" xlink:type="simple"/></inline-formula>norm error</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/8-7403381x185.png"/></fig><p>rate in L<sup>2</sup> norm. With the numerical experiments we can conclusively support the theoretical result and confirm the superconvergence of NCFEM for second-order elliptic problems by L<sup>2</sup>-projection method.</p></sec><sec id="s6"><title>Acknowledgements</title><p>We thank the Editor and the peer-reviewers for their comments. Research of Anna Harris is funded by the National Science Foundation Historical Black Colleges and Universities Undergraduate Program Research Initiative Award grant (#1505119). This support is greatly appreciated.</p></sec><sec id="s7"><title>Cite this paper</title><p>Harris, A., Harris, S. and Rauls, D. (2016) Numerical Experiments Using MATLAB: Superconvergence of Nonconforming Finite Element Approximation for Second-Order Elliptic Problems. Applied Mathematics, 7, 2174-2182. http://dx.doi.org/10.4236/am.2016.717173</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72160-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Croouzeix, M. and Raviart, P.A. (1973) Conforming and Nonconforming Finite Element Methods for Solving the Stationary Stokes Equations. R.A.I.R.O. R, 3, 33-76.</mixed-citation></ref><ref id="scirp.72160-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Douglas Jr, J., Santos, J.E., Sheen, D. and Ye, X. (1999) Nonconforming Galerkin Methods Based on Quadrilateral Elements for Second Order Elliptic Problems. Mathematical Modelling and Numerical Analysis, 33, 747-770. https:/doi.org/10.1051/m2an:1999161</mixed-citation></ref><ref id="scirp.72160-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Girault, V. and Raviart, P.A. 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