<?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">ENG</journal-id><journal-title-group><journal-title>Engineering</journal-title></journal-title-group><issn pub-type="epub">1947-3931</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/eng.2017.95031</article-id><article-id pub-id-type="publisher-id">ENG-76655</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  On the Relation of Grain Orientation and Opening Crack of an Al-Cu-Mg Sheet
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Cai</surname><given-names>Hu</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Light Alloy Research Institute, Central South University, Changsha, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>27</day><month>05</month><year>2017</year></pub-date><volume>09</volume><issue>05</issue><fpage>510</fpage><lpage>516</lpage><history><date date-type="received"><day>May</day>	<month>4,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>May</month>	<year>28,</year>	</date><date date-type="accepted"><day>May</day>	<month>31,</month>	<year>2017</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 orientation of grains which adjacent to a developed opening crack was investigated by EBSD. A definition of 
  <em>θ</em> has been came up with which represents the angle between the principal stress plane and each plane of the grains. Smaller 
  <em>θ</em> means easier to crack. It gave a good explanation of the crack propagation throughout the grains. It also revealed that propagation path is along with the plane. This finding will give a prediction of tear properties and help us understanding the cracking mechanism and the behavior of tearing.
 
</p></abstract><kwd-group><kwd>Al-Cu-Mg Sheet</kwd><kwd> Tearing Crack</kwd><kwd> Grain Orientation</kwd><kwd> Plane</kwd><kwd> Crack  Propagation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>High strength and high toughness aluminum alloys such as 2024 is the key materials of aviation industry. It should have good durability while under severe environment. Not only the strength but also fracture toughness plays an important role in application. Not until A.A. Griffith did people realize that the fracture can happen even under a load significantly less than the yield range if the surface is scratched [<xref ref-type="bibr" rid="scirp.76655-ref1">1</xref>] . After that the discipline of fracture mechanism developed quickly [<xref ref-type="bibr" rid="scirp.76655-ref2">2</xref>] . Grain orientation cannot be ignored if we discuss the fracture mechanism. The slip plane is the principal stress plane that can accelerate the cracking process [<xref ref-type="bibr" rid="scirp.76655-ref3">3</xref>] . Large misorientation angle can prevent the dislocation to penetrate so that it leads to more energy consuming and the crack growth rate is negative correlation of misorientation angle [<xref ref-type="bibr" rid="scirp.76655-ref4">4</xref>] . Crack propagation has a huge influent to the evaluation of the fracture toughness. The resistance to the crack propagation is a vital property of materials. Fatigue crack propagation behavior has been studied by lots of researchers [<xref ref-type="bibr" rid="scirp.76655-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref7">7</xref>] . The path of the fatigue crack has something to do with the slip plane of aluminum alloy. Tilt and twist angle is proposed to explain the crystallographic mechanism of crack propagates through the grain boundary [<xref ref-type="bibr" rid="scirp.76655-ref8">8</xref>] . It also can be found in H.C.P. metals that the deformation mechanism of dislocation slips [<xref ref-type="bibr" rid="scirp.76655-ref9">9</xref>] . Texture plays an important role in every kinds of crack. Even the intergranular stress corrosion crack has something to do with the crystallographic texture of the material [<xref ref-type="bibr" rid="scirp.76655-ref10">10</xref>] . Not only experiment but also simulation certified the theory that crack follows <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x5.png" xlink:type="simple"/></inline-formula> planes in F.C.C. metals [<xref ref-type="bibr" rid="scirp.76655-ref11">11</xref>] . Since its stress state differs from that of fatigue crack propagation, the propagation behavior of tearing differs from that of fatigue. In this paper, tear crack propagation inside the grain is focused to investigate the influence of grain orientation on the crack propagation and corresponding mechanism. For this purpose, EBSD is a useful method that can be observed both in one picture [<xref ref-type="bibr" rid="scirp.76655-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.76655-ref16">16</xref>] . If a specimen with a tear crack tip observed in EBSD, the relation between grain orientation and the crack propagation path will be found. In this work, we torn an aluminum sheet and observed grain orientations adjacent to an opening crack by EBSD. The close relationship of crack propagation path and the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x6.png" xlink:type="simple"/></inline-formula> planes was revealed.</p></sec><sec id="s2"><title>2. Materials and Experiments</title><p>A notched 2024-T39 aluminum sheet with a thickness of 0.3 mm was torn, which polished by 180#, 320#, 600#, 800#, 1000#, 1200#, 1500# rough sand paper and 800#, 1000# fine sand paper before tearing. Loading stopped before the crack went edge opposite to the notch. The specimens for tearing are thin enough for tearing it easily, as well as minimize the influence of inner grains that can’t observe. It treated by annealing of 200˚C, 1 h to release the residual stress. Twin-jet electro polishing was conducted before EBSD. EBSD data was acquired in FEI Helios Nanolab 600i with a step length of 6 μm.</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>In order to measure how the orientation influence the crack propagation, the Euler angles and the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x7.png" xlink:type="simple"/></inline-formula> pole figures of the related grains A, B, C, D, and E were showed in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The EBSD patterns were analyzed by OIM software. IPF map was automatic generation. And the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x8.png" xlink:type="simple"/></inline-formula> pole figures were calculated from Euler angles of each grains and generated also from OIM. The crack came from the grain boundary of grain A and C, then came across the grain D. Obviously the way of the crack changed the direction and reached grain B. It has a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x9.png" xlink:type="simple"/></inline-formula> direction that close to the transverse direction, which makes it vulnerable to the crack along the rolling direction. The crack doesn’t get through grain D. As crack reached the grain E, it stopped eventually. As showed in <xref ref-type="fig" rid="fig1">Figure 1</xref> E, whose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x10.png" xlink:type="simple"/></inline-formula> direction is far from the TD, the crack was arrested.</p><p>The crack resistance can be identified quantitatively by calculating the angle between all symmetrically equivalent <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x11.png" xlink:type="simple"/></inline-formula> plane and the principal stress plane. It’s all known that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x12.png" xlink:type="simple"/></inline-formula> has 8 corresponding plane of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x14.png" xlink:type="simple"/></inline-formula>,</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> EBSD map of crack propagation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8102819x15.png"/></fig><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x16.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x17.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x18.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula>. All of them are taken into consideration. The principal stress plane denoted as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula> of the sample reference which is perpendicular to TD. Orientation matrixes were used in order to change the sample coordinate system to the crystal coordinate system. Here given a definition: θ, represent the angle between principal stress plane <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x23.png" xlink:type="simple"/></inline-formula> and each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x24.png" xlink:type="simple"/></inline-formula> plane. Then every θ can be calculated. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the definition of θ. A principal stress plane (blue line) cut through a cubic crystal (black line). Red line shows each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x25.png" xlink:type="simple"/></inline-formula> plane of this crystal. The cross line of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x26.png" xlink:type="simple"/></inline-formula> plane and principal stress plane are in purple. The angle between the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x27.png" xlink:type="simple"/></inline-formula> plane and principal stress plane called θ.</p><p>The θ of each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula> plane in every related grain are shown in the <xref ref-type="table" rid="table1">Table 1</xref>. The θ larger than 90 degrees is equivalent as its counterpart of the number whose sum is 180 degrees. The 8 <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x29.png" xlink:type="simple"/></inline-formula> planes can be simplified into 4:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x30.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x31.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x32.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x33.png" xlink:type="simple"/></inline-formula>.</p><p>It can be seen that the grain B has minor θ of 37.10 degrees compared to the 40.56 of the neighbor grain D. High angle of θ prevented the grains from being cut though by crack. It also can inhibit the crack propagation. The calculating of θ successfully revealed that the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x34.png" xlink:type="simple"/></inline-formula> plane is easy to crack (<xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>By testing the grains orientation, resistance level of crack propagation can be</p><p>estimated. Furthermore, when using the appropriate processing method to change the grains orientation, tear properties as well as fracture toughness can be improved.</p><p>If only the crack is along <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula> plane, the path of the crack observed by us will be the intersection line of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula> plane and the sheet plane in grain B. <xref ref-type="fig" rid="fig3">Figure 3</xref> also shows the intersection lines (red lines) of 4 <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula> plane and the sheet plane in grain B. the crack path match the intersection line of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x40.png" xlink:type="simple"/></inline-formula>plane obviously. This map clearly demonstrates the crack propagation along the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x41.png" xlink:type="simple"/></inline-formula> first then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x42.png" xlink:type="simple"/></inline-formula> finally <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x43.png" xlink:type="simple"/></inline-formula> plane in grain B. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x44.png" xlink:type="simple"/></inline-formula>is not cracked due to its large θ (72.94 in <xref ref-type="table" rid="table1">Table 1</xref>).</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Definition of θ</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8102819x45.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Intersection lines of the 4 <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x47.png" xlink:type="simple"/></inline-formula> planes and the sheet plane in grain B</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8102819x46.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> θ of each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x48.png" xlink:type="simple"/></inline-formula> plane</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="3"  >Euler angles</th><th align="center" valign="middle" >Miller indices</th><th align="center" valign="middle"  colspan="4"  >θ (Angle between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x49.png" xlink:type="simple"/></inline-formula> plane and the principal stress plane)</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x50.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x51.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x52.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x53.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >111</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x55.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x56.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x57.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >Grain A</td><td align="center" valign="middle" >289.140</td><td align="center" valign="middle" >38.773</td><td align="center" valign="middle" >70.21</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x58.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >66.49</td><td align="center" valign="middle" >43.32</td><td align="center" valign="middle" >50.51</td><td align="center" valign="middle" >60.63</td></tr><tr><td align="center" valign="middle" >Grain B</td><td align="center" valign="middle" >102.842</td><td align="center" valign="middle" >39.348</td><td align="center" valign="middle" >277.39</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x60.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >62.87</td><td align="center" valign="middle" >50.59</td><td align="center" valign="middle" >37.10</td><td align="center" valign="middle" >72.94</td></tr><tr><td align="center" valign="middle" >Grain C</td><td align="center" valign="middle" >49.646</td><td align="center" valign="middle" >27.581</td><td align="center" valign="middle" >294.75</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x62.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >61.19</td><td align="center" valign="middle" >53.51</td><td align="center" valign="middle" >75.61</td><td align="center" valign="middle" >34.10</td></tr><tr><td align="center" valign="middle" >Grain D</td><td align="center" valign="middle" >143.167</td><td align="center" valign="middle" >23.512</td><td align="center" valign="middle" >221.12</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x64.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >61.08</td><td align="center" valign="middle" >69.27</td><td align="center" valign="middle" >50.94</td><td align="center" valign="middle" >40.56</td></tr><tr><td align="center" valign="middle" >Grain E</td><td align="center" valign="middle" >330.275</td><td align="center" valign="middle" >11.894</td><td align="center" valign="middle" >26.38</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x66.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >44.88</td><td align="center" valign="middle" >59.87</td><td align="center" valign="middle" >50.84</td><td align="center" valign="middle" >64.86</td></tr></tbody></table></table-wrap><p>It’s all know that the close-packed plane of f.c.c. metal is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula>. This atom arrangement has great influence in behavior of materials which leads to anisotropic of a crystal. As a consequence, a crystal can be torn easier apart by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x69.png" xlink:type="simple"/></inline-formula> than other directions because the connection of grains in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x70.png" xlink:type="simple"/></inline-formula> plane is the closest and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x71.png" xlink:type="simple"/></inline-formula> directions have the least bonding energy. The interatomic forces between atoms must be overcome in order to tear the two atom plane. The more distant of two atom plane, the more energy will be consumed. It can be seen in grain B, the crack change their routes into another direction even though inside the grain. But it still along intersecting lines of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x72.png" xlink:type="simple"/></inline-formula> plane and the sample surface. This phenomenon may attribute to independent critical stress of different direction, which is identified by molecular dynamics simulation within a single crystal [<xref ref-type="bibr" rid="scirp.76655-ref17">17</xref>] . Slip occurs in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x73.png" xlink:type="simple"/></inline-formula> plane first and soon apart from each other.</p><p>It can be inferred from above, when crack come across the grain boundary and the orientation of the grain in front of the crack tip is different; the crack propagation will also be different. As is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, when the crack direction differs widely from the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x74.png" xlink:type="simple"/></inline-formula> plane through grains, the crack propagation may change the direction to the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x75.png" xlink:type="simple"/></inline-formula> plane, because the fracture in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x76.png" xlink:type="simple"/></inline-formula> plane is easier than others. When the crack enters another misaligned grain, direction changing continues. That also leads to the crack behaving not a straight line. The curved crack increased the surface of the cracking plane. During this procedure, more energy would be consumed due to the extra surface where dislocation cut through extra particles.</p><p>The θ of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x77.png" xlink:type="simple"/></inline-formula> plane provides a good prediction of crack propagation path. By testing the grains orientation, resistance level of crack propagation can be estimated. Each θ can be considered as an energy barrier. Crack propagation always prefers the way with less energy consumption. So turning of a crack direction may occur in order to choose an easier way. If a material has a lot of high θ<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x78.png" xlink:type="simple"/></inline-formula>planes, the resistance from cracking is strong. Furthermore, when using the appropriate processing method to change the grains orientation, tear properties as well as fracture toughness can be improved. This finding is based on the tearing crack of 2024 aluminum alloy, but it can be applied to other aluminum alloy, other f.c.c metal even other materials.</p></sec><sec id="s4"><title>4. Conclusion</title><p>A definition of θ explained the crack propagation path of tearing, which has a lot</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Crack propagation through grains with different orientation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-8102819x79.png"/></fig><p>to do with the grain orientation. If a grain’s <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x80.png" xlink:type="simple"/></inline-formula> plane paralleled to the principal stress plane, it’s easy to become the path of the crack. On the other hand, if all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x81.png" xlink:type="simple"/></inline-formula> planes diverge the principal stress plane, it’s hard to fracture corresponding with a high θ. Crack follows the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-8102819x82.png" xlink:type="simple"/></inline-formula> plane may due to the highest critical stress. This phenomenon is not only applied inside the grain but also intergranular crack. To go further, the texture with high θ makes the materials tougher.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is supported by the Major State Research Program of China (Project No. 2016YFB0300901) and the Chinese National Science Foundation (Project No. 51375503).</p></sec><sec id="s6"><title>Cite this paper</title><p>Hu, C. (2017) On the Relation of Grain Orientation and Opening Crack of an Al-Cu-Mg Sheet. Engineering, 9, 510-516. https://doi.org/10.4236/eng.2017.95031</p></sec></body><back><ref-list><title>References</title><ref id="scirp.76655-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Griffith, A.A. (1921) The Phenomena of Rupture and Flow in Solids. Philosophical Transactions of the Royal Society of London Series A, Containing Papers of a Mathematical or Physical Character, 221, 163-198.  
https://doi.org/10.1098/rsta.1921.0006</mixed-citation></ref><ref id="scirp.76655-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Fl&amp;uuml;gge, S. (1958) Elasticity and Plasticity/Elastizit&amp;auml;t und Plastizit&amp;auml;t. Springer Berlin Heidelberg, Berlin.</mixed-citation></ref><ref id="scirp.76655-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Herbig, M. (2011) 3D Short Fatigue Crack Investigation in Beta Titanium Alloys Using Phase and Diffraction Contrast Tomography. INSA de Lyon, Lyon.</mixed-citation></ref><ref id="scirp.76655-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Zhou, P., Zhou, J., Ye, Z., Hong, X., Huang, H. and Xu, W. (2016) Effect of Grain Size and Misorientation Angle on Fatigue Crack Growth of Nanocrystalline Materials. Materials Science and Engineering: A, 663, 1-7.  
https://doi.org/10.1016/j.msea.2016.03.105</mixed-citation></ref><ref id="scirp.76655-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Wu, S.C., Yu, C., Yu, P.S., Buffière, J.Y., Helfen, L. and Fu, Y.N. (2016) Corner Fatigue Cracking Behavior of Hybrid Laser AA7020 Welds by Synchrotron X-Ray Computed Microtomography. Materials Science and Engineering: A, 651, 604-614.  
https://doi.org/10.1016/j.msea.2015.11.011</mixed-citation></ref><ref id="scirp.76655-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Proudhon, H., Li, J., Wang, F., Roos, A., Chiaruttini, V. and Forest, S. (2016) 3D Simulation of Short Fatigue Crack Propagation by Finite Element Crystal Plasticity and Remeshing. International Journal of Fatigue, 82, 238-246.  
https://doi.org/10.1016/j.ijfatigue.2015.05.022</mixed-citation></ref><ref id="scirp.76655-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, T., Bao, R., Lu, S. and Fei, B. (2016) Investigation of Fatigue Crack Propagation Mechanisms of Branching Crack in 2324-T39 Aluminum Alloy Thin Plates under Cyclic Loading Spectrum. International Journal of Fatigue, 82, 602-615.  
https://doi.org/10.1016/j.ijfatigue.2015.09.017</mixed-citation></ref><ref id="scirp.76655-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Lavigne, O., Gamboa, E., Luzin, V., Law, M., Giuliani, M. and Costin, W. (2014) The Effect of the Crystallographic Texture on Intergranular Stress Corrosion Crack Paths. Materials Science and Engineering: A, 618, 305-309.  
https://doi.org/10.1016/j.msea.2014.09.038</mixed-citation></ref><ref id="scirp.76655-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Culbertson, D. and Jiang, Y. (2016) An Experimental Study of the Orientation Effect on Fatigue Crack Propagation in Rolled AZ31B Magnesium Alloy. Materials Science and Engineering: A, 676, 10-19. https://doi.org/10.1016/j.msea.2016.08.088</mixed-citation></ref><ref id="scirp.76655-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Lavigne, O, Gamboa, E., Luzin, V., Law, M., Giuliani, M. and Costin, W. (2014) The Effect of the Crystallographic Texture on Intergranular Stress Corrosion Crack Paths. Materials Science &amp; Engineering: A, 618, 305-309.  
https://doi.org/10.1016/j.msea.2014.09.038</mixed-citation></ref><ref id="scirp.76655-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Sabnis, P.A., Forest, S. and Cormier, J. (2016) Microdamage Modelling of Crack Initiation and Propagation in FCC Single Crystals under Complex Loading Conditions. Computer Methods in Applied Mechanics and Engineering, 312, 468-491.  
https://doi.org/10.1016/j.cma.2016.04.018</mixed-citation></ref><ref id="scirp.76655-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Li, F., Liu, Z., Wu, W., Xia, P., Ying, P., Zhou, Y., et al. (2017) Enhanced Fatigue Crack Propagation Resistance of Al-Cu-Mg Alloy by Intensifying Goss Texture and Refining Goss Grains. Materials Science and Engineering: A, 679, 204-214.  
https://doi.org/10.1016/j.msea.2016.10.003</mixed-citation></ref><ref id="scirp.76655-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Wei, L., Pan, Q., Huang, H., Feng, L. and Wang, Y. (2014) Influence of Grain Structure and Crystallographic Orientation on Fatigue Crack Propagation Behavior of 7050 Alloy Thick Plate. International Journal of Fatigue, 66, 55-64.  
https://doi.org/10.1016/j.ijfatigue.2014.03.009</mixed-citation></ref><ref id="scirp.76655-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Yan, L. and Fan, J. (2016) In-Situ SEM Study of Fatigue Crack Initiation and Propagation Behavior in 2524 Aluminum Alloy. Materials &amp; Design, 110, 592-601.  
https://doi.org/10.1016/j.matdes.2016.08.004</mixed-citation></ref><ref id="scirp.76655-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Li, F., Liu, Z., Wu, W., Xia, P., Ying, P., Zhao, Q., et al. (2016) On the Role of Texture in Governing Fatigue Crack Propagation Behavior of 2524 Aluminum Alloy. Materials Science and Engineering: A, 669, 367-378.  
https://doi.org/10.1016/j.msea.2016.05.091</mixed-citation></ref><ref id="scirp.76655-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Wen, W., Cai, P., Ngan, A.H.W. and Zhai, T. (2016) An Experimental Methodology to Quantify the Resistance of Grain Boundaries to Fatigue Crack Growth in an AA2024 T351 Al-Cu Alloy. Materials Science and Engineering: A, 666, 288-296.  
https://doi.org/10.1016/j.msea.2016.04.071</mixed-citation></ref><ref id="scirp.76655-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Sung, P.-H. and Chen, T.-C. (2015) Studies of Crack Growth and Propagation of Single-Crystal Nickel by Molecular Dynamics. Computational Materials Science, 102, 151-158. https://doi.org/10.1016/j.commatsci.2015.02.031</mixed-citation></ref></ref-list></back></article>