<?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">OJCM</journal-id><journal-title-group><journal-title>Open Journal of Composite Materials</journal-title></journal-title-group><issn pub-type="epub">2164-5612</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojcm.2014.42011</article-id><article-id pub-id-type="publisher-id">OJCM-44687</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Interfacial Fracture Toughness Evaluation of Poly(L-lactide acid)/Natural Fiber Composite by Using Double Shear Test Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hin</surname><given-names>Voon Sia</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yoshikazu</surname><given-names>Nakai</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>Hiroshi</surname><given-names>Tanaka</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>Daiki</surname><given-names>Shiozawa</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mechanical Engineering, Kobe University, Kobe, Japan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>cvsia@swinburne.edu.my(HVS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>04</month><year>2014</year></pub-date><volume>04</volume><issue>02</issue><fpage>97</fpage><lpage>105</lpage><history><date date-type="received"><day>18</day>	<month>February</month>	<year>2014</year></date><date date-type="rev-recd"><day>18</day>	<month>March</month>	<year>2014</year>	</date><date date-type="accepted"><day>25</day>	<month>March</month>	<year>2014</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 work, interfacial fracture toughness between treated fiber and matrix was investigated by using double shear test method. Susrface treatment on the oil palm empty fruit bunch (OPEFB) fibers was performed to improve the interfacial bosnding properties of natural fiber reinforced Poly(L-lactide acid) composites. Three fibers model composite and four fibers model composite were prepared for the double shear test. The interfacial fracture toughness of both model composites is dependent on matrix length. In addition, the interfacial fracture toughness and the critical interfacial shear stress were increased with increasing the concentration of NaOH and the duration of surface treatment. 
 
</p></abstract><kwd-group><kwd>Fiber</kwd><kwd> Interfacial Fracture Toughness</kwd><kwd> Interfacial Shear Strength</kwd><kwd> Surface Treatment</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Fiber reinforced plastic (FRP) composites have played an important role in various applications for their high specific strength and modulus. Recently, renewal of interest in the research of fibers derived from natural sustainable sources as potential reinforcement for high performance composites has been growing. The increasing interest in the biodegradable composites reinforced with natural fibers [<xref ref-type="bibr" rid="scirp.44687-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref5">5</xref>] due to the advantages of being biodegradable, renewable, environmentally friendly and low cost. However, many studies revealed that the poor mechanical properties of natural fibers reinforced composites can be attributed to the low interfacial bonding strength between fiber and matrix [<xref ref-type="bibr" rid="scirp.44687-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref8">8</xref>]. Therefore, there is an interest in developing test methods for measuring the interfacial toughness between fiber and matrix.</p><p>The recent evaluation crack propagation behaviour of FRP was based on meso-mechanical analysis. The common test methods used to evaluate the interfacial fracture between fiber and matrix are Microbond test [<xref ref-type="bibr" rid="scirp.44687-ref9">9</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref11">11</xref>], Broutman test [<xref ref-type="bibr" rid="scirp.44687-ref12">12</xref>] , fiber push-out [<xref ref-type="bibr" rid="scirp.44687-ref13">13</xref>] and fiber pull-out test [<xref ref-type="bibr" rid="scirp.44687-ref14">14</xref>] . The crack propagation in FRP was evaluated from fracture process like matrix fracture and fiber/matrix interfacial cracking [<xref ref-type="bibr" rid="scirp.44687-ref15">15</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref17">17</xref>] . Kotaki et al. [<xref ref-type="bibr" rid="scirp.44687-ref18">18</xref>] and Hojo et al. [<xref ref-type="bibr" rid="scirp.44687-ref19">19</xref>] reported that the crack propagation behavior in FRP is strongly influenced by the interfacial bonding between fiber and matrix. Koiwa et al. [<xref ref-type="bibr" rid="scirp.44687-ref20">20</xref>] introduced the measurement on the interfacial fracture toughness of Mode I and Mode II crack growth by using real size model composite. They reported a significant increase in fracture toughness with increasing bonding length. However, the results of fracture toughness were evaluated at a very short range of the matrix lengths.</p><p>In the present study, Mode II interfacial fracture toughness between treated oil palm empty fruit bunch (OPEFB) fiber and Poly(L-lactide acid) (PLLA) composite was evaluated by using the double shear test method which consists of 3 fibers model composite and 4 fibers model composite. The fibers used in both model composites were pretreated 0.5 M alkali solution for 24 h. In addition, 0.5 M, 2 h alkali treated fibers were also prepared in the present study in order to compare the effects of the alkali treatments on interfacial fracture toughness and the critical interfacial shear stress of the model composites. Scanning electron microscope (SEM) was utilized to observe the morphology of the crack propagation between fiber/matrix interfaces.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Materials</title><p>OPEFB fibers were purchased from Ecofibre Technology Sdn. Bhd, Malaysia. These untreated fibers were approximately 150 - 550 μm diameter and 40 - 150 mm in length. PLLA fibers with diameter of 0.2 mm were supplied by Unitika Ltd, Japan and sodium hydroxide (NaOH) was purchased in Hyogo, Japan.</p></sec><sec id="s2_2"><title>2.2. Surface Treatment</title><p>OPEFB fibers were kept in oven at 21˚C &#177; 1˚C for 24 h for conditioning which according to ASTM D1776-04 [<xref ref-type="bibr" rid="scirp.44687-ref21">21</xref>] . The fibers were then separately soaked in 0.5 M NaOH solution for 2 hand 1.0 M NaOH solution for 24 h. After completing treatment, the alkali treated fibers were washed and rinsed with distilled water for several times until the final pH was maintained at 7.0. Finally, the fibers were dried at room temperature for 48 h before making the composites.</p></sec><sec id="s2_3"><title>2.3. Model Composite Specimens</title><p>Three fiber model composite and four fibers model composite were prepared for the Mode II interfacial test. Prior to preparing the specimens, OPEFB fibers were aligned closely in parallel on a paper tab with a small tension force applied on the fibers to avoid loosening of the fibers. Both end points of the fibers were then glued by using epoxy resin adhesive. After the fibers were aligned, a small amount of melted PLLA obtained from a PLLA fiber was placed at the mid-point in between 2 OPEFB fibers. The final matrix length of the specimen was measured after the melted PLLA was completely cured. The schematics and SEM micrographs of the 3 fibers model specimen and 4 fibers model specimen were shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> respectively. The matrix length, L of the test specimens was from 0.24 to 5.81 mm, and the angle of the fibers, 2θ which shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) for bonding section was from 98 to 180 degrees.</p></sec><sec id="s2_4"><title>2.4. Mode II Interfacial Test Method</title><p>Double shear test of the specimens were carried out by using a Tohei MT201 tensile test machine with a crosshead speed of 9 mm/min and 50 N loads.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref>(a) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) show the schematics of the three fibers double shear model composite and the</p><p>four fibers double shear model composite respectively. By simplifying the model composites into Sections 1-3, the strain energy of the model composites can be obtained as below.</p><disp-formula id="scirp.44687-formula53736"><label>(1)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\b62b20db-f1c6-4db7-9193-82bc03c5c043.png"  xlink:type="simple"/></disp-formula><p>where U<sub>i</sub>, U<sub>ii</sub> and U<sub>iii</sub> are the strain energy of the Section (1), (2) and (3) in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b). The equations of U<sub>i</sub>, U<sub>ii</sub> and U<sub>iii</sub> are stated below.</p><p>Three fibers model:</p><disp-formula id="scirp.44687-formula53737"><label>(2)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\8a167c35-dbe9-4c76-8632-dc90470b32c5.png"  xlink:type="simple"/></disp-formula><p>Four fibers model:</p><disp-formula id="scirp.44687-formula53738"><label>(3)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\d2c5fe7d-f37a-4ea9-9474-ab4f17cb24a9.png"  xlink:type="simple"/></disp-formula><p>where E = 4.95 GPa [<xref ref-type="bibr" rid="scirp.44687-ref22">22</xref>] , D is diameter of OPEFB fiber, P is the applied force, L, m and n are the length of the section in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b).</p><p>The energy release rate at crack tip A and B are given by the following equations.</p><p>Three fibers model:</p><disp-formula id="scirp.44687-formula53739"><label>(4)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\354c9882-7612-429a-8e32-0e8ad0803c9a.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.44687-formula53740"><label>(5)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\896e368b-ce57-450e-a30e-58803ac886ef.png"  xlink:type="simple"/></disp-formula><p>Four fibers model:</p><disp-formula id="scirp.44687-formula53741"><label>(6)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\93475040-86b6-433a-946e-9b17689efa3d.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.44687-formula53742"><label>(7)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\ff20fe57-3042-45cc-8856-5a45537d3a22.png"  xlink:type="simple"/></disp-formula><p>Since the matrix length is measured after the resin is cured, the both sides of the center fiber may have different matrix lengths. By considering one outer fiber bonded with minimum matrix length, L<sub>min</sub> in Section (3) from the <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) or <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) have the equilibrium of forces in longitudinal direction, the mean interfacial shear stress at the shortest interface of fiber/matrix with bonding area, A = DθL<sub>min</sub> can be defined as:</p><disp-formula id="scirp.44687-formula53743"><label>(8)</label><graphic position="anchor" xlink:href="htmlimages\2-1810104x\eb478c66-b68e-45be-979c-67afde5cd73a.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_5"><title>2.5. Scanning Electron Microscopy (SEM)</title><p>Treated and untreated fiber surface were observed by using a (Hitachi, TM3000, Japan) scanning electronmicroscope. The SEM fractography of the model composites were also investigated and the bonding angle, 2θ can be obtained from the SEM images by using image analyzing software (ImageJ v1.38x, National Institutes of Health, Bethesda, USA).</p></sec></sec><sec id="s3"><title>3. Result and Discussion</title><sec id="s3_1"><title>3.1. Surface Characterization of Treated Fibers</title><p>Alkali treatment of OPEFB fibers causes disruption of hydrogen bonding in the network structure. This treatment also removes certain amount of lignin, wax, oils and other impurities that cover on the external surface layer of the fiber. As a result, the surface roughness of the fiber is improved [<xref ref-type="bibr" rid="scirp.44687-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.44687-ref23">23</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref25">25</xref>] .  <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) show the SEM micrographs of the untreated fiber, fiber treated with 0.5 M NaOH for 2 h and fiber treated with 1.0 M NaOH for 24 h respectively. As seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), the roughness of fiber surface increased when the concentration of alkali solution and the duration of alkali treatment were increased.</p></sec><sec id="s3_2"><title>3.2. Interfacial Fracture Toughness of the Model Composites</title><p>For all cases, the interfacial fracture toughness, G<sub>i</sub><sub> </sub>was found independent on the fiber diameters, D, angle of bonding interface, 2θ and spacing between fibers, t. However, interfacial fracture toughness of both model composites does depend on the matrix length (<xref ref-type="fig" rid="fig5">Figure 5</xref>). For 0.24 &lt; L &lt; 2.35 mm, the G<sub>i</sub> value of the 3 fibers model composite increases from 14.7 J/m<sup>2</sup> to 108.6 J/m<sup>2</sup> as the L increased. The G<sub>i</sub><sub> </sub>value is stable at L &gt; 2.35 mm. Hence, the data points s to the matrix lengths ranging more than 2.35 mm were used to calculate the average G<sub>i</sub><sub> </sub>value (70.8 &#177; 13.7 J/m<sup>2</sup>). Same observation was found in 4 fibers model composite. For 0.66 &lt; L &lt; 2.29 mm, G<sub>i</sub><sub> </sub> value of the 4 fibers model composite increases from 21.4 J/m<sup>2</sup> to 102.4 J/m<sup>2</sup> as the L in-</p><p>creased. After that, the G<sub>i</sub><sub> </sub>value is stable with further increase in matrix length. For L &gt; 3 mm, the average G<sub>i</sub><sub> </sub>value obtained from the data points is 73.6 &#177; 15.7 J/m<sup>2</sup>. A slight difference from the average G<sub>i</sub> value of the 3 fibers model composite was observed.</p><p>The increase of interfacial fracture toughness, G<sub>i</sub> with matrix length, L at small matrix lengths was attributed to the increase in volume of matrix for plastic deformation in response to shear. However, the interfacial fracture toughness leveling off when the plastic deformation at the crack tip no longer occupies uniformly the entire matrix length, but constraint at the vicinity at the crack tips with further increase in matrix length, L [<xref ref-type="bibr" rid="scirp.44687-ref26">26</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref28">28</xref>] .</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows the relationship between interfacial fracture toughness and matrix length with different fiber treatment conditions. As seen in <xref ref-type="fig" rid="fig6">Figure 6</xref>, the G<sub>i</sub> value of the 3 fibers model composite with 0.5 M, 2 h alkali treated fibers generally increased with matrix length until a stable value was reach at matrix length about 2.5 mm. The average G<sub>i</sub> value obtained from the data points at L &gt; 2.5 mm is 57.1 &#177; 10.4 J/m<sup>2</sup>, which is 13.7 J/m<sup>2</sup> lower than the average G<sub>i</sub> value of the 3 fibers model composite with 1.0 M, 24 h alkali treated fibers.</p></sec><sec id="s3_3"><title>3.3. Interfacial Shear Stress</title><p><xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref> present the relationship between mean interfacial shear stress, τ<sub>i</sub> and bonding area at minimum bonding length, A. As illustrated in  <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>, the mean interfacial shear stress, τ<sub>i</sub><sub> </sub>of the model composite decreased with increasing in bonding area, A. Similar observations were found in other studies for kevlar fiber [<xref ref-type="bibr" rid="scirp.44687-ref9">9</xref>] , glass fiber [<xref ref-type="bibr" rid="scirp.44687-ref29">29</xref>] , carbon fiber [<xref ref-type="bibr" rid="scirp.44687-ref30">30</xref>] , and steel wire [<xref ref-type="bibr" rid="scirp.44687-ref31">31</xref>] which bonded with either thermoplastic orthermosetting adhesives. The τ<sub>i</sub>-A relation can be explained as follows. The occurrence probability of the critical flaws increases with increasing the bonding area, thereby increasing the chances that initiate fracture upon loading [<xref ref-type="bibr" rid="scirp.44687-ref29">29</xref>] -[<xref ref-type="bibr" rid="scirp.44687-ref31">31</xref>] .</p><p>As seen in <xref ref-type="fig" rid="fig7">Figure 7</xref>, the τ<sub>i</sub> values of the 3 fibers model composite have some slight differences with the τ<sub>i</sub> values of the 4 fibers model composite, but in general results are in rather good agreement with the results ob-</p><p>tained from 4 fibers model composite. <xref ref-type="fig" rid="fig8">Figure 8</xref> compares the τ<sub>i</sub>-A relation of the model composites with different alkali treatment conditions. The overall τ<sub>i</sub><sub> </sub>value of the model composite with 0.5 M, 2 h alkali treated fibers are slightly lower than the τ<sub>i</sub><sub> </sub>value of the model composite with 1.0 M, 24 halkali treated fibers. As explanation above, the improvement of the mean interfacial shear stress is believed to be due to surface roughening by the alkali treatment. This promotes better interlocking between fiber and matrix and improves the interfacial adhesion.</p></sec><sec id="s3_4"><title>3.4. Morphological Analysis</title><p><xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0 show the micrographs of the fracture surface at the initial crack tips of the treated fiber/ PLLA models. The surface of the fiber can be clearly observed from <xref ref-type="fig" rid="fig9">Figure 9</xref>(a) and the matrix was also found on the surface of the outer fiber (<xref ref-type="fig" rid="fig9">Figure 9</xref>(b)). Therefore, the crack was propagated along the interface between center fiber and matrix. From the experimental data, 31 out of 34 tested 3 fibers model composites and 18 out of 30 tested 4 fibers model composites were identified where the crack was propagated along the interface between</p><p>center fiber and matrix.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>The present work evaluated the interfacial fracture toughness and the interfacial shear stress of the treated OPEFB fiber/PLLA model composites. The following conclusions can be drawn from this work:</p><p>1) The interfacial fracture toughness of the model composites is dependent on matrix length. The average interfacial fracture toughness can be successfully evaluated at L &gt; 2.35 mm for 3 fibers model composite and at L &gt; 3 mm for 4 fibers model composite.</p><p>2) The mean interfacial shear stress decreases with increasing in bonding area, A. This may be due to the increase of the occurrences probability of the critical defects when the bonding interface between fiber and matrix was increased.</p><p>3) The interfacial fracture toughness and the mean interfacial shear stress of the model composite increase with increasing the concentration of alkali solution and the duration of surface treatment.</p></sec><sec id="s5"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.44687-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mohanty, A.K., Misra, M. and Drzal, L.T. (2005) Natural Fibers, Biopolymers and Biocomposite. CRC Press, Boca Raton. http://dx.doi.org/10.1201/9780203508206</mixed-citation></ref><ref id="scirp.44687-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Shinoj, S., Visvanathan, R., Panigrahi, S. and Kochubabu, M. (2011) Oil Palm Fiber (OPF) and Its Composite: A Review. 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