<?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">MSCE</journal-id><journal-title-group><journal-title>Journal of Materials Science and Chemical Engineering</journal-title></journal-title-group><issn pub-type="epub">2327-6045</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msce.2019.73003</article-id><article-id pub-id-type="publisher-id">MSCE-91440</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>
 
 
  Fatigue Responses of Three AA 2000 Series Aluminum Alloys
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gbadebo</surname><given-names>Moses Owolabi</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>Mark</surname><given-names>Thom</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>Olusegun</surname><given-names>Ajide</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>Amin</surname><given-names>Azimi</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>Horace</surname><given-names>Whitworth</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>Grant</surname><given-names>Warner</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>Nikhil</surname><given-names>Kumar</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, Howard University, Washington DC, USA</addr-line></aff><aff id="aff2"><addr-line>Department of Mechanical Engineering, University of Ibadan, Ibadan, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>27</day><month>03</month><year>2019</year></pub-date><volume>07</volume><issue>03</issue><fpage>32</fpage><lpage>48</lpage><history><date date-type="received"><day>17,</day>	<month>February</month>	<year>2019</year></date><date date-type="rev-recd"><day>24,</day>	<month>March</month>	<year>2019</year>	</date><date date-type="accepted"><day>27,</day>	<month>March</month>	<year>2019</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, smooth specimens of three aluminum alloys: AA 2219-T8, AA 2519-T8 and AA 2624-T351, were subjected to the same level of uniaxial (tension/compression) fatigue loading to compare their fatigue responses. Fractographic investigations of the failed specimens after fatigue loading was also conducted using a scanning electron microscope. The fatigue test results showed considerable differences in the fatigue lives of the three investigated alloys with AA 2219-T8 having the shortest fatigue life and AA 2624-T351 the longest fatigue life. The fractographic analysis showed that coalescence of micropores, microvoids, particles cleavage and microcracks are the predominant features in the fracture surface of AA 2219-T8. The fracture surface features of AA 2519-T8 revealed higher resistance to fatigue cracks nucleation and growth when compared to AA 2219-T8. The features depicted mainly partly ductile and partly brittle fracture. The AA 2624-T351 fracture surface features revealed noteworthy ductile failure mechanism. The results suggest a strong correlation between the surface fractographic features and the fatigue lives of the alloys. It is also observed that in addition to the yield strengths and ultimate tensile strengths, the total strain energy densities (SED) may provide a reasonable indication of the relative fatigue performance of the three alloys. AA 2219-T8 had the lowest SED and the lowest fatigue life, while AA 2624-T351 had the highest SED and the highest fatigue life. Thus, AA 2624-T351 would be the most suitable materials for components subjected to fatigue loading.
 
</p></abstract><kwd-group><kwd>Fatigue Life</kwd><kwd> Aluminum Alloy</kwd><kwd> Strain Energy Density</kwd><kwd> Fractography</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Remarkable progress has been made over the past few decades in the development of high performance aluminum alloys. Aluminum alloys have a proven 70-year record of continuously improvement in terms performance and production cost [<xref ref-type="bibr" rid="scirp.91440-ref1">1</xref>] . The benefits of these alloys include their high specific strength, excellent corrosion resistance, high fracture toughness and fatigue crack growth resistance [<xref ref-type="bibr" rid="scirp.91440-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.91440-ref8">8</xref>] . The high strength-to-weight ratio of aluminum alloys makes them choice materials in air and spacecraft where their low density translates to increased fuel efficiency and reduction in green gas emissions [<xref ref-type="bibr" rid="scirp.91440-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.91440-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.91440-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.91440-ref12">12</xref>] .</p><p>Fatigue is critical to the structural integrity of aluminum alloys. Laudable efforts have been made on studies that focused on the fatigue behavior of aluminum alloys. The research investigations conducted recently by Xue et al. [<xref ref-type="bibr" rid="scirp.91440-ref13">13</xref>] on the fatigue life of aging aircraft have invigorated research activities on the formation, detection and estimation of fatigue damage on high strength aluminum alloys. The authors asserted that the determinations of fatigue life and cracks size and crack growth rates are critical for strategic safety evaluation process. Fatigue has been identified by Gupta and Agnew to pose a serious threat to service lives of critical components in aero structures [<xref ref-type="bibr" rid="scirp.91440-ref14">14</xref>] . The fatigue response of Al 2024 T3 laser machined sheets was investigated by Carpio et al. [<xref ref-type="bibr" rid="scirp.91440-ref15">15</xref>] . Results obtained by the authors revealed that the laser machined experimental data are very close to aeronautic requirements for fatigue resistance. However, the predicted theoretical or intrinsic material fatigue resistance was estimated to be significantly higher than the obtained laser machined experimental data. The observed variations were attributed to the surface roughness of the heat affected zone (HAZ), thus promoting crack initiations. In the concluding remark of the paper, it was suggested that the surface roughness as well as the fatigue resistance of the alloy can be enhanced by using higher power and high absorption wavelength (such as λ =1.06 &#181;m). Desmukh et al. [<xref ref-type="bibr" rid="scirp.91440-ref16">16</xref>] investigated the influence of scandium alloying addition on the fatigue response of 7010 aluminum alloy. The study revealed that addition of scandium refines the grain structure of the alloy, but yielded poor fatigue crack growth resistance and fatigue thresholds. Very long-life fatigue and near threshold fatigue crack growth response of 7075 and 6061 aluminum alloys in T6 condition were investigated by Wang et al. [<xref ref-type="bibr" rid="scirp.91440-ref17">17</xref>] . The experimental results show that both alloys can withstand fatigue fracture beyond 10<sup>7</sup> cycles at 210 MPa and 140 MPa for Al-alloys 7075 and 6061, respectively. In addition, the authors observed no evidence of endurance limit in the two alloys until 10<sup>9</sup> cycles (at approximately 195 MPa and 90 MPa for 7075 and 6061, respectively). It was found that the fatigue strength of 7075 alloy is higher than that of 6061, even in the super long life region. Their study also revealed superior fatigue properties of 7075 in comparison with 6061, and could be attributed to the higher tensile strength of the 7075 Al-alloy. The authors were able to establish that the fatigue crack growth rates of small cracks in the investigated alloys were found to be greater than those of large cracks for the same stress intensity factor range. The fractographic analysis revealed that substantial void nucleation occurred in the two aluminum alloys in early stage of fatigue crack propagation. During high crack growth rates, the observed voids were insignificant while striations became obvious. Ceschini et al. [<xref ref-type="bibr" rid="scirp.91440-ref18">18</xref>] studied the influence of Hot Isostatic Pressing (HIP) on the fatigue response of sand-cast A356-T6 and 204-T6 aluminum alloys. Findings from this study revealed that HIP process led to immense reduction in fatigue resistance by about 40% for A356 and 70% for A204. It was also reported that the non-HIP processed A204 alloy showed slightly lower fatigue resistance than A356, which was attributed to the presence of many shrinkage cavities along grain boundaries.</p><p>Sharma et al. [<xref ref-type="bibr" rid="scirp.91440-ref19">19</xref>] examined the fatigue response of AA 2219 under different aging conditions. They reported that the alloy in naturally aged condition exhibited the highest resistance to fatigue cracks initiation. This was followed by fatigue responses of the under aged, peak aged and over aged conditions in that order. The crack growth rate increased while the near threshold stress intensity range decreased with advancing aging conditions. The fracture morphology was observed to experience immense changes from crystallographic facets near the threshold region to region of well-developed ductile striations. Zheng et al. [<xref ref-type="bibr" rid="scirp.91440-ref20">20</xref>] investigated the fatigue behavior of AA 2524-T34 alloys and reported that the fatigue crack initiation and propagation in AA 2524-T34 alloy was dramatically influenced by the presence of second phase particles. The deflection of cracks showed clear crystallographic features, which in turn implies that grain orientation plays a significant role in controlling fatigue crack propagation in the alloy.</p><p>Ma et al. [<xref ref-type="bibr" rid="scirp.91440-ref21">21</xref>] studied the mechanical properties and fatigue crack growth rates in Friction Stir Welded (FSW) nugget of 2198-T8 Al-Li alloy joints. Fatigue tests under different stress ratio (R) were performed on the welded nugget and the parent material. Results showed that the fatigue crack growth rates in the nugget are not like the parent material that is sensitive to stress ratio. In addition, striations on the fracture surfaces were observed in the welded nugget. The fracture surface 2524 aluminum alloy that failed under fatigue loading revealed that the fatigue cracks in this alloy nucleated either on second phase particles or the interface between these particles and the continuous aluminum-rich phase [<xref ref-type="bibr" rid="scirp.91440-ref22">22</xref>] . The observed fracture mechanism consists of microcracks initiation and growth, and merging of microcracks. Yan and Fan [<xref ref-type="bibr" rid="scirp.91440-ref22">22</xref>] have also reported that the direction of microcrack propagation can be influenced by grain boundary. The effect of grain size on the fatigue crack growth in 2524-T3 alloy was examined by Shou et al. [<xref ref-type="bibr" rid="scirp.91440-ref23">23</xref>] . They observed that alloys with grain sizes in the range of 50 - 100 &#181;m to exhibit higher fatigue crack growth rates. Fractography examinations revealed that fatigue cracks propagated in a more tortuous manner in the alloy with grain sizes within the range 50 - 100 &#181;m. Wu et al. [<xref ref-type="bibr" rid="scirp.91440-ref24">24</xref>] investigated the fatigue behavior of an Al-Cu-Li and observed that grain boundaries could not impede the fatigue crack growth due to coarse second phase particles present along the grain boundaries. The propagation of fatigue cracks along grain boundaries reduces the resistance to fatigue crack propagation. Ovono et al. [<xref ref-type="bibr" rid="scirp.91440-ref25">25</xref>] investigated the effect of aging treatment and alloying addition on the fatigue response of A319 and AS9U3G alloys in T5 condition. Results obtained by the authors showed that increase in volume fraction of the alloying elements affected the fatigue life of AS9U3G alloy considerably when compared to that of A319. It was also reported that aging at 320˚C for 100 h yielded notable increase in the fatigue lives of the two investigated alloys.</p><p>Takahashi et al. [<xref ref-type="bibr" rid="scirp.91440-ref26">26</xref>] studied the mechanism surrounding the growth characteristics of microcracks inherent in the Al-Mg-Si 6061-T6 alloy in the high cycle fatigue regime and reported that at a low stress level, over 90% of the total fatigue life was characterized by the growth of microcracks. The microcrack was found to be halted after more than 10<sup>6</sup> cycles to failure and for a long period. After this long period, it began to grow again, which resulted in a significantly slow growth process. Fatigue crack growth response of Friction Stir Welded (FSW) AA 7075-T651 aluminum joint was studied by Sivaraj et al. [<xref ref-type="bibr" rid="scirp.91440-ref27">27</xref>] . The study was carried out using Center Cracked Tensile (CCT) specimens extracted from the FSW joints and that of unwelded material (as-received condition). The outcome of the study showed clearly that the fatigue life of the FSW AA 7075-T651 aluminum alloy suffered a considerable reduction in comparison with the unwelded as-received alloy. The authors attributed the dissolution of the precipitates in the weld region during the friction stir welding as the main cause of fatigue life reduction. The influence of heat treatment and surface quality on the fatigue life of Selective Laser Melting (SLM) produced AlSi10Mg has been examined by Aboulkhair et al. [<xref ref-type="bibr" rid="scirp.91440-ref28">28</xref>] . The study showed that a carefully conducted heat treatment significantly enhanced the fatigue response of the alloy. At 94 MPa stress level, the heat-treated samples survived beyond the nominal fatigue life of 3 &#215; 10<sup>7</sup> cycles of the as-produced SLM AlSi10Mg alloy. Szusta and Seweryn [<xref ref-type="bibr" rid="scirp.91440-ref29">29</xref>] investigated the low cycle fatigue (LCF) behavior of EN AW-2024-T3 at elevated temperatures under multiaxial loading. It was observed that fatigue life of EN AW 2024-T3 aluminum alloy increased as the phase shift between progressions of tensile and torsional loading increased at elevated temperatures. Wang et al. investigated the effects of Laser Shock Peening on high temperature fatigue response of 7075 aluminum alloy [<xref ref-type="bibr" rid="scirp.91440-ref30">30</xref>] using a load frequency of 30 Hz and a load ratio R = 0.1. The authors reported that the high temperature fatigue life of the specimens after laser shock peening treatment exhibited 20% and 110% enhancement at 200˚C and 150˚C, respectively when compared with those without treatment. However, the emergence of gradual reductions in fatigue life commenced at 250˚C. Many other works [<xref ref-type="bibr" rid="scirp.91440-ref31">31</xref>] - [<xref ref-type="bibr" rid="scirp.91440-ref40">40</xref>] have further enriched literature on the fatigue life of aluminum based alloys.</p><p>Enormous research efforts have been made on the study of fatigue lives of 2000 series aluminum alloys. The influence of heat treatment and anodization on fatigue life of 2017A alloy was investigated by Hemmouche et al. [<xref ref-type="bibr" rid="scirp.91440-ref41">41</xref>] . The outcome of the tests showed a decrease in fatigue life of anodized specimens as compared to the untreated ones. The nature of oxide layer and heterogeneous microstructures of the film was reported to cause the observed decrease in the fatigue life of the alloy. The effect of strain ratio and microstructural features on the fatigue response of 2124-T851 aluminum alloy (with smooth surface) during low cycle fatigue was investigated by Hao et al. [<xref ref-type="bibr" rid="scirp.91440-ref42">42</xref>] . The observed microstructural features revealed that density and length of slip bands influences the magnitude of strain ratios. The authors showed that the higher density and larger length of slip bands led to larger strain ratios at the strain amplitude of 0.6%. It was also shown that at larger strain ratios, volume fraction and size of coarse constituents increases. The aftermath of these changes in microstructures were attributed to the reduction in fatigue life of the material. Fares et al. investigated the coupled effect of substrate microstructure and sulphuric process anodizing on the fatigue performance of a 2017A-T4 aluminum alloy [<xref ref-type="bibr" rid="scirp.91440-ref43">43</xref>] . At high alternating stresses, the existence of the anodic film has no pronounced effect on fatigue crack growth of the alloy for both microstructural conditions. Nevertheless, the results obtained at low alternating stresses revealed that anodizing significantly reduces the fatigue life of the alloy for both microstructural conditions. This reduction in fatigue life was attributed to the preferential dissolution of the matrix around the cathodic particles (such as Al<sub>2</sub>Cu). This led to the formation of cavities which acted as stress concentrators thus promoting the nucleation of several fatigue microcracks. A comparative study of the fatigue response of AA 2198-T8 and AA 2024-T3 was considered by Stanley et al. [<xref ref-type="bibr" rid="scirp.91440-ref44">44</xref>] . Fatigue fracture surface morphology was examined. Fractography results shows that AA 2024-T3 exhibited significant twisting fracture surface with localized fatigue crack growths along many directions. Whereas the fracture surface of the AA 2198-T8 was observed by the authors to be characterized with evenly distributed but shallow striations. It was concluded that AA 2198-T8 showed a better fatigue resistance. Jayaraman et al. [<xref ref-type="bibr" rid="scirp.91440-ref45">45</xref>] studied the possibility of improving the fatigue life of Friction Stir Welded (FSW) joint of 2219-T8751 aluminum alloy. The presence of compressive residual stress on the surface of FSW joint has been identified to pose a detrimental effect on the fatigue life of the alloy. A recently developed technique, Low Plasticity Burnishing (LPB), was employed to introduce a deep surface layer on the FSW joint. Fatigue life of FSW joint with LPB and without LPB was estimated. It was found that the FSW joint with LPB had higher fatigue life than the FSW joint without LPB. The outcome of this study reinforces the authors’ hypothesis that the presence of compressive residual stress on the surface of FSW joint can affect its fatigue life. Xu et al. performed strain-controlled cycle fatigue tests on FSW 2219-T62 aluminum at different welding parameters and cooling conditions [<xref ref-type="bibr" rid="scirp.91440-ref46">46</xref>] . Experimental results indicated a slight decrease in fatigue life of the alloy as welding speed was increased from 60 to 200 mm/min. In addition, FSW joints with water cooling condition experienced a higher fatigue life than that with air cooling condition.</p><p>Among the 2000 series aluminum alloys, the choice of AA 2219-T8, AA 2519-T8 and AA 2624-T351 are gaining more prominent research interests for application in aerostructures applications. Notwithstanding, not much work has been done that focused on the fatigue behavior of AA 2219-T8, AA 2519-T8 and AA 2624-T351 aluminum alloys. The main objective of this paper is to provide experimental data on the fatigue response of these alloys and compare their behavior fatigue loading condition.</p></sec><sec id="s2"><title>2. Materials and Experimental Methods</title><sec id="s2_1"><title>2.1. Fatigue Tests</title><p>The three aluminum alloys investigated in this work are AA 2219-T8, AA 2519-T8 and AA 2624-T351. The main alloying element in each of these alloys is copper. The approximate percentages of alloying elements in each of the alloys are presented in <xref ref-type="table" rid="table1">Table 1</xref>. Tensile tests were also conducted on the samples from the same alloys in order to correlate the mechanical properties under quasi-static loading with the fatigue lives of the alloys.</p><p>The fatigue test specimens were machined according to ASTM E466-15 [<xref ref-type="bibr" rid="scirp.91440-ref47">47</xref>] standard as presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Force-controlled loads were applied to the fatigue test specimens, in which each specimen was subjected to nominal stress</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Approximate percentage of the alloying elements</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Elements</th><th align="center" valign="middle" >AA 2219</th><th align="center" valign="middle" >AA 2519</th><th align="center" valign="middle" >AA 2624</th></tr></thead><tr><td align="center" valign="middle" >Aluminum, Al Chromium, Cr Copper, Cu Iron, Fe Magnesium, Mg Manganese, Mn Si + Fe Silicon, Si Titanium, Ti Vanadium, V Zinc, Zn Zirconium, Zr Other, total</td><td align="center" valign="middle" >91.5% - 93.8% - 5.8% - 6.8% ≤0.30% ≤0.02% 0.20% - 0.40% - ≤0.20% 0.02% - 0.10% 0.05% - 0.15% ≤0.10% 0.10% - 0.25% ≤0.15 %</td><td align="center" valign="middle" >91% - 94.4% - 5.3% - 6.4% ≤0.30% 0.05% - 0.40% 0.10% - 0.50% ≤0.40% ≤0.25% 0.02% - 0.10% 0.05% - 0.15% ≤0.10% 0.10% - 0.25% ≤0.15</td><td align="center" valign="middle" >92.79% - 94.55% ≤0.05% 3.8% - 4.3% ≤0.08% 1.2% - 1.6% 0.45% - 0.70% - ≤0.08% ≤0.10% - ≤0.15% - ≤0.15%</td></tr></tbody></table></table-wrap><p>amplitude of approximately 246 MPa. The nominal stress amplitude was kept constant for each specimen in order to provide a basis for comparison of the performance of each tested alloy. Given the nominal diameter of the specimen, the amplitude of force on the specimens was 15.6 kN. The testing frequency was 1 Hz and the stress ratio (R) was −1. The fatigue experiments were conducted on the MTS 809 Axial/Torsional Test System following ASTM E606/E606M-12 [<xref ref-type="bibr" rid="scirp.91440-ref48">48</xref>] standard. The MTS 809 Axial/Torsional is a servo hydraulic system which provides a maximum axial load of 250 kN and a maximum torsional load of 2200 Nm. Tensile tests were also conducted on samples from the same alloys in order to correlate the mechanical properties under quasi-static loading with the fatigue lives of the alloys.</p></sec><sec id="s2_2"><title>2.2. Fractographic Examinations</title><p>Cutting of the required fatigue fracture samples for fractographic examinations was done using high performance tabletop Struers Secotom-15 machine (with rotational speed range: 300 - 5000 rpm). Fracture surfaces of fractured specimens were investigated with the aid of Scanning Electron Microscope, SEM (TESCAN XEIA3).</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Tensile Results</title><p>The results of tensile tests are presented in <xref ref-type="table" rid="table2">Table 2</xref> and their stress-strain curves are illustrated in <xref ref-type="fig" rid="fig2">Figure 2</xref>. It can be seen that the AA 2219-T8 alloy has the lowest yield strength of 288 MPa, while AA 2519-T8 has the highest yield strength of 421 MPa. AA 2624-T351 has a yield strength of 374 MPa. <xref ref-type="table" rid="table2">Table 2</xref> also shows that AA 2219-T8 has the lowest ultimate tensile strength (UTS) of the three alloys with a UTS of 299.54 MPa. AA 2519.T8 and AA 2624-T351 have very similar UTS of 463 and 467 MPa, respectively. The distinction between yield and ultimate strengths indicates lower strain hardening phenomenon in AA 2219-T8 than the two other alloys. However, this microstructure modification is highest in AA 2624-T351 which makes this alloy stronger than other samples. The Young’s modulus (E), Elongation (ε), Poisson’s ratio (υ) and Strain Energy Density (SED) for the three alloys are also included in <xref ref-type="table" rid="table2">Table 2</xref>. These parameters</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Tensile properties of alloys</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Property</th><th align="center" valign="middle" >AA 2219-T8</th><th align="center" valign="middle" >AA 2519-T8</th><th align="center" valign="middle" >AA 2624-T351</th></tr></thead><tr><td align="center" valign="middle" >YS (MPa)</td><td align="center" valign="middle" >288</td><td align="center" valign="middle" >421</td><td align="center" valign="middle" >374</td></tr><tr><td align="center" valign="middle" >UTS (MPa)</td><td align="center" valign="middle" >299</td><td align="center" valign="middle" >463</td><td align="center" valign="middle" >467</td></tr><tr><td align="center" valign="middle" >E (GPa)</td><td align="center" valign="middle" >75.8</td><td align="center" valign="middle" >67.9</td><td align="center" valign="middle" >72.8</td></tr><tr><td align="center" valign="middle" >ε</td><td align="center" valign="middle" >10.6%</td><td align="center" valign="middle" >10.0%</td><td align="center" valign="middle" >19.0%</td></tr><tr><td align="center" valign="middle" >υ</td><td align="center" valign="middle" >0.356</td><td align="center" valign="middle" >0.314</td><td align="center" valign="middle" >0.302</td></tr><tr><td align="center" valign="middle" >SED</td><td align="center" valign="middle" >34.31</td><td align="center" valign="middle" >43.45</td><td align="center" valign="middle" >85.09</td></tr></tbody></table></table-wrap><p>provide insights to the basic tensile characteristics of the three alloys investigated in this work. Poisson’s ratio (υ) is the negative ratio of the transverse strain to the longitudinal strain for given material subjected to uniform longitudinal stress within the elastic deformation range. It is an elastic coefficient that provides insight into strength and ductility which are key design parameters for the investigated alloys. Strain energy density (SED) is a measure of the critical value that can provide insight into the fatigue life as well as macroscopic material failure criterion. The Young’s modulus (E) is a measure of the stiffness of an elastic material in terms of ratio of stress to strain.</p></sec><sec id="s3_2"><title>3.2. Fatigue Test’s Results</title><p>The fatigue lives of the investigated smooth specimens for the three alloys are presented in <xref ref-type="fig" rid="fig3">Figure 3</xref>. AA 2219-T8 had the lowest fatigue life with 3787 cycles. The relatively low fatigue life of AA 2219-T8 was expected due to its being tested at 0.820 of its UTS (which is a significantly higher fraction of its UTS in comparison with the other two alloys). The fatigue life of AA 2519-T8 is 32196 cycles which is almost 9 times higher than that of AA 2219-T8 (see <xref ref-type="fig" rid="fig3">Figure 3</xref>). AA 2519-T8 was tested at 0.531 of its UTS while AA 2624-T351 was tested at 0.526 of its UTS. Notwithstanding, the fatigue life of AA 2624-T351 is 59540 cycles, which is nearly twice that of AA 2519-T8. Assessing the relative fatigue performances against relative tensile test performances of the alloys, a consistent relationship can be observed between the fatigue life and the strain energy density required (SED) for failure of the alloys in the tensile tests. The SED<sub> </sub>for failure of each of the alloy was determined using the area under their respective tensile stress-strain curves (<xref ref-type="fig" rid="fig1">Figure 1</xref>). SED for failure increases with fatigue life of the specimen. As illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>, AA 2219-T8 had the lowest SED and lowest fatigue life, while AA 2624-T351 had the highest SED<sub> </sub>for failure and highest fatigue life. The use of strain energy density in fatigue life prediction</p><p>has been explored and proven to be satisfactory by Tang et al. [<xref ref-type="bibr" rid="scirp.91440-ref49">49</xref>] .</p></sec><sec id="s3_3"><title>3.3. Fatigue Fracture</title><p>Figures 4(a)-(c), Figures 5(a)-(c) and Figures 6(a)-(c) show the SEM fractographs of AA 2219-T8, AA 2519-T8 and AA 2624-T351, respectively. Although traces of dimples are observed in the fractograph of AA 2219-T8 as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), the fracture surface features are characterized by the presence of macrocracks, microcracks, voids and micropores. These significant defects are marked by arrows in <xref ref-type="fig" rid="fig4">Figure 4</xref>. In <xref ref-type="fig" rid="fig4">Figure 4</xref>(b), the presence of particles cleavage, microvoids and microcracks are more prominent at the core of the fracture surface. Secondary phase particles can be observed on the fracture surfaces. There is also evidence of transgranular fracture on the surface failed specimen. In <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), both fine and coarse second phase particles are observed. The fracture morphologies of AA 2219-T8 illustrated in Figures 4(a)-(c) generally depicts ductile and brittle failure modes. However, from the analogy of Rambabu et al. [<xref ref-type="bibr" rid="scirp.91440-ref50">50</xref>] , the coalescence of micropores, microvoids, particles cleavage, microcracks and random intermix are reminiscent of low resistance to fatigue cracks initiation and growth as well as brittle fracture failure mechanism. The features also portray fatigue transgranular fracture. The fracture surface of AA 2519-T8 in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a) can be described as a combination of ridge-like and undulations-like structure containing pores, microcracks and voids that are not pronounced when compared to AA 2219-T8 in Figures 4(a)-(c). Fine particles are seen to be uniformly distributed in the alloy. For AA 2519-T8 (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)), the presence of fatigue striations can be observed on the fracture surface of this alloy, but more intense in the central core as well as X-marked regions of the fractograph. Secondary phase particles appeared to be scanty in the vicinity of striations but densely distributed in region P of the fractograph. There is also the presence of</p><p>microvoids but very limited when compared to that of AA 2219-T8 in Figures 4(a)-(c). The presence of some secondary phase particles in AA 2519-T8 is also</p><p>observed in the vicinity of striations (<xref ref-type="fig" rid="fig5">Figure 5</xref>(c)) and these features are found more significant at the region R of the fracture surface. Microvoids are observed but relatively scanty. The fracture surface features of AA 2519-T8 as observed in Figures 5(a)-(c) showed high resistance to fatigue cracks nucleation and growth in comparison with AA 2219-T8. Although the features depicted dual failure mechanisms (ductile and brittle failure), failure due to ductile was found to be predominant.</p><p>Very fine fatigue striations can be observed on the fracture surface of AA 2624-T351 (<xref ref-type="fig" rid="fig6">Figure 6</xref>(a) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b)). The observed microvoids can be considered insignificant relative to the bulk microstructure. Unlike in the case of AA 2519-T8 alloy where secondary particles are observed in the vicinity of striations (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a) and <xref ref-type="fig" rid="fig5">Figure 5</xref>(b)), the presence of these particles along the striations pattern are not obvious in the fracture surface of AA 2624-T351. In addition, <xref ref-type="fig" rid="fig5">Figure 5</xref>(c) shows an array of very fine fatigue striations to be predominant on the fracture surface of this alloy. The presence of microvoids and microcracks features can be considered insignificant in AA 2624-T351 (Figures 6(a)-(c)) relative to AA 2219-T8 (Figures 4(a)-(c)) and AA 2519-T8 (Figures 5(a)-(c)). The fracture features generally observed in Figures 6(a)-(c) implies highly significant ductile failure mechanism and high resistance to fatigue cracks nucleation and propagation in AA 2624-T351 when compared to AA 2219-T8 and AA 2519-T8 aluminum alloys.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>The fatigue response of smooth specimens of AA 2219-T8, AA 2519-T8 and AA 2624-T351 were investigated in this work. Three different alloys of AA 2000 aluminum series were tested under quasi-static tensile and uniaxial fatigue loads. Fractographic examinations were also carried out to understand the failure and fracture mechanisms of the alloys. The tensile test results show that AA 2219 has the lowest strength, with an ultimate tensile strength that is 65% less than that of the other two alloys. The fatigue results show significant differences in the fatigue lives of the three alloys with AA 2219-T8 having the lowest fatigue life and AA 2624-T351 with the highest fatigue life at the same stress amplitude.</p><p>The following specific conclusions are drawn from this study:</p><p>1) The fracture morphologies of AA 2219-T8 indicate ductile and brittle failure modes. The coalescence of micropores, microvoids, particles cleavage, microcracks and random intermix is indication of low resistance to fatigue cracks initiation and growth. The features strongly revealed brittle and transgranular fracture.</p><p>2) The fracture surface of AA 2519-T8 depicted high resistance to fatigue cracks nucleation and propagation when compared to AA 2219-T8. Dual failure mechanisms (ductile and brittle failure) are observed. However, ductile fracture failure was however found to be predominant.</p><p>3) The AA 2624-T351 fracture surface features implied highly significant ductile failure mechanism and revealed higher resistance to fatigue cracks nucleation and propagation in comparison to AA 2219 and AA 2519 aluminum alloys.</p><p>Future study will focus on obtaining data for plotting the complete S-N curves for each alloy. To attain such data, tests will be conducted in several samples of each alloy over a range of nominal stresses. Future study will also include the effect of thermal treatments on the microstructure and fatigue responses of these alloys.</p></sec><sec id="s5"><title>Acknowledgements</title><p>Financial support for this work was provided by DoD through contract # W911NF-15-1-0457 under the direct supervision of Patricia Huff (HBCU/MI Program Manager, ARO).</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Owolabi, G.M., Thom, M., Ajide, O., Kumar, N., Azimi, A., Whitworth, H. and Warner, G. (2019) Fatigue Responses of Three AA 2000 Series Aluminum Alloys. 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