<?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">MSA</journal-id><journal-title-group><journal-title>Materials Sciences and Applications</journal-title></journal-title-group><issn pub-type="epub">2153-117X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/msa.2022.132005</article-id><article-id pub-id-type="publisher-id">MSA-115360</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>
 
 
  Polylactic Acid (PLA) Foaming: Design of Experiments for Cell Size Control
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Miada</surname><given-names>Abubaker Osman</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>Nick</surname><given-names>Virgilio</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>Mahmoud</surname><given-names>Rouabhia</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Frej</surname><given-names>Mighri</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Chemical Engineering, Polytechnique Montreal, Montreal, Canada</addr-line></aff><aff id="aff3"><addr-line>Faculty of Dentistry, Laval University, Quebec, Canada</addr-line></aff><aff id="aff1"><addr-line>Research Center for High Performance Polymer and Composite Systems, CREPEC, Montreal, Canada</addr-line></aff><aff id="aff4"><addr-line>Department of Chemical Engineering, Faculty of Science and Engineering, Laval University, Quebec, Canada</addr-line></aff><pub-date pub-type="epub"><day>21</day><month>02</month><year>2022</year></pub-date><volume>13</volume><issue>02</issue><fpage>63</fpage><lpage>77</lpage><history><date date-type="received"><day>8,</day>	<month>Jnauary</month>	<year>2022</year></date><date date-type="rev-recd"><day>19,</day>	<month>February</month>	<year>2022</year>	</date><date date-type="accepted"><day>22,</day>	<month>February</month>	<year>2022</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 study, a design of experiments (DoE) approach was used to develop a PLA open-cell foam morphology using the compression molding technique. The effect of three molding parameters (foaming time, mold opening temperature, and weight concentration of the ADA blowing agent) on the cellular structure was investigated. A regression equation relating the average cell size to the above three processing parameters was developed from the DoE and the analysis of variance (ANOVA) was used to find the best dimensional fitting parameters based on the experimental data. With the help of the DoE technique, we were able to develop various foam morphologies having different average cell size distribution levels, which is important in the development of open-cell PLA scaffolds for bone regeneration for which the control of cell morphology is crucial for osteoblasts proliferation. For example, at a constant ADA weight concentration of 5.95 wt%, we were able to develop a narrow average cell size distribution ranging between 275 and 300 μm by varying the mold opening temperature between 106
  &#176;C and 112
  &#176;C, while maintaining the foaming time constant at 8 min, or by varying the mold foaming time between 6 and 11 min and maintaining the mold opening temperature at 109&#176;C.
 
</p></abstract><kwd-group><kwd>PLA</kwd><kwd> Open-Cell Foam</kwd><kwd> Design of Experiments</kwd><kwd> Cell Size Distribution</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Polymer foams are found everywhere in our modern world daily life since they are used in different applications such as cushioning, insulation material [<xref ref-type="bibr" rid="scirp.115360-ref1">1</xref>], and biomedical applications as scaffolds in tissue engineering [<xref ref-type="bibr" rid="scirp.115360-ref2">2</xref>]. A polymer foam is typically obtained from a polymer and gas mixture, which gives the polymer a cellular structure (open-cell or closed-cell) with the desired thermal, mechanical, and/or acoustic properties. In addition, it causes the polymer to have a lower density. There are several methods to produce polymer foams, such as injection or compression molding, and extrusion. Polymer foams are either based on thermoplastics or thermosets; the main difference being that the first ones can be reprocessed, while the second ones cannot [<xref ref-type="bibr" rid="scirp.115360-ref1">1</xref>]. For all the foaming processes (extrusion, injection, or compression molding) using chemical foaming agents, the selection of the latter is based on a general rule of thumb. Its decomposition temperature should be relatively close to the polymer processing temperature, and the released gas should not chemically react with the polymer [<xref ref-type="bibr" rid="scirp.115360-ref3">3</xref>].</p><p>Recently, research has focused on the partial substitution of petrochemical-based polymers with biobased ones due to safety (non-toxicity), environmental, and economic challenges [<xref ref-type="bibr" rid="scirp.115360-ref4">4</xref>]. Polylactic acid (PLA) is one of the main biobased thermoplastic polymers due to its good processability and its high strength and modulus [<xref ref-type="bibr" rid="scirp.115360-ref5">5</xref>]. It is presently considered as one of the main biomaterials and is largely used in industrial packaging, biocompatible/bioabsorbable medical devices, and as a replacement of regular petrochemical-based polymers for many industrial applications [<xref ref-type="bibr" rid="scirp.115360-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref6">6</xref>]. PLA is obtained from lactic acid (LA), which is an organic acid produced from renewable non-toxic raw materials [<xref ref-type="bibr" rid="scirp.115360-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref8">8</xref>]. Corn starch or sugarcane are examples of the renewable resources from which LA can be obtained by fermentation [<xref ref-type="bibr" rid="scirp.115360-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref10">10</xref>]. As a result, PLA is classified as an eco-friendly material, is considered to be biocompatible with the human body (nontoxicity), and is presently classified by the United States Food and Drug Administration (FDA) as a safe biomaterial (GRAS) [<xref ref-type="bibr" rid="scirp.115360-ref4">4</xref>]. This has led to more research activities, especially in the biomedical sector [<xref ref-type="bibr" rid="scirp.115360-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref13">13</xref>].</p><p>There are many advantages of PLA compared to other biopolymers [<xref ref-type="bibr" rid="scirp.115360-ref4">4</xref>]: 1) its biocompatibility is particularly attractive for biomedical applications. A biocompatible material must not generate carcinogenic or toxic effects in local tissues, and the products coming from its degradation should not interfere with the healing tissue. When a PLA scaffold is implanted in living organisms, it hydrolyzes to its constituent α-hydroxy acid, then combines into the tricarboxylic acid cycle, and is finally eliminated from the organism [<xref ref-type="bibr" rid="scirp.115360-ref13">13</xref>]; 2) PLA is an eco-friendly material since it is synthesized from renewable resources (e.g., wheat, corn, or rice). It is also recyclable, biodegradable, and compostable [<xref ref-type="bibr" rid="scirp.115360-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.115360-ref14">14</xref>]; 3) PLA presents a good thermal processability, compared to many other biopolymers [<xref ref-type="bibr" rid="scirp.115360-ref15">15</xref>]; 4) Finally, the production of PLA needs 25% to 55% less energy compared to petroleum-based polymers [<xref ref-type="bibr" rid="scirp.115360-ref13">13</xref>].</p><p>The main objective of this study is to design, by compression molding, an open-cell PLA foam scaffold for bone and cartilage regeneration. Research presented in this article is a first part of a broader study and focuses only on the effect of the processing parameters on cell morphology and cell size distribution of the developed foams. This will be essential in the second part of the project, where a biocompatible PLA-based open cell scaffold with a tailored cell size and narrow cell size distribution will be designed. So, the originality of the present work is the obtention of adequate sets of optimised processing parameters needed for the design of different levels of narrow cell size distributions needed for cells proliferation, such as bone or cartilage cells.</p><p>To do this, a three-level factorial Design of Experiments (DoE) based on the response surface method (RSM) [<xref ref-type="bibr" rid="scirp.115360-ref16">16</xref>] is used to investigate the influence of three foaming process parameters (foaming time, mold opening temperature, and the blowing agent weight concentration) and their interactions on the average cell size of the developed foamed scaffolds. The main purpose of the DoE is the selection of the experimental conditions and the evaluation of their corresponding responses. A polynomial mathematical model representing the process is then constructed to find the optimal design [<xref ref-type="bibr" rid="scirp.115360-ref17">17</xref>]. The Central Composite Design (CCD) sketched in <xref ref-type="fig" rid="fig1">Figure 1</xref> is a type of RSM technique that is used to find the minimum number of experiments that should be evaluated to optimize the variables and their corresponding responses. The eight black corners of the cube correspond to the factorial points, while the six white circles correspond to the axial points. As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, if the distance from the center of the design space to a factorial point is &#177;1 unit for each factor, the distance α ( | α | &gt; 1 ) from the center of the design space to an axial point can be found with the following Equation (1) [<xref ref-type="bibr" rid="scirp.115360-ref18">18</xref>]:</p><p>α = ( n f ) 1 / 4 (1)</p><p>For a three-level factorial DoE, eight factorial points ( n f = 2 3 = 8 ), six axial points (2 &#215; 3) and six centre runs, a total of 20 experimental runs can be considered. Generally, these experimental runs are conducted in random order [<xref ref-type="bibr" rid="scirp.115360-ref18">18</xref>], [<xref ref-type="bibr" rid="scirp.115360-ref19">19</xref>]. The value of α in Equation (1) is then calculated ( α = 8 1 / 4 = 1.682 ).</p><p>The appropriate low-level (−1) and high-level (+1) settings of each variable for the “cube” are calculated as follows:</p><p>{ Low-level ( − 1 ) = ( ( α − 1 ) V max + ( α + 1 ) V min ) / 2 α High-level ( + 1 ) = ( ( α − 1 ) V min + ( α + 1 ) V max ) / 2 α (2)</p><p>where V<sub>min</sub> and V<sub>max</sub> are respectively the minimum and maximum levels of the process parameters studied.</p></sec><sec id="s2"><title>2. Materials and Methodology</title><sec id="s2_1"><title>2.1. Materials</title><p>Polylactide (PLA) (Ingeo biopolymer 2003D, 4.3 mol% D-lactide content, specific gravity: 1.24, tensile strength: 53 MPa, melting temperature: 151˚C) was purchased from NatureWorks, USA. Azodicarbonamide (ADA, CELOGEN 754A, density: 1.68 g/cm<sup>3</sup> at 25˚C, decomposition temperature: 164˚C - 180˚C) was purchased from CelChem, USA.</p></sec><sec id="s2_2"><title>2.2. Sample Preparation and Foaming Process</title><p>First, PLA was dried under vacuum for 12 h at 50˚C using a Shel Lab oven, model 1445. Then, it was mixed for 3 min with ADA added at different weight concentrations (see <xref ref-type="table" rid="table1">Table 1</xref>), using a Hamilton Beach Single-Serve Blender (model 51101BZ). The PLA/ADA mixture was then placed into the mold cavity (0.3 cm &#215; 6 cm &#215; 6 cm) placed between the plates of an automatic compression press (Carver, Model: Auto series 3893). For all of the samples, the compressing pressure was maintained constant at 12 MPa and the compression (foaming) time was varied from 5 to 15 min, depending on the experiment, as shown in <xref ref-type="table" rid="table2">Table 2</xref>. Foamed PLA samples were then obtained by reducing the temperature of the mold to the mold opening temperature (values are shown in <xref ref-type="table" rid="table1">Table 1</xref>). Finally, the mold was opened, and the foamed sample was cooled down to room temperature. Scheme 1 shows a sketch of the different steps of the foaming process.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The three independent foaming parameters (foaming time, mold opening temperature, blowing agent concentration) and their corresponding levels obtained by the CCD technique</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Factors</th><th align="center" valign="middle" >Tag</th><th align="center" valign="middle" >Symbol</th><th align="center" valign="middle" >Units</th><th align="center" valign="middle"  colspan="5"  >Levels</th></tr></thead><tr><td align="center" valign="middle"  colspan="4"  ></td><td align="center" valign="middle" >−α</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >+α</td></tr><tr><td align="center" valign="middle" >Foaming time</td><td align="center" valign="middle" >t</td><td align="center" valign="middle" >X<sub>1</sub></td><td align="center" valign="middle" >min</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >7.03</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12.97</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" >Mold opening temperature</td><td align="center" valign="middle" >T</td><td align="center" valign="middle" >X<sub>2</sub></td><td align="center" valign="middle" >˚C</td><td align="center" valign="middle" >80</td><td align="center" valign="middle" >88.1</td><td align="center" valign="middle" >100</td><td align="center" valign="middle" >111.9</td><td align="center" valign="middle" >120</td></tr><tr><td align="center" valign="middle" >ADA blowing agent weight concentration</td><td align="center" valign="middle" >IC</td><td align="center" valign="middle" >X<sub>3</sub></td><td align="center" valign="middle" >Wt%</td><td align="center" valign="middle" >4.20</td><td align="center" valign="middle" >4.91</td><td align="center" valign="middle" >5.95</td><td align="center" valign="middle" >6.99</td><td align="center" valign="middle" >7.70</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Randomization of the independent factors for X<sub>1</sub>, X<sub>2</sub>, and X<sub>3</sub> in experimental runs and their corresponding average cell size</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Run number</th><th align="center" valign="middle" >Factor for X<sub>1</sub></th><th align="center" valign="middle" >Factor for X<sub>2</sub></th><th align="center" valign="middle" >Factor for X<sub>3</sub></th><th align="center" valign="middle" >Average cell size (&#181;m)</th><th align="center" valign="middle" >Average cell size standard deviation (&#181;m)</th><th align="center" valign="middle" >Coefficient of variation, CV = (Standard deviation/ average cell size)</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >287</td><td align="center" valign="middle" >41</td><td align="center" valign="middle" >0.140</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−α</td><td align="center" valign="middle" >194</td><td align="center" valign="middle" >39</td><td align="center" valign="middle" >0.200</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >311</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0.019</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >289</td><td align="center" valign="middle" >17</td><td align="center" valign="middle" >0.059</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >368</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >0.068</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >+α</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >326</td><td align="center" valign="middle" >49</td><td align="center" valign="middle" >0.150</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >276</td><td align="center" valign="middle" >31</td><td align="center" valign="middle" >0.110</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >−α</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >209</td><td align="center" valign="middle" >19.5</td><td align="center" valign="middle" >0.093</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >+α</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >294</td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >0.065</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >254</td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >0.098</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >−α</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >136</td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >0.140</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >232</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >0.052</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >84</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.060</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >α</td><td align="center" valign="middle" >317</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >0.038</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >323</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >0.050</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >251</td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >0.140</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >278</td><td align="center" valign="middle" >49</td><td align="center" valign="middle" >0.176</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >+1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >−1</td><td align="center" valign="middle" >233</td><td align="center" valign="middle" >62</td><td align="center" valign="middle" >0.266</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >283</td><td align="center" valign="middle" >39</td><td align="center" valign="middle" >0.140</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >262</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >0.092</td></tr></tbody></table></table-wrap></sec><sec id="s2_3"><title>2.3. Foam Cell Measurement</title><p>PLA foam samples were first frozen in liquid nitrogen to ensure a brittle fracture [<xref ref-type="bibr" rid="scirp.115360-ref19">19</xref>]. Magnified pictures of the fractured surfaces were then acquired using a stereomicroscope (Model: SZ-PT 126x) and the average cell size was obtained using the image processing, Image J, software (at least three measurements per cell were done and their average value is reported). The final average cell size was calculated from the results of at least three different samples for each run.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. Determination of the Three Levels of the Processing Parameters: Foaming Time, Mold Opening Temperature, and ADA Blowing Agent Concentration</title><p>The central composite design (CCD) technique was used in this work to design the three levels (low-level: −1, mid-level: 0, and high-level: +1) of the three independent processing parameters shown in <xref ref-type="table" rid="table1">Table 1</xref>, which are the foaming time under compression, X<sub>1</sub> (min), the mold opening temperature, X<sub>2</sub> (˚C), and the ADA blowing agent weight concentration, X<sub>3</sub> (wt%). The mold opening temperature is the temperature at which the mold is opened following a rapid cooling upon the end of the foaming time.</p><p>As reported in literature, the decomposition temperature of ADA is between 165˚C and 180˚C [<xref ref-type="bibr" rid="scirp.115360-ref20">20</xref>], and the melting temperature of PLA is 150˚C [<xref ref-type="bibr" rid="scirp.115360-ref21">21</xref>]. Using ADA as a foaming agent, Luo, Zhang, Qi, Lu, Hu and Jiang [<xref ref-type="bibr" rid="scirp.115360-ref21">21</xref>] reported that the optimum foaming temperature for PLA is 180˚C during a foaming time under compression of 10 min. Based on this study, the foaming temperature was maintained constant at 180˚C and the foaming time X<sub>1</sub> (min) was considered as an independent parameter for cell size optimization. Its minimum and maximum limits were taken at equal intervals from the foaming time of 10 min used by the above authors (X<sub>1min</sub> = 5 min, X<sub>1max</sub> = 15 min).</p><p>To get an adequate foam, the mold must be cooled quickly after PLA foaming to increase the PLA viscosity and consequently avoid cell collapse. Mold opening should be performed at a temperature that is between the glass transition temperature (T<sub>g</sub>) and the melting temperature of PLA, which are 58˚C and 151˚C, respectively [<xref ref-type="bibr" rid="scirp.115360-ref21">21</xref>]. It was found that when the mold opening temperature was higher than 120˚C, bubbles were ruptured due to the low PLA viscosity; on the other hand, when the temperature was lower than 80˚C, not enough bubbles were formed. Based on these observations, the mold opening temperature was set between X<sub>2min</sub> = 80˚C and X<sub>2max</sub> = 120˚C for cell optimization.</p><p>To study the effect of the ADA blowing agent concentration on the average cell size, preliminary tests were performed at 180˚C to determine the minimum and maximum ADA concentrations needed to obtain a foam with an open-cell structure. For a mold opening temperature of 100˚C and a foaming time of 10 min, the ADA concentration was slowly increased until the formation of an open cell structure, which was obtained at 4.2 wt% ADA. On the other hand, foam collapse was observed for ADA weigh concentrations higher than 7.7 wt%. Based on these results, the ADA concentration was set between 4.2 wt% and 7.7 wt%.</p><p>Knowing the minimum and maximum values of the three independent parameters X<sub>1</sub>, X<sub>2</sub> and X<sub>3</sub>, the calculation of their corresponding low-level (−1), mid-level (0), and high-level (+1) values is done using the CCD technique (<xref ref-type="fig" rid="fig1">Figure 1</xref>) and the corresponding values are shown in <xref ref-type="table" rid="table1">Table 1</xref>. As an example, the following steps show how to find the corresponding values for the foaming time, X<sub>1</sub> (min): 1) First, the minimum and maximum values of X<sub>1</sub> corresponding to −α and +α are respectively 5 min and 15 min, as mentioned above in this section; 2) the mid-level (0), which is the center between −α and +α, is then equal to (5 + 15)/2 = 10 min; 3) Equation (2) is then used to get the low and high level settings of X<sub>1</sub>, which are respectively:</p><p>{ Low-level ( − 1 ) = ( ( 1.682 − 1 ) &#215; 15   min   + ( 1.682 + 1 ) &#215; 5   min ) / ( 2 &#215; 1.682 ) = 7.03   min High-level ( + 1 ) = ( ( 1.682 − 1 ) &#215; 5   min   + ( 1.682 + 1 ) &#215; 15   min ) / ( 2 &#215; 1.682 ) = 12.97   min</p><p>The low, mid, and high levels for X<sub>2</sub> and X<sub>3</sub> are calculated in the same manner and their corresponding values are shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p></sec><sec id="s3_2"><title>3.2. Effect of the Foaming Time, Mold Opening Temperature, and ADA Blowing Agent Concentration on the Average Cell Size</title><p>Figures 2(a)-(c) show SEM micrographs corresponding to foamed samples respectively obtained from the runs 11, 1 and 6, presented below in <xref ref-type="table" rid="table2">Table 2</xref>. Their corresponding foaming time and blowing agent concentration were kept constant at 10 min and 5.95 wt% and their mold opening temperature was varied [80˚C (level: −α) (<xref ref-type="fig" rid="fig2">Figure 2</xref>(a)), 100˚C (level: 0) (<xref ref-type="fig" rid="fig2">Figure 2</xref>(b)), and 120˚C (level: +α) (<xref ref-type="fig" rid="fig2">Figure 2</xref>(c))]. As shown, closed cell structure was obtained under a mold opening temperature of 80˚C and larger cells were obtained with increasing the mold opening temperature, leading to an open cell structure at 120˚C. The corresponding results are presented in <xref ref-type="table" rid="table2">Table 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). An increase of the mold opening temperature from 80˚C to 120˚C is accompanied by a respective increase in the average cell size from 136 &#181;m to 326 &#181;m. Because of PLA matrix viscosity decrease and gas diffusion increase inside the PLA matrix with increasing the temperature, this leads to an increase in the formation and growth</p><p>of bubbles [<xref ref-type="bibr" rid="scirp.115360-ref21">21</xref>].</p><p>Keeping the foaming time and mold opening temperature constant at 10 min and 100˚C, respectively, the ADA weight concentration was varied from 4.2 wt% to 7.7 wt% and the corresponding results are presented in <xref ref-type="table" rid="table2">Table 2</xref> (runs 1, 2, and 14) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(b). The results show that an increase in ADA concentration is accompanied by an increase in cell size due to the higher gas concentration/amount generated inside the PLA matrix during ADA degradation, [<xref ref-type="bibr" rid="scirp.115360-ref21">21</xref>].</p><p>The effect of the foaming time on the average cell size was studied under a constant mold opening temperature (T = 100˚C) and ADA concentration (5.95 wt%) (i.e., X<sub>2</sub> and X<sub>3</sub> = 0: runs 8, 9, 7). As shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(c), an increase of the foaming time from 5 min to 15 min leads to a respective increase of the average cell size from 209 &#181;m to 294 &#181;m. This is because there is enough time for the generated smaller bubbles to expand and in many cases meet each other due to the high pressure gases [<xref ref-type="bibr" rid="scirp.115360-ref22">22</xref>].</p></sec><sec id="s3_3"><title>3.3. Statistical Analysis and Equation Relating the Average Cell Size to the Foaming Time, Mold Opening Temperature and Foaming Agent Weight Concentration</title><p>The Minitab 17.0 software was used to randomize the 20 experimental runs shown in <xref ref-type="table" rid="table2">Table 2</xref>, and the polynomial model used by the software for the calculation of the cells average size, Y, as a function of the three significant factors X<sub>1</sub>, X<sub>2</sub>, and X<sub>3</sub>, and their combinations, is given by Equation (3):</p><p>Y = a + b &#215; X 1 + c &#215; X 2 + d &#215; X 3 + e &#215; ( X 1 &#215; X 1 ) + f &#215; ( X 2 &#215; X 2 )     + g &#215; ( X 3 &#215; X 3 ) + h &#215; ( X 1 &#215; X 2 ) + i &#215; ( X 1 &#215; X 3 ) + j &#215; ( X 2 &#215; X 3 ) (3)</p><p>where the parameters a to j are adimensional fitting parameters.</p><p>The coefficient of variation (CV) shown in <xref ref-type="table" rid="table2">Table 2</xref>, which is the ratio between the standard deviation and the average cell size, gives an indication about the level of dispersion around the average cell size. Lower CV means a lower level of dispersion around the average cell size. Distributions with a coefficient of variation (CV) less than 1 are considered to be low-variance distributions, whereas those with a CV higher than 1.0 are considered to be high-variance distributions [<xref ref-type="bibr" rid="scirp.115360-ref23">23</xref>].</p><p>The analysis of variance (ANOVA) was used to find the best dimensional fitting parameters a to j of Equation (2), based on the experimental data of <xref ref-type="table" rid="table2">Table 2</xref> obtained for the 20 experimental runs. The final form of this equation with the calculated fitting parameters is as follows (Equation (4)):</p><p>Y = − 2352 + 72.2 &#215; X 1 + 26.1 &#215; X 2 + 189 &#215; X 3 − 0.006 &#215; ( X 1 &#215; X 1 )     − 0.0515 &#215; ( X 2 &#215; X 2 ) + 1.26 &#215; ( X 3 &#215; X 3 ) − 0.375 &#215; ( X 1 &#215; X 2 )     − 4.13 &#215; ( X 1 &#215; X 3 ) − 1.252 &#215; ( X 2 &#215; X 3 ) (4)</p><p>The statistical significance of the fitting parameters of the above regression model used to estimate the average cell size was based on their probability values (P-values) presented in <xref ref-type="table" rid="table3">Table 3</xref>. These P-values indicate if the regression model</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> The P-values corresponding to the regression model (Equation (4))</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Source</th><th align="center" valign="middle" >P-Value</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"  >Linear interactions</td></tr><tr><td align="center" valign="middle" >X 1</td><td align="center" valign="middle" >0.001</td></tr><tr><td align="center" valign="middle" >X 2</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >X 3</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle"  colspan="2"  >Square interactions</td></tr><tr><td align="center" valign="middle" >X 1 ∗ X 1</td><td align="center" valign="middle" >0.993</td></tr><tr><td align="center" valign="middle" >X 2 ∗ X 2</td><td align="center" valign="middle" >0.291</td></tr><tr><td align="center" valign="middle" >X 3 ∗ X 3</td><td align="center" valign="middle" >0.839</td></tr><tr><td align="center" valign="middle"  colspan="2"  >2-Way Interaction</td></tr><tr><td align="center" valign="middle" >X 1 ∗ X 2</td><td align="center" valign="middle" >0.162</td></tr><tr><td align="center" valign="middle" >X 1 ∗ X 3</td><td align="center" valign="middle" >0.177</td></tr><tr><td align="center" valign="middle" >X 2 ∗ X 3</td><td align="center" valign="middle" >0.108</td></tr><tr><td align="center" valign="middle" >Lack-of-Fit</td><td align="center" valign="middle" >0.273</td></tr></tbody></table></table-wrap><p>fails to sufficiently describe the functional relationship between the average cell size and the three studied parameters (foaming time, X<sub>1</sub>, mold opening temperature, X<sub>2</sub>, and ADA blowing agent concentration, X<sub>3</sub>). The fitting parameters are considered significant if their corresponding P-values are less than 0.05, and not significant if their P-values are greater than 0.05 [<xref ref-type="bibr" rid="scirp.115360-ref24">24</xref>]. As shown in <xref ref-type="table" rid="table3">Table 3</xref>, the P-values corresponding to the linear interaction between the cell size (Y) and the foaming process parameters X<sub>1</sub>, X<sub>2</sub>, and X<sub>3</sub> were all significant(their corresponding p-values are less than 0.05). However, their corresponding square and 2-way interactions were insignificant (corresponding P-values where higher than 0.05). Finally, the P-value for the lack of fit was 0.273 (i.e., higher than 0.05), which means that there is no lack of fit and the regression model sufficiently describes the functional relationship between the average cell size (Y) and the independent processing parameters X<sub>1</sub>, X<sub>2</sub>, and X<sub>3</sub>.</p><p>The regression analysis of the 20 runs presented in <xref ref-type="table" rid="table2">Table 2</xref> also provides various residual plots and two of them are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> (the normal probability plot, <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), and the residuals versus associated fitted values, <xref ref-type="fig" rid="fig4">Figure 4</xref>(b)). The normal probability plot of the residuals displays the residuals versus their expected values when the distribution is normal. Ideally, this plot should approximately follow a diagonal straight line (fitted values). <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) clearly shows a normal distribution of the residuals. The difference between the observed values (round symbols) and their corresponding diagonal fitted values (continuous line), is relatively small. On the other hand, the residuals should ideally fall randomly around the center (zero) line, which is the case, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b). This indicates a high degree of correlation between the observed and predicted residual values.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the optimization curves for the average cell size maximization (i.e., the maximization of the response Y) obtained using the “response optimizer” in the Minitab software. To do this, the three independent parameters X<sub>1</sub>, X<sub>2</sub> and X<sub>3</sub> were respectively varied from 5 to15 min (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a)), 80˚C to 120˚C (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)), and 4.2 to 7.7 wt% (<xref ref-type="fig" rid="fig5">Figure 5</xref>(c)). As shown, the maximum average cell size of 392.4 μm was obtained at a foaming time of 5 min, and a mold opening temperature of 120˚C.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> presents the contour plots showing the evolution of the average cell size (&#181;m) with the variation of two of the three independent processing parameters, while maintaining the third one constant. <xref ref-type="fig" rid="fig6">Figure 6</xref>(a) shows that, for a constant ADA weight concentration of 5.95 wt%, the average cell size increases from 125 &#181;m to about 375 &#181;m with increasing the foaming time from 5 min to 15 min (X-axis) and the mold opening temperature from 80˚C to 120˚C (Y-axis). So, the average cell size can be tailored by varying one or both of the two processing parameters, mold opening temperature or the foaming time. For example, a narrow average cell size ranging between 275 and 300 &#181;m can be obtained under a foaming time of 8 min and a mold opening time ranging between 106˚C and 112˚C, or a mold opening temperature of 109˚C and a foaming time ranging between 6 and 11 min. <xref ref-type="fig" rid="fig6">Figure 6</xref>(b) shows that, for a foaming time maintained constant at 10 min, the average cell size increases from 100 &#181;m to about 400 &#181;m with increasing the mold opening temperature from 80˚C to 120˚C (X-axis) and the ADA weight concentration from 4.2 wt% to 7.7 wt% (Y-axis). So, a narrow average cell size ranging between 275 and 300 &#181;m can be obtained using 7.0 wt% ADA and a mold opening time ranging between 91 and</p><p>101˚C. Finally, <xref ref-type="fig" rid="fig6">Figure 6</xref>(c) shows that, at a constant mold opening temperature of 100˚C, the average cell size varied from 150 &#181;m to about 375 &#181;m with increasing the foaming time from 5 min to 15 min (X-axis) and ADA concentration from 4.2 wt% to 7.7 wt% (Y-axis). The same narrow average cell size ranging between 275 and 300 &#181;m can be obtained using 6.8 wt% ADA and a foaming time between 7.2 min and 11.6 min.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>In this work, open-cell foamed PLA scaffolds were developed by compression molding and a three-level factorial Design of Experiments (DoE) was used to optimize the molding parameters (foaming time, mold opening temperature, and ADA blowing agent concentration) to reach a well-controlled open-cell structure. The minimum and maximum values of these three molding parameters were obtained using the CCD technique and their corresponding values were 5 and 15 min, 80˚C and 120˚C, and 4.2 and 7.7 wt%, respectively. The morphology of the developed foams was then studied by varying the three processing parameters between these limits. It was observed that, for a constant ADA concentration of 5.95 wt%, when the mold opening temperature increased from 80˚C to 120˚C, the average cell size was respectively increased from 136 &#181;m to 326 &#181;m because of the decrease in PLA matrix viscosity and consequently ADA gas diffusion increase inside the PLA matrix, leading to an increase in the formation and growth of cells. Also, under a constant mold opening temperature of 100˚C, an increase of the foaming time from 5 min to 15 min led to a respective increase of the average cell size from 209 &#181;m to 294 &#181;m because more time is given to the generated smaller bubbles to expand. Furthermore, for constant foaming time (10 min) and mold opening temperature (100˚C), an increase of ADA weight concentration from 4.2 wt% to 7.7 wt% led to an increase of the average cell size from 197 &#181;m to 317 &#181;m due to the higher gas concentration generated during ADA degradation.</p><p>Finally, we were able to show how the average cell size can be tailored by varying two of the three independent processing parameters, while maintaining the third one constant. For example, a narrow average cell size ranging between 275 and 300 &#181;m was obtained under a foaming time of 8 min and mold opening time values between 106˚C and 112˚C, or a mold opening temperature of 109˚C and foaming time values between 6 and 11 min. This is important in the development of open-cell PLA scaffolds for bone regeneration for which the control of cell morphology is crucial for osteoblasts proliferation.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors acknowledge the financial support of the Natural Science and Engineering Research Council of Canada (NSERC) and the Research center for high performance polymer and composite systems (CREPEC).</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>Osman, M.A., Virgilio, N., Rouabhia, M. and Mighri, F. (2022) Polylactic Acid (PLA) Foaming: Design of Experiments for Cell Size Control. Materials Sciences and Applications, 13, 63-77. https://doi.org/10.4236/msa.2022.132005</p></sec></body><back><ref-list><title>References</title><ref id="scirp.115360-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Sivertsen, K. (2007) Polymer Foams. 3.063 Polymer Physics. https://ocw.mit.edu/courses/materials-science-and-engineering/3-063-polymer-physics-spring-2007/assignments/polymer_foams.pdf</mixed-citation></ref><ref id="scirp.115360-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Nofar, M. and Park, C.B. (2014) Poly(Lactic Acid) Foaming. Progress in Polymer Science, 39, 1721-1741. https://doi.org/10.1016/j.progpolymsci.2014.04.001</mixed-citation></ref><ref id="scirp.115360-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Rhomie, L. and Heck, I. (2004) A Review of Commercially Used Chemical Foaming Agents for Thermoplastic Foams. Journal of Vinyl and Additive Technology, 4, 113-116. https://doi.org/10.1002/vnl.10027</mixed-citation></ref><ref id="scirp.115360-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Jamshidian, M., Arab-Tehrany, E., Imran, M., Jacquot, M. and Desobry, S. (2010) Poly-Lactic Acid: Production, Applications, Nanocomposites, and Release Studies. Comprehensive Reviews in Food Science and Food Safety, 9, 552-571. https://doi.org/10.1111/j.1541-4337.2010.00126.x</mixed-citation></ref><ref id="scirp.115360-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Auras, R., Lim, L.T., Selke, S.E.M. and Tsuji, H. (2010) Poly(Lactic Acid): Synthesis, Structures, Properties, Processing, and Applications. John Wiley Sons Inc., Hoboken, 529. https://doi.org/10.1002/9780470649848</mixed-citation></ref><ref id="scirp.115360-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Drumright, R.E., Gruber, P.R. and Henton, D.E. (2000) Polylactic Acid Technology. Advanced Materials, 12, 1841-1846. https://doi.org/10.1002/1521-4095(200012)12:23&lt;1841::AID-ADMA1841&gt;3.0.CO;2-E</mixed-citation></ref><ref id="scirp.115360-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Savioli Lopes, M., Jardini, A.L. and Maciel Filho, R. (2012) Poly(Lactic Acid) Production for Tissue Engineering Applications. Procedia Engineering, 42, 1402-1413. https://doi.org/10.1016/j.proeng.2012.07.534</mixed-citation></ref><ref id="scirp.115360-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Lasprilla, A.J., Martinez, G.A., Lunelli, B.H., Jardini, A.L. and Filho, R.M. (2012) Poly-Lactic Acid Synthesis for Application in Biomedical Devices—A Review. Biotechnology Advances, 30, 321-328. https://doi.org/10.1016/j.biotechadv.2011.06.019</mixed-citation></ref><ref id="scirp.115360-ref9"><label>9</label><mixed-citation publication-type="book" xlink:type="simple">Mckeen, L. (2014) Plastics Used in Medical Devices. In: Modjarrad, K. and Ebnesajjad, S, Eds., Handbook of Polymer Applications in Medicine and Medical Devices, Elsevier, Amsterdam, 21-53. https://doi.org/10.1016/B978-0-323-22805-3.00003-7</mixed-citation></ref><ref id="scirp.115360-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Sodergard, A. and Stolt, M. (2002) Properties of Lactic Acid Based Polymers and Their Correlation with Composition. Progress in Polymer Science, 27, 1123-1163. https://doi.org/10.1016/S0079-6700(02)00012-6</mixed-citation></ref><ref id="scirp.115360-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Phiriyawirut, M., Sarapat, K., Sirima, S. and Prasertchol, A. (2019) Porous Electrospun Nanofiber from Biomass-Based Polyester Blends of Polylactic Acid and Polybutylene Succinate. Open Journal of Polym. Chemistry, 9, 1-15. https://doi.org/10.4236/ojpchem.2019.91001</mixed-citation></ref><ref id="scirp.115360-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Tachibana, Y., et al. (2021) Environmental Biodegradability of Recombinant Structural Protein. Scientific Reports, 11, Article No. 242. https://doi.org/10.1038/s41598-020-80114-6</mixed-citation></ref><ref id="scirp.115360-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Rasal, R.M., Janorkar, A.V. and Hirta, D.E. (2010) Poly(Lactic Acid) Modifications. Progress in Polymer Science, 35, 338-356. https://doi.org/10.1016/j.progpolymsci.2009.12.003</mixed-citation></ref><ref id="scirp.115360-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Sawyer, D.J. (2003) Bioprocessing—No Longer a Field of Dreams. Macromolecular Symposia, 201, 271-281. https://doi.org/10.1002/masy.200351130</mixed-citation></ref><ref id="scirp.115360-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Auras, R., Harte, B. and Selke, S. (2004) An Overview of Polylactides as Packaging Materials. Macro-Molecular Bioscience, 4, 835-864. https://doi.org/10.1002/mabi.200400043</mixed-citation></ref><ref id="scirp.115360-ref16"><label>16</label><mixed-citation publication-type="book" xlink:type="simple">Khuri, A.I. (2003) Current Modeling and Design Issues in Response Surface Methodology: GLMs and Models with Block Effects. In: Khattree, R., Ed., Handbook of Statistics, Vol. 22, Elsevier, Amsterdam, 209-229. https://doi.org/10.1016/S0169-7161(03)22008-3</mixed-citation></ref><ref id="scirp.115360-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Song, C., Kitamura, Y. and Li, S. (2014) Optimization of a Novel Cryogenic CO2 Capture Process by Response Surface Methodology (RSM). Journal of the Taiwan Institute of Chemical Engineers, 4, 1666-1676. https://doi.org/10.1016/j.jtice.2013.12.009</mixed-citation></ref><ref id="scirp.115360-ref18"><label>18</label><mixed-citation publication-type="book" xlink:type="simple">Prasanta, S. and Tapan, Kr.B. (2012) ANN Modelling of Fractal Dimension in Machining. In: Davim, J.P., Ed., Mechatronics and Manufacturing Engineering, Elsevier, Amsterdam, 159-226. https://doi.org/10.1533/9780857095893.159</mixed-citation></ref><ref id="scirp.115360-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Lin, L., Lee, Y. and Park, H.E. (2021) Recycling and Rheology of Poly(Lactic Acid) (PLA) to Make Foams Using Supercritical Fluid. Physics of Fluids, 33, Article ID: 067119. https://doi.org/10.1063/5.0050649</mixed-citation></ref><ref id="scirp.115360-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Tatibouet, J. and Gendron, R. (2005) Nucleation Mechanisms Investigated on Polystyrene/HFC-134 Mixtures. The 7th International Conference on Blowing Agents and Foaming Processes, Stuttgart, 10-11 May 2005, 1-8. https://books.google.ca/books/about/Blowing_Agents_and_Foaming_Processes_200.html?id=BVl-aENtK48C&amp;redir_esc=y</mixed-citation></ref><ref id="scirp.115360-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Luo, Y., Zhang, J., Qi, R., Lu, J., Hu, X. and Jiang, P. (2013) Polylactide Foams Prepared by a Traditional Chemical Compression-Molding Method. Journal of Applied Polymer Science, 130, 330-337. https://doi.org/10.1002/app.39023</mixed-citation></ref><ref id="scirp.115360-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Bhatnagar, N. and Srivatsan, T.S. (2009) Processing and Fabrication of Advanced Materials, XVII. International Publishing House Pvt. Ltd., New Delhi, Vol. 2, 728-729. https://www.worldcat.org/title/processing-and-fabrication-of-advanced-materials-xvii/oclc/318093504</mixed-citation></ref><ref id="scirp.115360-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Ospina, R. and Marmolejo-Ramos, F. (2019) Performance of Some Estimators of Relative Variability. Frontiers in Applied Mathematics and Statistics, 5, Article No. 43. https://doi.org/10.3389/fams.2019.00043</mixed-citation></ref><ref id="scirp.115360-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Genawi, N.M., Ibrahim, M.H., El-Naas, M.H. and Alshaik, A.E. (2020) Chromium Removal from Tannery Wastewater by Electrocoagulation: Optimization and Sludge Characterization. MDPI Water, 12, 1374. https://doi.org/10.3390/w12051374</mixed-citation></ref></ref-list></back></article>