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  <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">2327-6053</issn>
      <issn pub-type="ppub">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.2026.142004</article-id>
      <article-id pub-id-type="publisher-id">msce-149704</article-id>
      <article-categories>
        <subj-group>
          <subject>Article</subject>
        </subj-group>
        <subj-group>
          <subject>Chemistry</subject>
          <subject>Materials Science</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Optimization of the Viscosity of Wack (Cameroon) Clay Slurry for Coating of a Filtration Layer over a Tubular Ceramic Support Layer by the Slip Casting Technique for Domestic Water Treatment</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Yanu</surname>
            <given-names>Celestine Asobo</given-names>
          </name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <contrib-id contrib-id-type="orcid">0000-0002-8508-3807</contrib-id>
          <name name-style="western">
            <surname>Nguiamba</surname>
            <given-names>Ngiongboung</given-names>
          </name>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Ngomo</surname>
            <given-names>Orleans</given-names>
          </name>
          <xref ref-type="aff" rid="aff3">3</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Sieliechi</surname>
            <given-names>Joseph Marie</given-names>
          </name>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
        <contrib contrib-type="author">
          <name name-style="western">
            <surname>Ngassoum</surname>
            <given-names>Martin Benoit</given-names>
          </name>
          <xref ref-type="aff" rid="aff4">4</xref>
        </contrib>
      </contrib-group>
      <aff id="aff1"><label>1</label> Department of Chemistry, Faculty of Science, University of Buea, Buea, Cameroon </aff>
      <aff id="aff2"><label>2</label> Department of Applied Chemistry, Faculty of Science, University of Ebolowa, Ebolowa, Cameroon </aff>
      <aff id="aff3"><label>3</label> Department of Organic Chemistry, Faculty of Science, University of Yaounde 1, Yaounde, Cameroon </aff>
      <aff id="aff4"><label>4</label> Department of Applied Chemistry, National School of Agro-Industrial Sciences, University of Ngaoundere, Ngaoundere, Cameroon </aff>
      <author-notes>
        <fn fn-type="conflict" id="fn-conflict">
          <p>The authors declare no conflicts of interest regarding the publication of this paper.</p>
        </fn>
      </author-notes>
      <pub-date pub-type="epub">
        <day>09</day>
        <month>02</month>
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="collection">
        <month>02</month>
        <year>2026</year>
      </pub-date>
      <volume>14</volume>
      <issue>02</issue>
      <fpage>50</fpage>
      <lpage>72</lpage>
      <history>
        <date date-type="received">
          <day>20</day>
          <month>08</month>
          <year>2025</year>
        </date>
        <date date-type="accepted">
          <day>21</day>
          <month>02</month>
          <year>2026</year>
        </date>
        <date date-type="published">
          <day>24</day>
          <month>02</month>
          <year>2026</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>© 2026 by the authors and Scientific Research Publishing Inc.</copyright-statement>
        <copyright-year>2026</copyright-year>
        <license license-type="open-access">
          <license-p> This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license ( <ext-link ext-link-type="uri" xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</ext-link> ). </license-p>
        </license>
      </permissions>
      <self-uri content-type="doi" xlink:href="https://doi.org/10.4236/msce.2026.142004">https://doi.org/10.4236/msce.2026.142004</self-uri>
      <abstract>
        <p>The objective of this work is to optimize the viscosity of Wack clay slurry for coating of a filtration layer over a tubular ceramic membrane support by the slip casting technique for application in domestic water treatment. Coating of a slurry over tubular ceramic membrane support by the slip casting technique requires a clay slurry of appropriate viscosity for it to adhere to the ceramic support by capillary suction. The clay slurry is elaborated using a mixture experimental design with constraint used to determine the optimum viscosity of the slurry, the proportions of raw materials in the slurry and the level of influence and interactions between the proportions of raw material on the viscosity of the slurry. The experimental domain used for the raw materials was: proportion of clay between 10% and 12%, proportion of binder between 11% and 22% and proportion of water between 66% and 79%. It resulted that the proportion of clay has the highest positive influence on the viscosity of the slurry and the interaction proportion of clay-proportion of binder influences positively the viscosity of the slurry. The optimal viscosity was found to be 40.4 mPa∙s for optimal proportions of clay, binder and water/dispersant of 10%, 11% and 79% respectively. The prepared optimal slurry was then cast over the support for contact times of 2, 4 and 6 minutes in order to determine the effect time on the compromise homogeneity (no cracks) and thickness (5 - 15 µm) of the deposited layer. When each contact time was attended, it was dried, sintered at 900˚C and characterized. It resulted that as the contact time increases, there is an increase in the thickness of the deposited layer from 8.8 to 23 µm with the gradual appearance of cracks from 4 minutes. The tubular membrane coated for 2 minutes gave the best results in terms of homogeneity and thickness of 8.8 µm. The porosity, permeability and average pore size this multilayer membrane were determined. It resulted from this that the membrane had a porosity of 32.6%, permeability of 305.67 L/h∙m<sup>2</sup> bar and an average pore size of 0.48 µm adapted for microfiltration.</p>
      </abstract>
      <kwd-group kwd-group-type="author-generated" xml:lang="en">
        <kwd>Slip Casting</kwd>
        <kwd>Filtration Layer</kwd>
        <kwd>Mixture Design with Constraint</kwd>
        <kwd>Contact Time</kwd>
        <kwd>Viscosity</kwd>
        <kwd>Optimization</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>1. Introduction</title>
      <p>Ceramic membrane layers have been widely used in the treatment of domestic drinking water [<xref ref-type="bibr" rid="B1">1</xref>][<xref ref-type="bibr" rid="B2">2</xref>]. These membranes are porous support layers made from inorganic materials such as clay and capable of eliminating suspended particles and even microorganisms from water [<xref ref-type="bibr" rid="B3">3</xref>]. These ceramic support layers however do not eliminate these pollutants totally from water (retention capacity generally less than 85%) [<xref ref-type="bibr" rid="B4">4</xref>]. Recent studies have shown that coating these ceramic support layers with another fine clay layer greatly ameliorates the elimination of these pollutants from water (retention capacity greater than 95%) [<xref ref-type="bibr" rid="B5">5</xref>]. The coated layer consists of a filtration layer over which filtration takes place first before going through the porous support layer. The support ceramic layer and the deposited filtration layer constitute a multilayer ceramic membrane used in the treatment and amelioration of the quality of domestic drinking water. Different techniques have been used to coat these ceramic support layers they include: spray coating, dip coating, sol-gel process, tape casting and slip casting techniques. Slip casting is the most appropriate technique used in coating slurry on a tubular ceramic support layers since it is easy to realize at a relatively lower cost compared to the other techniques [<xref ref-type="bibr" rid="B6">6</xref>]. Tubular membranes have the advantage over the other forms of membrane (disc, pot, cylindrical) in that they offer low fouling during filtration as it is mostly used in tangential filtration compared to the frontal filtration used by the other forms [<xref ref-type="bibr" rid="B7">7</xref>]. Previous studies have shown that coating a filtration layer over a tubular ceramic support by the slip casting technique is influenced by the viscosity of the clay slurry which depends on the proportion of raw materials used [<xref ref-type="bibr" rid="B8">8</xref>][<xref ref-type="bibr" rid="B9">9</xref>]. Slurries that are too viscose or not viscose at all will not adhere properly on the ceramic support layer by capillary suction producing a deformed and cracked deposited filtration layer which would not retain the pollutants efficiently from water, hence low retention [<xref ref-type="bibr" rid="B6">6</xref>][<xref ref-type="bibr" rid="B8">8</xref>][<xref ref-type="bibr" rid="B10">10</xref>]. Authors have shown that the viscosity of the slurry increases with the proportion of clay and binder but tends to decrease with an increase in the proportion of water [<xref ref-type="bibr" rid="B5">5</xref>][<xref ref-type="bibr" rid="B10">10</xref>]. These authors generally used the one variable analysis method to study the effects of these factors on the viscosity of the clay slurry. No experimental design was used by these authors, resulting in little information known on the effect and the interaction between the clay, binder and water on the viscosity of the slurry [<xref ref-type="bibr" rid="B11">11</xref>]. Hence, the needs to use an experimental mixture design with constraints to determine the effect and optimal proportions of each ingredient on the viscosity of the slurry. Mixture design with constraint is a better tool used for mixing the different proportions of raw materials rather than one variable mixing as it verifies how the properties of interest (viscosity in this case) are affected by the variation of these proportions in a mixture. It also permits to determine the interactions and the optimal proportions of the raw materials in the mixture [<xref ref-type="bibr" rid="B12">12</xref>]. Casting or coating of slurry of optimum viscosity onto the porous support is influenced by the parameter contact time slurry/support which determines the homogeneity and thickness of the deposited layer by capillary suction of the slurry onto the porous support [<xref ref-type="bibr" rid="B5">5</xref>]. Authors have shown that high contact times ≥ 6 mins lead to a high suction of the slurry on the support, but have as a consequence in that it leads to the saturation of the support giving a fragile (cracked) layer after sintering and to the formation of a thick and less porous layer which decreases the flow rate [<xref ref-type="bibr" rid="B8">8</xref>]. The best contact time is one which will give ideally a homogenous layer with thickness comprised between 5 - 15 µm, porosity between 30% - 35% and pore size between 0.1 - 2 μm after sintering to be adapted for microfiltration for the elimination of suspended particles and other pollutants [<xref ref-type="bibr" rid="B6">6</xref>][<xref ref-type="bibr" rid="B10">10</xref>].</p>
      <p>Considering such research trends, the objective of this work is to elaborate and coat the filtration layer (tubular multilayer) from Wack (Cameroon) clay by the slip casting technique. Specifically, to determine the optimal formulation of raw materials that gives the best viscosity of the slurry using a mixture design with constraint and to determine the best contact time to have the required homogeneity and thickness of the filtration layer. </p>
    </sec>
    <sec id="sec2">
      <title>2. Material and Methods</title>
      <sec id="sec2dot1">
        <title>2.1. Composition of the Wack Clay Slurry for the Filtration Layer</title>
        <p>A slurry is a stable suspension of mineral particles and is generally composed of mineral powder, solvent, the dispersant and organic additives. Indeed, organic additives such as binders, surfactants or thickeners make it possible to control the rheology of the slurry and to ensure the adhesion of the layer after evaporation of solvent during first stages of sintering and the creation of pores on the layer after thermal treatment. The slurry was composed of the following:</p>
        <p>Wack Clay (50 µm);The solvent (alkali water of pH 8.2 that acts as both a solvent and a dispersant);The binder (PVA prepared at 12%).</p>
        <p>The combination of a well-defined percentage of the different elements making up the slurry, leads to a stable, not flocculated suspension that can be deposited on the support to form layers without defects (homogenous).</p>
        <p>2.1.1. Preparation of the Wack Clay</p>
        <p>The choice of the granulometry of the clay powder to be deposited will depend on final morphological characteristics desired for the membrane. Indeed, the principal parameter that should be well mastered and known is the size (granulometry) of the raw material. This parameter will influence in a direct way the final characteristics of the membrane after sintering, particularly the porosity and the diameter of the pores. The presence of heterogeneous particles size in the powder can lead to the reduction in the porosity and the homogeneity on the surface of the layer [<xref ref-type="bibr" rid="B8">8</xref>]. A monodisperse granulometric distribution is thus desirable for any raw material.</p>
        <p>Clay mineral was collected at a depth of about 1.5 m from a mining site located in Wack village, in the Adamawa region, at 50 km SW of Ngaoundere, Cameroon at an altitude of 708 m, latitude 07˚40.685 N and longitude 013˚33.026 E. Generally, it is known as Wack clay. The Wack clay is predominantly composed of silica and alumina with a small amount of Fe<sub>2</sub>O<sub>3</sub>, CaO, K<sub>2</sub>O, MgO and Na<sub>2</sub>O. The percentage of Al<sub>2</sub>O<sub>3</sub> corresponds to non-refractory clay since it does not exceed 45% [<xref ref-type="bibr" rid="B1">1</xref>]. The presence of a high level K<sub>2</sub>O confirms that it can be used as a melting material in our formulation [<xref ref-type="bibr" rid="B1">1</xref>].</p>
        <p>The Wack clay powder was crushed using a ceramic mortar and pistol and then sieved using a 50 µm sieve to obtain a homogenous clay powder. The final powder obtained from the sieved powder clay crushed above, has a granulometry which do not exceed the 50 µm. The percentage or proportion of clay used in the preparation of the slurry varies and it depends on the thickness of the deposited layer to be attained. To elaborate a microfiltration membrane of a few tenths of µm, the order of magnitude of mineral materials (clay) to be used is 10% [<xref ref-type="bibr" rid="B5">5</xref>]. In the case of this study we used a proportion of clay in the range 10% - 12 %.</p>
        <p><bold>The solvent:</bold></p>
        <p>Water is generally used as the solvent. This is because water has a low viscosity and allows the solubilisation of the organic additives. The water used in the preparation of the slurry is usually basic in the range of pH of 8 - 9, this in order to enhance repulsion between the powder particles and have a stable suspension. In our case we used water of pH 8.2 which was prepared by adjusting the pH with NaOH. The solvent here that acts as both a solvent and a dispersant.</p>
        <p><bold>Organic polymer (Binder):</bold></p>
        <p>It can be used both as a dispersant and binder while contributing to modify or adjust viscosity. It protects the membrane from cracks which generally appear during the drying and at the beginning of re-sintered. In our case we used Polyvinyl Alcohol (PVA). The PVA has a role of binder but also of plasticizer since it forms a thin film very elastic after drying. PVA is a hydrosoluble polymer of structure—(CH<sub>2</sub>-CHOH)<sub>n</sub>, with degree of polymerisation of 2000 and degree of hydrolysation of 86 - 89 mol%. It was prepared at 12% concentration [<xref ref-type="bibr" rid="B10">10</xref>]. The PVA was supplied by the department of Applied Chemistry of the University of Ngaoundere.</p>
        <p>2.1.2. Tubular Ceramic Membrane Support Layer</p>
        <p>The tubular ceramic membrane support layer shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> was elaborated by Yanu <italic>et al</italic><italic>.</italic> in 2020 and consist of optimal size and amount of raw materials of 66% Wack clay, 30% red sawdust and 4% binder for particle size of 100 µm elaborated by the extrusion technique. The tubular ceramic membrane support layer has geometrical configuration such as outer and inner diameters and length of the tube were 4 cm, 2 cm, and 19 cm, respectively. The sintered membrane possessed a porosity of 43.5%, water permeability of 244.9 L/h∙m<sup>2</sup> bar, an average pore size of 2.4 μm and mechanical strength of 9.2 MPa with very good corrosion resistance in acidic and basic conditions [<xref ref-type="bibr" rid="B1">1</xref>]. </p>
        <fig id="fig1">
          <label>Figure 1</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId17.jpeg?20260224013258" />
        </fig>
        <p><bold>Figure 1</bold><bold>.</bold> Tubular ceramic membrane support layer [<xref ref-type="bibr" rid="B1">1</xref>].</p>
      </sec>
      <sec id="sec2dot2">
        <title>2.2. Mixture Design with Constraint (Extreme Vertex Design)</title>
        <p>The synergetic effect of a combination of two or more components on a property of interest can be easily identified by means of a mixture design approach. In a mixture experimental design, the total amount is held constant and a measured property of the mixture changes when the proportions of the components of the mixture are changed. Therefore, the main purpose of using this methodology is to verify how the properties of interest are affected by the variation of the proportions of the mixture components [<xref ref-type="bibr" rid="B13">13</xref>]. The mixture experimental design generates a map of the response over a specified region of formulation. It is possible to discover the critical variables, to define mathematical models and by them, to optimize the process [<xref ref-type="bibr" rid="B14">14</xref>].</p>
        <p>Recall that the purpose of this work is to study the effect of three components, namely proportion of clay, proportion of binder and proportion of water on the viscosity of the clay slurry (suspensions). A mixture design with constraints (Extreme vertex designs) is used when there is a constraint on both the lower and upper bound of the proportions of raw materials present, or when linear constraints are added to several components. <bold>Table 1</bold> below gives the experimental domain of the components (raw materials) with their lower and higher bounds obtained from literature [<xref ref-type="bibr" rid="B6">6</xref>][<xref ref-type="bibr" rid="B10">10</xref>]. The constraint in our mixture design was at the level of the proportions of clay and binder which has to be maintained between 10% and 12% and between 11% and 22% respectively. This is because literature shows that proportions lower that the above values give thin and cracked layers while higher proportions values give thick non porous layers when the slurry is deposited on the ceramic support layer [<xref ref-type="bibr" rid="B5">5</xref>][<xref ref-type="bibr" rid="B10">10</xref>].</p>
        <p>In the case of three components, the factorial space constituted by all the possible fractions of the components is a triangle whose vertices correspond to pure components. In this design, the constraints define the area of the factor space that can be used as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. The relationship between the viscosity of the slurry and the components of the mixture can be represented using a polynomial mathematical model, as the sum of the components <inline-formula><mml:math display="inline"><mml:mrow><mml:mo> ∑ </mml:mo><mml:msub><mml:mi> X </mml:mi><mml:mi> j </mml:mi></mml:msub><mml:mo> = </mml:mo><mml:mtext></mml:mtext><mml:msub><mml:mi> X </mml:mi><mml:mn> 1 </mml:mn></mml:msub><mml:mo> + </mml:mo><mml:mtext></mml:mtext><mml:msub><mml:mi> X </mml:mi><mml:mn> 2 </mml:mn></mml:msub><mml:mo> + </mml:mo><mml:mo> ⋯ </mml:mo><mml:mo> + </mml:mo><mml:mtext></mml:mtext><mml:msub><mml:mi> X </mml:mi><mml:mi> q </mml:mi></mml:msub></mml:mrow></mml:math></inline-formula> must be 1 or equivalent to 100%. For three components, the Scheffe’s canonical special cubic model takes the following form [<xref ref-type="bibr" rid="B15">15</xref>]:</p>
        <disp-formula id="FD1">
          <label>(1)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>Y</mml:mi>
              <mml:mi>i</mml:mi>
              <mml:mtext>
              </mml:mtext>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mi>c</mml:mi>
                  <mml:mi>a</mml:mi>
                  <mml:mi>l</mml:mi>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mrow>
                  <mml:mn>12</mml:mn>
                </mml:mrow>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mrow>
                  <mml:mn>13</mml:mn>
                </mml:mrow>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mrow>
                  <mml:mn>23</mml:mn>
                </mml:mrow>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:msub>
                <mml:mi>b</mml:mi>
                <mml:mrow>
                  <mml:mn>123</mml:mn>
                </mml:mrow>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <italic>Yi</italic> (<italic>cal</italic>) is the calculated response value at the <italic>i</italic>th experiment, bi are the model coefficients, <italic>X</italic><sub>1</sub>, <italic>X</italic><sub>2</sub> and <italic>X</italic><sub>3</sub> represent the proportions of raw materials (wack clay, binder (PVA) and water) respectively. In the present research, a mixture design with 13 experiments was generated using the software Minitab version 2017 and Statgraphics plus software. The statistical experimental design as specified by the software as shown in <bold>Table 2</bold>.</p>
        <p><bold>Table 1</bold><bold>.</bold> Experimental domain for the raw materials.</p>
        <table-wrap id="tbl1">
          <label>Table 1</label>
          <table>
            <tbody>
              <tr>
                <td rowspan="2">
                  <bold>Components</bold>
                </td>
                <td rowspan="2">
                  <bold>Variables</bold>
                </td>
                <td colspan="2">
                  <bold>Levels/Variations</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>Lower (</bold>
                  <bold>−</bold>
                  <bold>1)</bold>
                </td>
                <td>
                  <bold>Higher (+1)</bold>
                </td>
              </tr>
              <tr>
                <td>Clay (%)</td>
                <td>
                  X
                  <sub>1</sub>
                </td>
                <td>10</td>
                <td>12</td>
              </tr>
              <tr>
                <td>Binder (PVA) (%)</td>
                <td>
                  X
                  <sub>2</sub>
                </td>
                <td>11</td>
                <td>22</td>
              </tr>
              <tr>
                <td>Water (%)</td>
                <td>
                  X
                  <sub>3</sub>
                </td>
                <td>66</td>
                <td>79</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <fig id="fig2">
          <label>Figure 2</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId22.jpeg?20260224013258" />
        </fig>
        <p><bold>Figure 2</bold><bold>.</bold> Distribution of the experimental points in the studied domain.</p>
        <p>Thus a mixture design with constraint with 3 factors gives a total number of experiments of 13 experiments. The total number of experience was determined using the equation below:</p>
        <disp-formula id="FD2">
          <label>(2)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>N</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:msup>
                    <mml:mn>2</mml:mn>
                    <mml:mi>p</mml:mi>
                  </mml:msup>
                  <mml:mo>+</mml:mo>
                  <mml:mn>2</mml:mn>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>+</mml:mo>
              <mml:mi>N</mml:mi>
              <mml:mi>o</mml:mi>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where, <italic>N</italic> = Number of experiments, <italic>p</italic> = Number of factors and <italic>No</italic> = Number of centre points.</p>
        <p><bold>Table 2</bold><bold>.</bold> Experimental matrix with the 13 formulations of the clay slurry.</p>
        <table-wrap id="tbl2">
          <label>Table 2</label>
          <table>
            <tbody>
              <tr>
                <td rowspan="2">S/N</td>
                <td colspan="3">Real Values</td>
                <td rowspan="2">Viscosity (Vep) mPa∙s</td>
              </tr>
              <tr>
                <td>Clay (%)</td>
                <td>Binder (%)</td>
                <td>Water (%)</td>
              </tr>
              <tr>
                <td>1</td>
                <td>11.0</td>
                <td>22.0</td>
                <td>67.0</td>
                <td rowspan="13">
                </td>
              </tr>
              <tr>
                <td>2</td>
                <td>11.5</td>
                <td>13.75</td>
                <td>74.75</td>
              </tr>
              <tr>
                <td>3</td>
                <td>12.0</td>
                <td>11.0</td>
                <td>77.0</td>
              </tr>
              <tr>
                <td>4</td>
                <td>10.0</td>
                <td>11.0</td>
                <td>79.00</td>
              </tr>
              <tr>
                <td>5</td>
                <td>12.0</td>
                <td>16.50</td>
                <td>71.5</td>
              </tr>
              <tr>
                <td>6</td>
                <td>11.5</td>
                <td>19.25</td>
                <td>69.25</td>
              </tr>
              <tr>
                <td>7</td>
                <td>10.5</td>
                <td>13.75</td>
                <td>75.75</td>
              </tr>
              <tr>
                <td>8</td>
                <td>12.0</td>
                <td>22.0</td>
                <td>66.0</td>
              </tr>
              <tr>
                <td>9</td>
                <td>11.0</td>
                <td>11.00</td>
                <td>78.00</td>
              </tr>
              <tr>
                <td>10</td>
                <td>10.5</td>
                <td>13.75</td>
                <td>75.75</td>
              </tr>
              <tr>
                <td>11</td>
                <td>10.0</td>
                <td>22.00</td>
                <td>68.0</td>
              </tr>
              <tr>
                <td>12</td>
                <td>11.0</td>
                <td>16.50</td>
                <td>72.5</td>
              </tr>
              <tr>
                <td>13</td>
                <td>10.5</td>
                <td>13.75</td>
                <td>75.75</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>Validation of the Models </p>
        <p>The empirical model obtained is validated by comparing the values of the answers envisaged and those observed. This will make it possible to predict the answers in the field defined for the study.</p>
        <p><bold>Linear regression coefficient (</bold><italic><bold>R</bold></italic><bold><sup>2</sup></bold><bold>)</bold></p>
        <p>The analysis of the variance makes it possible to calculate very useful statistics: <italic>R</italic><sup>2</sup> or R square. It indicates how well the model explains the variability of the response variable. A higher <italic>R</italic><sup>2</sup> value suggests a better fit, meaning the model can effectively capture the relationship in the data. These statistics are the ratio of the sum of squares of the calculated answers (corrected average) to the sum of squares of the measured answers (corrected average):</p>
        <disp-formula id="FD3">
          <label>(3)</label>
          <mml:math>
            <mml:mrow>
              <mml:msup>
                <mml:mi>R</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msup>
              <mml:mo>=</mml:mo>
              <mml:mo>
              </mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:mtext>corrected</mml:mtext>
                  <mml:mtext>
                     
                  </mml:mtext>
                  <mml:mtext>average sum of squares of the calculated answers</mml:mtext>
                </mml:mrow>
                <mml:mrow>
                  <mml:mtext>corrected average sum of squares of the measured answers</mml:mtext>
                </mml:mrow>
              </mml:mfrac>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>For the model to be valid, the <italic>R</italic><sup>2</sup> value has to be &gt;95%. In addition to the linear regression coefficient (<italic>R</italic><sup>2</sup>), other mathematical procedures and tools were used. The Absolute Average Deviation (<italic>AAD</italic>) and the Bias factor (Bf).</p>
        <p><bold>Absolute Average Deviation (</bold><italic><bold>AAD</bold></italic><bold>)</bold></p>
        <p>The absolute average deviation quantifies the average magnitude or errors in the model’s predictions, providing insights into the precision of the model. By analysing the <italic>AAD</italic>, we can determine how closely the model’s predictions, which is essential for validating the model’s usefulness in real-world scenarios. The absolute average deviation was determined using the formula below. For the model to be valid, the <italic>AAD</italic> has to be comprised between 0 ≤ <italic>AAD</italic> ≤ 0.2.</p>
        <disp-formula id="FD4">
          <label>(4)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>A</mml:mi>
              <mml:mi>A</mml:mi>
              <mml:mi>D</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:msubsup>
                    <mml:mstyle mathsize="140%" displaystyle="true">
                      <mml:mo>∑</mml:mo>
                    </mml:mstyle>
                    <mml:mrow>
                      <mml:mi>i</mml:mi>
                      <mml:mo>=</mml:mo>
                      <mml:mn>1</mml:mn>
                    </mml:mrow>
                    <mml:mi>p</mml:mi>
                  </mml:msubsup>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mrow>
                      <mml:mfrac>
                        <mml:mrow>
                          <mml:mrow>
                            <mml:mo>|</mml:mo>
                            <mml:mrow>
                              <mml:msub>
                                <mml:mi>Y</mml:mi>
                                <mml:mrow>
                                  <mml:mi>i</mml:mi>
                                  <mml:mi>e</mml:mi>
                                  <mml:mi>x</mml:mi>
                                  <mml:mi>p</mml:mi>
                                </mml:mrow>
                              </mml:msub>
                              <mml:mo>−</mml:mo>
                              <mml:msub>
                                <mml:mi>Y</mml:mi>
                                <mml:mrow>
                                  <mml:mi>i</mml:mi>
                                  <mml:mi>c</mml:mi>
                                  <mml:mi>a</mml:mi>
                                  <mml:mi>l</mml:mi>
                                </mml:mrow>
                              </mml:msub>
                            </mml:mrow>
                            <mml:mo>|</mml:mo>
                          </mml:mrow>
                        </mml:mrow>
                        <mml:mrow>
                          <mml:msub>
                            <mml:mi>Y</mml:mi>
                            <mml:mrow>
                              <mml:mi>i</mml:mi>
                              <mml:mi>e</mml:mi>
                              <mml:mi>x</mml:mi>
                              <mml:mi>p</mml:mi>
                            </mml:mrow>
                          </mml:msub>
                        </mml:mrow>
                      </mml:mfrac>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
                <mml:mi>p</mml:mi>
              </mml:mfrac>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>With: <italic>Y</italic><italic><sub>iexp</sub></italic> = experimental answer, <italic>Y</italic><italic><sub>ical</sub></italic> = calculated response starting from the model for an experiment <italic>I</italic>, and <italic>p</italic> = total number of experiments.</p>
        <p><bold>Bias factor (</bold><italic><bold>Bf</bold></italic><bold>)</bold></p>
        <p>The Bias factor measures the systematic error of the model’s prediction. A bias factor close to 1 indicates that the model’s predictions are unbiased and generally accurate. Assessing the bias helps identify whether the model consistently overestimates or underestimates the response, which is crucial for practical applications. The Bias factor was determined using the formula below. For the model to be valid, the Bias factor has to be ≤1.2.</p>
        <disp-formula id="FD5">
          <label>(5)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>B</mml:mi>
              <mml:mi>f</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:msup>
                <mml:mrow>
                  <mml:mn>10</mml:mn>
                </mml:mrow>
                <mml:mi>B</mml:mi>
              </mml:msup>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>The Bias (<italic>B</italic>) is given by the relation:</p>
        <disp-formula id="FD6">
          <label>(6)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>B</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mn>1</mml:mn>
                <mml:mi>n</mml:mi>
              </mml:mfrac>
              <mml:mo>
              </mml:mo>
              <mml:mo>∑</mml:mo>
              <mml:mi>log</mml:mi>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mrow>
                  <mml:mfrac>
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>Y</mml:mi>
                        <mml:mrow>
                          <mml:mi>t</mml:mi>
                          <mml:mi>h</mml:mi>
                          <mml:mi>e</mml:mi>
                          <mml:mi>o</mml:mi>
                        </mml:mrow>
                      </mml:msub>
                    </mml:mrow>
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>Y</mml:mi>
                        <mml:mrow>
                          <mml:mi>o</mml:mi>
                          <mml:mi>b</mml:mi>
                          <mml:mi>s</mml:mi>
                        </mml:mrow>
                      </mml:msub>
                    </mml:mrow>
                  </mml:mfrac>
                </mml:mrow>
                <mml:mo>)</mml:mo>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>MINITAB version 2017 and Statgraphics plus software were used to analyse the data obtained.</p>
      </sec>
      <sec id="sec2dot3">
        <title>2.3. Preparation of the Slurry</title>
        <p>From the component design mixture given in <bold>Table 2</bold> above we have 13 experiments (mixtures) with 3 components. In general, rheological behaviour of clay suspensions or slurry depends on many characteristics such as proportions and nature of clay, binder and pH of solution. For this reason and in order to understand the effect of proportion of clay, binder and water on the rheological behaviour of the slurry we have worked in constant conditions (pH, nature and experiment conditions). The protocol for the preparation of the slurry is as <xref ref-type="fig" rid="fig3">Figure 3</xref>:</p>
        <fig id="fig3">
          <label>Figure 3</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId33.jpeg?20260224013259" />
        </fig>
        <p><bold>Figure 3</bold><bold>.</bold> Process diagram for the preparation of Wack clay slurry [<xref ref-type="bibr" rid="B5">5</xref>].</p>
        <p>The 50 µm sieved wack clay powder is mixed first with an aqueous solution of the water at a constant pH of 8.2 and manually agitated for 5 minutes.The desagglomeration of the clay powder is done through ultrasounds agitation for 25 minutes at a power of 150 W.The binder (PVA) is then added and homogenized by magnetic agitation for 5 mins.It is then cooled under tap water and the viscosity of the slurry is determined. </p>
        <p>Measure of the Viscosity of the Clay Slurry</p>
        <p>The viscosity of the slurry should be sufficient such that the capillary adsorption of the slurry on the support should allow a uniform flow and coating without any infiltration into the depths of the support. Indeed, the viscosity of the suspension must be sufficient to prevent the fast formation of a thick and inhomogeneous layer related to a very fast absorption of solvent by the support. This viscosity must also make it possible for the solution to be run inside the support without difficulties. Generally, the viscosity and contact time slurry/support determines the thickness and homogeneity of the deposited layer [<xref ref-type="bibr" rid="B8">8</xref>].</p>
        <p>The dynamic viscosity was measured under the same conditions for all samples using the same cycle with a DV III Ultra Rheometer. The rheological test consists of measuring the shear stress, shear rate and viscosity of the clay slurry at the same turn per minutes (tpm) of 10, 30, 60, 100, 150, 200 and 250 and at ambient temperature (25˚ ± 1˚) and viscosity values, shear rate and shear stress are retained.</p>
        <p>The model of Herschel-Bulkley is the model that is mostly used to describe the behaviour of clay slurry. The viscosity of the prepared slurry has to follow the dynamics of the Herschel-Bulkley model with n &lt; 1, for it to be adapted for coating on the support [<xref ref-type="bibr" rid="B16">16</xref>]. The reduced viscosity at higher shear ensures that the slurry can penetrate into fine details of the support structure, leading to a more consistent and even coating.</p>
      </sec>
      <sec id="sec2dot4">
        <title>2.4. Coating Technique: Slip Casting of Clay Slurry over the Tubular Support Layer</title>
        <p>The technique used for coating of the clay is called slip casting. It consists is putting the support in a vertical position held by a clamp and stand while blocking one end of the tube in order to fill the support with the optimal slurry (suspension) obtained from the mixture design with constraint for a contact of time 2 minutes, 4 minutes and 6 minutes. At the end of each contact time, the support is emptied and then dried at ambient temperature for 24 h. It should be noted that when we carry out slip casting, the pores of the macro-porous membrane exert a capillary suction force which enables the powder particles to be deposited on the support. At the same time, water infiltrates itself into the pores of the membrane. When these pores are filled with water, there is no longer a force to hold the solid particles deposited on the porous support forming a layer with cracks which is not homogeneous. The thickness of the layer is controlled by the contact time slurry-support, the characteristics of the support (pore diameter and porosity) and that of the deposited slurry (concentration and viscosity).</p>
        <p>2.4.1. Drying and Thermal Treatment</p>
        <p>After draining, the membrane is dried at ambient temperature vertically in order to allow the total evacuation of the extra slip remaining in the support. The qualities of the layers are modified by a premature rise in the temperature. In our case, drying is done at ambient temperature during 24 hours. The thermal treatment which is an operation that allows the elimination of organic products and the sintering of the membrane ensures the consolidation of the layer, its adherence with the support and gives its final characteristics. It is the most important stage in the elaboration of the membranes that should be well mastered. The temperature platform and the speed of heating must allow the evolution of organic matter, then the diffusion of the matter between the grains thus supporting the consolidation. By taking into account the presence of water and organic materials in the slurry, we established an adequate program for sintering allowing us to obtain a membrane without defect. The platform at 250˚C corresponds to the departure of PVA. The program used is as follows: </p>
        <p>The final temperature of sintering (T<sub>f</sub>) and the final time of sintering (t<sub>f</sub>) are very important parameters when sintering the membrane for microfiltration. Indeed, it is general judicious to choose temperatures approximately 50˚C at 100˚C lower than the sintering temperature of the support layer, in order not to densifier the layer [<xref ref-type="bibr" rid="B5">5</xref>]. In our case T<sub>f</sub> was at 900˚C for a support layer membrane sintered at 950˚C as shown below.</p>
        <disp-formula id="FD7">
          <mml:math display="inline">
            <mml:mrow>
              <mml:msup>
                <mml:mrow>
                  <mml:mn>25</mml:mn>
                </mml:mrow>
                <mml:mo>∘</mml:mo>
              </mml:msup>
              <mml:mtext>C</mml:mtext>
              <mml:mover>
                <mml:mo>→</mml:mo>
                <mml:mrow>
                  <mml:mn>1</mml:mn>
                  <mml:mrow>
                    <mml:mrow>
                      <mml:msup>
                        <mml:mrow>
                        </mml:mrow>
                        <mml:mo>∘</mml:mo>
                      </mml:msup>
                      <mml:mtext>C</mml:mtext>
                    </mml:mrow>
                    <mml:mo>/</mml:mo>
                    <mml:mrow>
                      <mml:mi>min</mml:mi>
                    </mml:mrow>
                  </mml:mrow>
                </mml:mrow>
              </mml:mover>
              <mml:mrow>
                <mml:mrow>
                  <mml:msup>
                    <mml:mrow>
                      <mml:mn>25</mml:mn>
                    </mml:mrow>
                    <mml:mo>∘</mml:mo>
                  </mml:msup>
                  <mml:mtext>C</mml:mtext>
                </mml:mrow>
                <mml:mo>/</mml:mo>
                <mml:mrow>
                  <mml:mn>1</mml:mn>
                  <mml:mtext>h</mml:mtext>
                </mml:mrow>
              </mml:mrow>
              <mml:mover>
                <mml:mo>→</mml:mo>
                <mml:mrow>
                  <mml:mn>2</mml:mn>
                  <mml:mrow>
                    <mml:mrow>
                      <mml:msup>
                        <mml:mrow>
                        </mml:mrow>
                        <mml:mo>∘</mml:mo>
                      </mml:msup>
                      <mml:mtext>C</mml:mtext>
                    </mml:mrow>
                    <mml:mo>/</mml:mo>
                    <mml:mrow>
                      <mml:mi>min</mml:mi>
                    </mml:mrow>
                  </mml:mrow>
                </mml:mrow>
              </mml:mover>
              <mml:mrow>
                <mml:mrow>
                  <mml:msub>
                    <mml:mtext>T</mml:mtext>
                    <mml:mtext>f</mml:mtext>
                  </mml:msub>
                </mml:mrow>
                <mml:mo>/</mml:mo>
                <mml:mrow>
                  <mml:mn>2</mml:mn>
                  <mml:mtext>h</mml:mtext>
                </mml:mrow>
              </mml:mrow>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p><xref ref-type="fig" rid="fig4">Figure 4</xref> below shows the stages of the casting process of the clay slurry over the tubular support by slip casting and <xref ref-type="fig" rid="fig5">Figure 5</xref> shows the imagine of the slurry in the tubular support layer and when emptied and drying.</p>
        <fig id="fig4">
          <label>Figure 4</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId36.jpeg?20260224013301" />
        </fig>
        <p><bold>Figure 4</bold><bold>.</bold> Classic technique for depositing a suspension by slip casting.</p>
        <fig id="fig5">
          <label>Figure 5</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId37.jpeg?20260224013300" />
        </fig>
        <p><bold>Figure 5</bold><bold>.</bold> Casting of the slurry on a membrane for microfiltration: (a) Support with slurry and (b) Support coated with slurry.</p>
        <p>2.4.2. Determination of the Best Contact Time Relating to the Thickness and Homogeneity of the Deposited Filtration Layer</p>
        <p>The optimal proportion of the slurry obtained from the mixture design with constraint was cast into the tubular support for contact times of 2 minutes, 4 minutes and 6 minutes. The support was dried, sintered and then analysed using a scanning electron microscope (SEM Hitachi S-4500) in order to study the influence of contact time slurry/support and to determine the best optimal contact time with respect to the homogeneity and thickness of the deposited filtration layer. The contact time that gives a homogeneous layer with no cracks and a thickness of layer in the range 5 - 20 µm will be considered as the best contact time.</p>
        <p>2.4.3. Determination of the Level of Influence of the Proportion of Clay</p>
        <p>Proportions of clay of 10%, 11% and 12% was mixed with the optimal proportion of binder obtained from the mixture design with constraint and the corresponding proportion of water. The three mixtures were then cast into three tubular supports using the best contact time obtained from above. After drying and sintering of the tubular membrane, it was then analysed using a scanning electron microscope (SEM Hitachi S-4500) in order to study the level of influence of the proportion of clay on the thickness of the deposited filtration layer.</p>
        <p>2.4.4. Determination of the Level of Influence of the Proportion of PVA</p>
        <p>Proportions of binder of 11%, 16.5% and 22% was mixed with the optimal proportion of clay obtained from the mixture design with constraint and the corresponding proportion of water. The three mixtures were then cast into three tubular supports using the optimal contact time obtained from above. After drying and sintering of the tubular membrane, it was then analysed using a scanning electron microscope (SEM Hitachi S-4500) in order to study the level of influence of the proportion of PVA on the thickness of the deposited filtration layer.</p>
      </sec>
      <sec id="sec2dot5">
        <title>2.5. Characterisation of the Tubular Multilayer Membrane Properties</title>
        <p>The deposited layer was then characterized by determining some intrinsic properties of the tubular multilayer membrane. These properties are given below:</p>
        <p>2.5.1. Morphology and Thickness</p>
        <p>Scanning Electronic microscope (SEM) gives information of the surface and morphology of a massive sample. The scanning electronic microscope used in this work is a microscope at variable pressure (Hitachi S-4500). The analysed sampled was segment of the tubular multilayer membrane (surface and depth) which was snapped by the scanning electronic microscope which is equipped with a computer that has a software that treats the data in terms of sharpness and enlargement of the image that appears on the screen.</p>
        <p>2.5.2. Permeability</p>
        <p>The water permeability (L<sub>h</sub>) of the membrane was determined by distilled water flux at different applied pressures. It was evaluated from the slope of the pure water flux (J<sub>W</sub>) versus applied pressure across the membrane (ΔP).</p>
        <disp-formula id="FD8">
          <label>(7)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>J</mml:mi>
              <mml:mi>w</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:msub>
                <mml:mi>L</mml:mi>
                <mml:mi>h</mml:mi>
              </mml:msub>
              <mml:mi>Δ</mml:mi>
              <mml:mi>P</mml:mi>
              <mml:mo>
              </mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>2.5.3. Porosity</p>
        <p>The porosity of the tubular multilayer membrane is measured using the below expression [<xref ref-type="bibr" rid="B1">1</xref>] as described in the previous chapter:</p>
        <disp-formula id="FD9">
          <label>(8)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>P</mml:mi>
              <mml:mi>o</mml:mi>
              <mml:mi>r</mml:mi>
              <mml:mi>o</mml:mi>
              <mml:mi>s</mml:mi>
              <mml:mi>i</mml:mi>
              <mml:mi>t</mml:mi>
              <mml:mi>y</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mrow>
                <mml:mo>(</mml:mo>
                <mml:mi>%</mml:mi>
                <mml:mo>)</mml:mo>
              </mml:mrow>
              <mml:mo>=</mml:mo>
              <mml:mfrac>
                <mml:mrow>
                  <mml:mrow>
                    <mml:mo>(</mml:mo>
                    <mml:mrow>
                      <mml:msub>
                        <mml:mi>W</mml:mi>
                        <mml:mn>1</mml:mn>
                      </mml:msub>
                      <mml:mo>−</mml:mo>
                      <mml:msub>
                        <mml:mi>W</mml:mi>
                        <mml:mn>0</mml:mn>
                      </mml:msub>
                    </mml:mrow>
                    <mml:mo>)</mml:mo>
                  </mml:mrow>
                </mml:mrow>
                <mml:mrow>
                  <mml:msub>
                    <mml:mi>W</mml:mi>
                    <mml:mn>1</mml:mn>
                  </mml:msub>
                </mml:mrow>
              </mml:mfrac>
              <mml:mo>×</mml:mo>
              <mml:mn>100</mml:mn>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>It was done using the Archimedes method whereby the dry tubular multilayer filter is weighed (<italic>W</italic><sub>0</sub>) and put into water for about 4 h and then reweighed (<italic>W</italic><sub>1</sub>).</p>
        <p>2.5.4. Average Pore Size</p>
        <p>Hagen-Poiseuille equation was employed to estimate the average pore size of the tubular multilayer membrane by assuming pores are cylindrical in shape [<xref ref-type="bibr" rid="B1">1</xref>][<xref ref-type="bibr" rid="B17">17</xref>] as described in the previous chapter.</p>
        <disp-formula id="FD10">
          <label>(9)</label>
          <mml:math>
            <mml:mrow>
              <mml:mi>r</mml:mi>
              <mml:mo>
              </mml:mo>
              <mml:mo>=</mml:mo>
              <mml:msqrt>
                <mml:mrow>
                  <mml:mrow>
                    <mml:mo>[</mml:mo>
                    <mml:mrow>
                      <mml:mfrac>
                        <mml:mrow>
                          <mml:msub>
                            <mml:mi>L</mml:mi>
                            <mml:mi>h</mml:mi>
                          </mml:msub>
                          <mml:mo>
                          </mml:mo>
                          <mml:mn>8</mml:mn>
                          <mml:mi>μ</mml:mi>
                          <mml:mi>τ</mml:mi>
                          <mml:mi>l</mml:mi>
                        </mml:mrow>
                        <mml:mi>ε</mml:mi>
                      </mml:mfrac>
                    </mml:mrow>
                    <mml:mo>]</mml:mo>
                  </mml:mrow>
                </mml:mrow>
              </mml:msqrt>
              <mml:mo>
              </mml:mo>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where, ε is the porosity of the membranes, r is the pore radius of the membrane (m), <italic>l</italic> is the pore length which is generally taken as thickness of the membrane, <italic>τ</italic> is the tortuosity factor (generally used as 1), and μ is the viscosity of water (0.00089 Pa∙s).</p>
      </sec>
    </sec>
    <sec id="sec3">
      <title>3. Results and Discussion</title>
      <sec id="sec3dot1">
        <title>3.1. Optimization of the Viscosity of the Clay Slurry</title>
        <p>Thirteen mixtures of clay slurry were prepared according to the experimental conditions. The measured and calculated values for the viscosity of the slurry are given in <bold>Table 3</bold> below. <bold>Table 3</bold> below gives the values of the viscosities of the slurry in the experimental matrix which varies between 32.2 - 88.6 mPa∙s.</p>
        <p><bold>Table 3.</bold> Experimental design for the viscosity of the clay slurry.</p>
        <table-wrap id="tbl3">
          <label>Table 3</label>
          <table>
            <tbody>
              <tr>
                <td rowspan="2">S/N</td>
                <td colspan="3">Real Values</td>
                <td rowspan="2">Viscosity exp (Vep) mPa∙s</td>
                <td rowspan="2">Viscosity cal (Vcal) mPa∙s</td>
              </tr>
              <tr>
                <td>Clay (%)</td>
                <td>PVA (%)</td>
                <td>Water (%)</td>
              </tr>
              <tr>
                <td>1</td>
                <td>11.0</td>
                <td>22.0</td>
                <td>67.0</td>
                <td>66.5</td>
                <td>70.04</td>
              </tr>
              <tr>
                <td>2</td>
                <td>11.5</td>
                <td>13.75</td>
                <td>74.75</td>
                <td>43.4</td>
                <td>41.12</td>
              </tr>
              <tr>
                <td>3</td>
                <td>12.0</td>
                <td>11.0</td>
                <td>77.0</td>
                <td>32.3</td>
                <td>34.79</td>
              </tr>
              <tr>
                <td>4</td>
                <td>10.0</td>
                <td>11.0</td>
                <td>79.00</td>
                <td>38.2</td>
                <td>40.34</td>
              </tr>
              <tr>
                <td>5</td>
                <td>12.0</td>
                <td>16.50</td>
                <td>71.5</td>
                <td>56.0</td>
                <td>55.76</td>
              </tr>
              <tr>
                <td>6</td>
                <td>11.5</td>
                <td>19.25</td>
                <td>69.25</td>
                <td>62.0</td>
                <td>62.85</td>
              </tr>
              <tr>
                <td>7</td>
                <td>10.5</td>
                <td>13.75</td>
                <td>75.75</td>
                <td>50.8</td>
                <td>42.27</td>
              </tr>
              <tr>
                <td>8</td>
                <td>12.0</td>
                <td>22.0</td>
                <td>66.0</td>
                <td>88.6</td>
                <td>86.49</td>
              </tr>
              <tr>
                <td>9</td>
                <td>11.0</td>
                <td>11.00</td>
                <td>78.00</td>
                <td>36.8</td>
                <td>34.98</td>
              </tr>
              <tr>
                <td>10</td>
                <td>10.0</td>
                <td>13.75</td>
                <td>75.75</td>
                <td>40.7</td>
                <td>42.65</td>
              </tr>
              <tr>
                <td>11</td>
                <td>10.0</td>
                <td>22.00</td>
                <td>68.0</td>
                <td>61.3</td>
                <td>58.14</td>
              </tr>
              <tr>
                <td>12</td>
                <td>11.0</td>
                <td>16.50</td>
                <td>72.5</td>
                <td>45.2</td>
                <td>46.78</td>
              </tr>
              <tr>
                <td>13</td>
                <td>10.5</td>
                <td>13.75</td>
                <td>75.75</td>
                <td>43.5</td>
                <td>39.02</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
      </sec>
      <sec id="sec3dot2">
        <title>3.2. ANOVA and Validation of the Model</title>
        <p>The good quality of the fitted model was attested with analysis of the variance (ANOVA) as shown in <bold>Table 4</bold>. Indeed, this table shows that the sum of squares related to the regression was statistically significant when using the F-test at a 99.9% probability level, which suggests that the variation accounted by the model was significantly greater than the residual variation.</p>
        <p><bold>Table 4.</bold> ANOVA for the clay slurry.</p>
        <table-wrap id="tbl4">
          <label>Table 4</label>
          <table>
            <tbody>
              <tr>
                <td>Source</td>
                <td>Sum of squares</td>
                <td>Degree of freedom</td>
                <td>Mean square</td>
                <td>Rapport F</td>
                <td>Proba.</td>
              </tr>
              <tr>
                <td>Special-cubic</td>
                <td>2799.07</td>
                <td>6</td>
                <td>466.51</td>
                <td>37.04</td>
                <td>0.0002**</td>
              </tr>
              <tr>
                <td>Residual (total error)</td>
                <td>75.5712</td>
                <td>6</td>
                <td>12.59</td>
                <td>
                </td>
                <td>
                </td>
              </tr>
              <tr>
                <td>Total (corr.)</td>
                <td>2874.64</td>
                <td>12</td>
                <td>
                </td>
                <td>
                </td>
                <td>
                </td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>**Significant at the level 99.9%.</p>
        <p><bold>Validation of the model</bold></p>
        <p><bold>Table 5</bold> below gives the criterions of evaluation and validation of the model. The analyses of variance give an <italic>R</italic><sup>2</sup> value of 97.37% which is greater than 95% meaning the model explains 97.37% the variability of the viscosity of the clay slurry. The Bias factor is less than 1 implying that the model error (uncertainty of prediction) is less than a unit. The AAD equal to 0.003 implying that there is no great variability in the data (the data is not spread out) and since the AAD is small it implies that the average value is indicative of the other values within the data set thus the data in the set are close together. With all these criterions respecting the reference values, it can be concluded that the proposed model is valid (accepted) and will explain the variation in the viscosity of the clay slurry at a confident level 95%.</p>
        <p><bold>Table 5.</bold> Criterion of validation of the model.</p>
        <table-wrap id="tbl5">
          <label>Table 5</label>
          <table>
            <tbody>
              <tr>
                <td>
                  <bold>Validation indicator</bold>
                </td>
                <td>
                  <bold>Viscosity slurry</bold>
                </td>
                <td>
                  <bold>Reference value</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <italic>
                    <bold>R</bold>
                  </italic>
                  <bold>
                    <sup>2</sup>
                  </bold>
                </td>
                <td>97.37%</td>
                <td>&gt;95%</td>
              </tr>
              <tr>
                <td>
                  <italic>
                    <bold>R</bold>
                  </italic>
                  <bold>
                    <sup>2</sup>
                  </bold>
                  <bold>adjusted</bold>
                </td>
                <td>94.74%</td>
                <td>&gt;90%</td>
              </tr>
              <tr>
                <td>
                  <bold>AAD</bold>
                </td>
                <td>0.003</td>
                <td>0 ≤ AAD ≤ 0.2</td>
              </tr>
              <tr>
                <td>
                  <bold>Bias factor</bold>
                </td>
                <td>0.99989</td>
                <td>≤1.2</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>3.2.1. Experimental and Statistical Modeling</p>
        <p>It consists of a group of techniques used in establishing empirical study of the relationship between a response and several input variables. Interpretation starts with the calculation of the coefficients of the model. The coefficient of the model is represented in the <bold>Table 6</bold> below. The equation of the special cubic model for the viscosity of the slurry is given below:</p>
        <disp-formula id="FD11">
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>Y</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mn>206.39</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mn>23.27</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mn>6.89</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mn>3.13</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:mo>−</mml:mo>
              <mml:mn>2.90</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>−</mml:mo>
              <mml:mn>0.50</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mn>0.03</mml:mn>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>1</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>2</mml:mn>
              </mml:msub>
              <mml:msub>
                <mml:mi>X</mml:mi>
                <mml:mn>3</mml:mn>
              </mml:msub>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <italic>Y</italic> = viscosity of clay slurry; <italic>X</italic><sub>1</sub> = proportion of clay; <italic>X</italic><sub>2</sub> = proportion of binder; <italic>X</italic><sub>3</sub> = proportion of water.</p>
        <p><bold>Table 6.</bold> Coefficient of the model.</p>
        <table-wrap id="tbl6">
          <label>Table 6</label>
          <table>
            <tbody>
              <tr>
                <td>
                  <bold>Terms</bold>
                </td>
                <td>
                  <bold>Coefficient</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>1</sub>
                </td>
                <td>+206.39</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>2</sub>
                </td>
                <td>+23.27</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>3</sub>
                </td>
                <td>+6.89</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>1</sub>
                  <italic>X</italic>
                  <sub>2</sub>
                </td>
                <td>+3.13</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>1</sub>
                  <italic>X</italic>
                  <sub>3</sub>
                </td>
                <td>−2.90</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>2</sub>
                  <italic>X</italic>
                  <sub>3</sub>
                </td>
                <td>−0.50</td>
              </tr>
              <tr>
                <td>
                  <italic>X</italic>
                  <sub>1</sub>
                  <italic>X</italic>
                  <sub>2</sub>
                  <italic>X</italic>
                  <sub>3</sub>
                </td>
                <td>+0.03</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>From the table above, all of the coefficients of the principal parameters that is proportions of clay, binder and water have a positive effect on the viscosity of the slurry (increases the viscosity of the slurry). But the proportion of clay has the highest positive effect on the viscosity. This can be explained by the fact that the clay particles in the medium hinder the flow of liquid limiting their freedom of movement hence resulting in an increase in the viscosity of slurry. For the interactions, only the interaction proportion of clay-proportion of binder has a positive effect on the viscosity of the slurry. The presence of binder makes the concentrated clay particles in the medium to stick together due to its gluing and gelling effect which forms miscelles with the particles through the formation of hydrogen bonds, increasing in the viscosity of the clay slurry. The third order interaction between the proportions of clay, binder and water influences positive the viscosity of the slurry but it is significantly low. Since the proportion of the clay has the highest individual effect and its interactions are low, it implies that the proportion of the clay is the component to follow as it influences significantly the viscosity. This is better seen and explained using the cox’s diagram below.</p>
        <p>3.2.2. Cox’s Diagram (Contribution of the Various Factors)</p>
        <p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows the response trace of the viscosity of the clay slurry using a reference mixture S the centroïd of the simplex domain (<italic>X</italic><sub>1</sub> = 14.33, <italic>X</italic><sub>2</sub> = 15.33, <italic>X</italic><sub>3</sub> = 70.33). In this figure, the vertical axis is the predicted response and the horizontal axis is the incremental change in each component. The reference mixture is shown as the point 0.00 on the horizontal axis. Each component is represented by one curve. </p>
        <p>From the diagram below it is observed that the blue curve for the effect of the proportion of clay changes significantly, this means it has a significant effect (increases) along its axial. This is explained by the fact that the clay particles are closely packed and their interaction hinders the freedom of movement of the fluid in the medium hence increasing the viscosity of clay slurry [<xref ref-type="bibr" rid="B15">15</xref>]. Meanwhile the red curve for the effect of the proportion of binder is almost flat; this means when the proportion of binder changes and other components kept fixed, the viscosity does not change very much. The pink curve for the effect of proportion of water is between component clay and binder and decreases along the axis. This is due to the dilution effect of water which breaks the links between the clay layers enhancing repulsion between them thus decreasing the viscosity of slurry [<xref ref-type="bibr" rid="B18">18</xref>].</p>
        <fig id="fig6">
          <label>Figure 6</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId46.jpeg?20260224013310" />
        </fig>
        <p><bold>Figure 6</bold><bold>.</bold> Cox’s Diagram using a reference mixture S domain (<italic>X</italic><sub>1</sub> = 14.33, <italic>X</italic><sub>2</sub> = 15.33, <italic>X</italic><sub>3</sub> = 70.33).</p>
        <p>3.2.3. Iso-Response Curve</p>
        <p>Following the validation of the model, it was used to generate response surface as a contour plot or a three dimensional surface plot over the explored domain as shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. The shaded area in red shows the optimal zone in the domain of study for the viscosity of the clay slurry. In order to evaluate the contribution of each of the three components and to determine the optimal values of each, the response trace technique is used [<xref ref-type="bibr" rid="B19">19</xref>]. In practice, the response trace is a plot of the estimated response value as we move away from a reference mixture and along the component axes.</p>
        <p>Recall that in ceramic industry, clay slurry used for coating support must have a low viscosity in the range 25 - 100 mPa∙s in order to facilitate the adhesion of the slurry on the support by capillary suction [<xref ref-type="bibr" rid="B5">5</xref>][<xref ref-type="bibr" rid="B8">8</xref>][<xref ref-type="bibr" rid="B10">10</xref>]. The contour plot (iso-response diagram) in <xref ref-type="fig" rid="fig8">Figure 8</xref> indicates that formulations which correspond to this requirement (viscosity &lt; 100 mPa∙s) are mixtures rich in water and binder with a small amount of clay. The optimal zone from the domain of study corresponds to the area with viscosity between 32.2 - 88.6 mPa∙s (shaded portion in red). The optimal zone falls within the experimental domain midpoint between the proportion of binder and water and a decrease in the proportion of clay.</p>
        <fig id="fig7">
          <label>Figure 7</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId47.jpeg?20260224013310" />
        </fig>
        <p><bold>Figure 7</bold><bold>.</bold> Experimental domain and the Iso-response diagram.</p>
        <p><bold>Table 7</bold> gives the optimal values of the proportions of clay, binder and water for the clay slurry. It is a formulation with low values of clay and binder but higher values of water. The optimal viscosity of 40.4 mPa∙s is obtained with lower proportions of clay and binder and a higher proportion of water. This is because high proportions of clay and binder lead to an increase in the viscosity of slurry which is not needed for the coating of the slurry over the support leading to thick and fragile layers. The optimal viscosity of the slurry is found within this viscosity range making it good for adhesion over the support by capillary suction.</p>
        <p><bold>Table 7.</bold> Optimal proportion of raw materials for the clay slurry.</p>
        <table-wrap id="tbl7">
          <label>Table 7</label>
          <table>
            <tbody>
              <tr>
                <td>
                  <bold>Proportions (%)</bold>
                </td>
                <td>
                  <bold>Optimum</bold>
                </td>
              </tr>
              <tr>
                <td>
                  <bold>Clay</bold>
                </td>
                <td>10</td>
              </tr>
              <tr>
                <td>
                  <bold>PVA</bold>
                </td>
                <td>11</td>
              </tr>
              <tr>
                <td>
                  <bold>Water</bold>
                </td>
                <td>79</td>
              </tr>
              <tr>
                <td>
                  <bold>Viscosity (mPa</bold>
                  <bold>∙</bold>
                  <bold>s)</bold>
                </td>
                <td>40.4</td>
              </tr>
            </tbody>
          </table>
        </table-wrap>
        <p>3.2.4. Flow Index of the Optimal Clay Slurry</p>
        <p>The Herschel-Bulkley model was used to describe the rheological behaviour of the optimal clay slurry. The model is given by the equation below where n is the flow index.</p>
        <disp-formula id="FD12">
          <label>(10)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>τ</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:msub>
                <mml:mi>τ</mml:mi>
                <mml:mi>o</mml:mi>
              </mml:msub>
              <mml:mo>+</mml:mo>
              <mml:mi>k</mml:mi>
              <mml:msup>
                <mml:mtext>ý</mml:mtext>
                <mml:mi>n</mml:mi>
              </mml:msup>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <disp-formula id="FD13">
          <label>(11)</label>
          <mml:math display="inline">
            <mml:mrow>
              <mml:mi>n</mml:mi>
              <mml:mo>=</mml:mo>
              <mml:mi>log</mml:mi>
              <mml:mfrac>
                <mml:mrow>
                  <mml:mi>τ</mml:mi>
                  <mml:mo>−</mml:mo>
                  <mml:msub>
                    <mml:mi>τ</mml:mi>
                    <mml:mi>o</mml:mi>
                  </mml:msub>
                </mml:mrow>
                <mml:mi>k</mml:mi>
              </mml:mfrac>
              <mml:mo>−</mml:mo>
              <mml:mi>log</mml:mi>
              <mml:mi>y</mml:mi>
            </mml:mrow>
          </mml:math>
        </disp-formula>
        <p>where <italic>k</italic> is the consistence of the fluid, <inline-formula><mml:math><mml:mi> τ </mml:mi></mml:math></inline-formula> is shear stress and <inline-formula><mml:math><mml:mi> ý </mml:mi></mml:math></inline-formula> is the shear stress, n the flow index (<italic>n</italic> &lt; 1 the fluid is shear thinning; <italic>n</italic> &gt; 1 the fluid is shear thickening).</p>
        <p>Flow index of the optimal slurry (<italic>n</italic>) was 0.79 (<italic>n</italic> &lt; 1) which is characteristic of a pseudoplastic fluids thus stable during the casting period. The flow curve of the optimal clay slurry is shown in <xref ref-type="fig" rid="fig8">Figure 8</xref> below. From the curve it is observe that as the shear rate increases, the viscosity decreases. This can be explained by the fact that the particle-particle interactions in the slurry are broken down causing a random movement of particles, reducing fluid flow and thus the viscosity of the slurry. This brings about a non-Newtonian, shear thinning behaviour such that the viscosity decreases when shear is increased. The shear-thinning behaviour of slurries enhances their flow characteristics, improves the coating process, reduces defects and allows for more efficient production [<xref ref-type="bibr" rid="B16">16</xref>].</p>
        <fig id="fig8">
          <label>Figure 8</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId56.jpeg?20260224013311" />
        </fig>
        <p><bold>Figure 8</bold><bold>.</bold> Rheogram of the optimal clay slurry.</p>
      </sec>
      <sec id="sec3dot3">
        <title>3.3. Influence of Contact Time on the Properties of the Filtration Layer (Homogeneity and Thickness of Layer)</title>
        <p><xref ref-type="fig" rid="fig9">Figure 9</xref> below shows the variation of the homogeneity and thickness of the deposited layer with respect to contact time. Looking at the surface view for the evolution of the homogeneity of the layer with respect with time, it is observed from the <xref ref-type="fig" rid="fig10">Figure 10</xref> below that as the contact time increases from 2 minutes to 6 minutes there is the gradual appearance of cracks. Meanwhile, looking at the cross-section view for the evolution of the thickness of the layers, it is observed that as the contact time increases from 2 minutes to 6 minutes, the thickness of the deposited layer also increases from 8.8 µm to 23 µm. The gradual appearance of cracks and the increase in the thickness of the deposited layer with time can be explained by the fact that as the contact time increases from 2 to 6 minutes, there is an increases in capillary suction of the slurry onto the support which leads to the formation of a heterogeneous compressible deposit which becomes thicker but fragile with time (appearance of cracks) due to saturation of the pores. With extended contact time, particles in the slurry have more time to rearrange and pack more efficiently. This leads to a reduction in the overall porosity and permeability as the particles settle more tightly together [<xref ref-type="bibr" rid="B3">3</xref>][<xref ref-type="bibr" rid="B6">6</xref>][<xref ref-type="bibr" rid="B10">10</xref>]. With the specifications set on the properties of the deposited layer for it to be homogenous (no cracks) and have a thickness comprised between 5 - 15 µm, the contact time of 2 minutes was chosen as the best as it gave homogenous layer with thickness of 8.8 µm. </p>
        <fig id="fig9">
          <label>Figure 9</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId57.jpeg?20260224013312" />
        </fig>
        <p><bold>Figure 9</bold><bold>.</bold> (a) Surface and (b) cross-section view for the evolution of the homogeneity and thickness of deposited layer with respect to contact time (clay 10%; binder 11%; water/dispersant 79%).</p>
        <p>3.3.1. Determination of the Level of Influence of the Proportion of Clay on the Thickness of the Deposited Layer</p>
        <p><xref ref-type="fig" rid="fig10">Figure 10</xref> below shows the variation of the thickness of the deposited layer with respect to the proportion of clay. The mineral content in the slurry (clay in our case), influences the thickness of the deposited layer at fixed contact time (best). It was noted during this work that at a fixed contact time of 2 minutes and using the optimal proportion of binder and water of 11% and 79% respectively, the thickness of the deposited layer support increases from 8.8 µm to 29.7 µm with an increase in the proportion of clay from 10% to 12%. This can be explained by the fact that as the proportion of clay increases, there is an increase in sedimentation and accumulation of the clay on the surface of the support by capillary suction of the clay particles in the slurry. </p>
        <fig id="fig10">
          <label>Figure 10</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId58.jpeg?20260224013312" />
        </fig>
        <p><bold>Figure 10</bold><bold>.</bold> Evolution of the thickness of the filtration layer with respect to the proportion of clay (Clay 10%; 11%; 12%, binder 11%, water 79% at contact time 2 minutes).</p>
        <p>3.3.2. Determine of the Level of Influence of the Proportion of Binder on the Thickness of the Deposited Layer</p>
        <p><xref ref-type="fig" rid="fig11">Figure 11</xref> below shows the variation of the thickness of the deposited layer with respect to the proportion of binder. The proportion of binder also influences the thickness of the deposited layer for a fixed contact time of 2 minutes, optimal proportion of clay of 10% and proportion of water of 79%. It was observed here that the thickness of the deposited layer increases from 8.8 µm to 35.0 µm as the proportion of the binder increases from 11% to 22%. This is explained by the fact that as the proportion of binder increases, it leads to an increase in the formation of the clay aggregate due to the gelling and gluing effect of the binder. This causes the clay particles to settle on the surface of the support thus increasing the thickness of the layer. </p>
        <fig id="fig11">
          <label>Figure 11</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId59.jpeg?20260224013313" />
        </fig>
        <p><bold>Figure 11</bold><bold>.</bold> Evolution of the thickness of the deposited layer with respect to the proportion of Binder (PVA 11%; 16.5%; 22%. Contact time 2 minutes, Clay 10% and water 79%).</p>
      </sec>
      <sec id="sec3dot4">
        <title>3.4. Characteristics of the Tubular Multilayer Membrane</title>
        <p>3.4.1. Porosity</p>
        <p>The porosity of the fired deposited filtration layer membrane was found to be 32.6%, which is in accordance with values reported in the literature for microfiltration membranes. The porosity of the tubular multilayer ceramic membrane is greater than 30% and this is due to disappearance of the binder as from 250˚C.</p>
        <p>3.4.2. Permeability</p>
        <p><xref ref-type="fig" rid="fig12">Figure 12</xref> illustrates the water flux of the fired deposited filtration layer membrane as a function of the different applied pressures. It can be noticed that the water flux increases linearly with an increase of applied pressures (0.5 - 3 bar). This stipulates that the variation in pressure is the barely driving force for permeation. For transportation operation exclusively by convection, the flow rate is proportionate to the pressure, and is in accordance with Darcy’s law. The water permeability (L<sub>h</sub>) of the tubular multilayer membrane was determined from the graph of water flux against different applied pressures. The gradient of this plot gives the permeability of the membrane. The water permeability (L<sub>h</sub>) of the tubular multilayer membrane was found to be 305.67 L/h∙m<sup>2</sup>bar which is in the domain for microfiltration (greater than 300 L/h∙m<sup>2</sup>∙bar).</p>
        <fig id="fig12">
          <label>Figure 12</label>
          <graphic xlink:href="https://html.scirp.org/file/1741438-rId60.jpeg?20260224013315" />
        </fig>
        <p><bold>Figure 12</bold><bold>.</bold> Determination of water permeability of the tubular multilayer membrane.</p>
        <p>3.4.3. Average Pore Size</p>
        <p>The average pore size of the fired tubular multilayer membrane was calculated to be 0.48 µm (0.48 × 10<sup>−</sup><sup>6</sup> m). The multilayer membrane is macroporous and adapted for microfiltration. Similar results were obtained by [<xref ref-type="bibr" rid="B20">20</xref>]. </p>
        <p>3.4.4. Chemical Resistance</p>
        <p>The corrosion resistance test was performed with respect to weight decrement of the membrane after keeping in harsh environments (acid and alkali). The weight decrement of the membrane is calculated to be 0.38% in acidic condition and 0.17% in alkali condition. In acid and alkali conditions, the membrane displays an excellent result in resisting corrosion. The loss of weight is &lt;3% indicating the support is stable chemically. The obtained results are more commensurable in comparison with the cordierite membrane fabricated by [<xref ref-type="bibr" rid="B21">21</xref>].</p>
      </sec>
    </sec>
    <sec id="sec4">
      <title>4. Conclusion</title>
      <p>The objective of this work was to elaborate and coat a filtration layer (tubular multilayer) from wack clay by the slip casting technique applied in water treatment. In order to do these, two objectives were set. The first objective was to determine the optimal formulation of raw materials (clay, binder and water) on the viscosity of the slurry using a mixture design with constraint. It resulted from this objective that the optimum formulation of the slurry is obtained at lower values of clay and binder (10% and 11%) but at higher values of water (79%) because high proportions of clay and binder lead to an increase in the viscosity of slurry which is not needed for the coating of the slurry over the support leading to thick and fragile layers. The interaction proportion of clay-proportion of binder has a positive effect on the viscosity of the slurry as the binder causes the concentrated clay particles within the medium to stick together through hydrogen bond links (its gelling and gluing effect) thus increasing the resistance of flow of the slurry. The optimal proportion of clay, binder and water was 10%, 11% and 79% respectively with optimal viscosity of the clay slurry was found to be 40.4 mPa∙s. The second objective was to determine the best contact time to have the required homogeneity and thickness of the filtration layer. It resulted from this objective that contact times of 2 minutes give the best compromise relating to the homogeneity and the thickness of the filtration layer giving a homogenous layer with thickness of 8.8 µm. This is so because higher contact times lead to thick and fragile (appearance of cracks) layers. The tubular multilayer membrane filter sintered at 900˚C, gave a membrane of porosity of 32.6%, permeability of 305.67 L/h∙m<sup>2</sup>bar, average pore diameter of 0.48 µm which is chemically stable and is adapted for microfiltration.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <title>References</title>
      <ref id="B1">
        <label>1.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Yanu, C.A., Sieliechi, J.M. and Ngassoum, M.B. (2020) Optimization of Ceramic Paste Viscosity Use for the Elaboration of Tubular Membrane Support by Extrusion and Its Application. <italic>Journal</italic><italic>of</italic><italic>Materials</italic><italic>Science</italic><italic>and</italic><italic>Chemical</italic><italic>Engineering</italic>, 8, 1-22. https://doi.org/10.4236/msce.2020.83001 <pub-id pub-id-type="doi">10.4236/msce.2020.83001</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.4236/msce.2020.83001">https://doi.org/10.4236/msce.2020.83001</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Yanu, C.A.</string-name>
              <string-name>Sieliechi, J.M.</string-name>
              <string-name>Ngassoum, M.B.</string-name>
            </person-group>
            <year>2020</year>
            <article-title>Optimization of Ceramic Paste Viscosity Use for the Elaboration of Tubular Membrane Support by Extrusion and Its Application</article-title>
            <source>Journal of Materials Science and Chemical Engineering</source>
            <volume>8</volume>
            <pub-id pub-id-type="doi">10.4236/msce.2020.83001</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B2">
        <label>2.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Nguiamba, N., Yanu, C.A., Belibi, P.D.B., Sieliechi, J.M. and Ngassoum, M.B. (2021) Identification of an Appropriate Formulation for Domestic Water Ceramic Filters from Soukamna Clay (Cameroon). <italic>Journal</italic><italic>of</italic><italic>Metallic</italic><italic>Material</italic><italic>Research</italic>, 4, 12-18. https://doi.org/10.30564/jmmr.v4i1.3462 <pub-id pub-id-type="doi">10.30564/jmmr.v4i1.3462</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.30564/jmmr.v4i1.3462">https://doi.org/10.30564/jmmr.v4i1.3462</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Nguiamba, N.</string-name>
              <string-name>Yanu, C.A.</string-name>
              <string-name>Belibi, P.D.B.</string-name>
              <string-name>Sieliechi, J.M.</string-name>
              <string-name>Ngassoum, M.B.</string-name>
            </person-group>
            <year>2021</year>
            <article-title>Identification of an Appropriate Formulation for Domestic Water Ceramic Filters from Soukamna Clay (Cameroon)</article-title>
            <source>Journal of Metallic Material Research</source>
            <volume>4</volume>
            <pub-id pub-id-type="doi">10.30564/jmmr.v4i1.3462</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B3">
        <label>3.</label>
        <citation-alternatives>
          <mixed-citation publication-type="thesis">Ndiapa Wandji Fabrice (2020) Elaboration des membranes minérales multicouches de microfiltration contenant des nanoparticules d’argent pour le traitement de l’eau de consummation. Mémoire de soutenance du Doctorate/PhD en chimie industrielle de l’université de Ngaoundere.</mixed-citation>
          <element-citation publication-type="thesis">
            <year>2020</year>
            <article-title>Elaboration des membranes minérales multicouches de microfiltration contenant des nanoparticules d’argent pour le traitement de l’eau de consummation</article-title>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B4">
        <label>4.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Belibi Belibi, P., Nguemtchouin, M.M.G., Rivallin, M., Ndi Nsami, J., Sieliechi, J., Cerneaux, S., <italic>et al</italic>. (2015) Microfiltration Ceramic Membranes from Local Cameroonian Clay Applicable to Water Treatment. <italic>Ceramics</italic><italic>International</italic>, 41, 2752-2759. https://doi.org/10.1016/j.ceramint.2014.10.090 <pub-id pub-id-type="doi">10.1016/j.ceramint.2014.10.090</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.ceramint.2014.10.090">https://doi.org/10.1016/j.ceramint.2014.10.090</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Belibi, P.</string-name>
              <string-name>Nguemtchouin, M.M.G.</string-name>
              <string-name>Rivallin, M.</string-name>
              <string-name>Nsami, J.</string-name>
              <string-name>Sieliechi, J.</string-name>
              <string-name>Cerneaux, S.</string-name>
            </person-group>
            <year>2015</year>
            <article-title>Microfiltration Ceramic Membranes from Local Cameroonian Clay Applicable to Water Treatment</article-title>
            <source>Ceramics International</source>
            <volume>41</volume>
            <pub-id pub-id-type="doi">10.1016/j.ceramint.2014.10.090</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B5">
        <label>5.</label>
        <citation-alternatives>
          <mixed-citation publication-type="confproc">Roseline, E. (2017) Matériaux membranaires en TiO <sub>2</sub> sous-stœchiométrique pour le traitement de l’eau par procédé d’oxydation avancée électrochimique Pour obtenir le grade de DOCTEUR de l’Université de MONTPELIER II Soutenue le 17 Novembre 2017.</mixed-citation>
          <element-citation publication-type="confproc">
            <person-group person-group-type="author">
              <string-name>Roseline, E.</string-name>
            </person-group>
            <year>2017</year>
            <article-title>Matériaux membranaires en TiO2 sous-stœchiométrique pour le traitement de l’eau par procédé d’oxydation avancée électrochimique Pour obtenir le grade de DOCTEUR de l’Université de MONTPELIER II Soutenue le 17 Novembre 2017</article-title>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B6">
        <label>6.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Iaich, S. and Messaoudi, L. (2014) Mise au point et caractérisation des membranes minérales de microfiltration déposées sur des supports céramiques tubulaires à base d’une. <italic>Journal of Materials and Environmental Science</italic>, 5, 1808-1815.</mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Iaich, S.</string-name>
              <string-name>Messaoudi, L.</string-name>
            </person-group>
            <year>2014</year>
            <article-title>Mise au point et caractérisation des membranes minérales de microfiltration déposées sur des supports céramiques tubulaires à base d’une</article-title>
            <source>Journal of Materials and Environmental Science</source>
            <volume>5</volume>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B7">
        <label>7.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Vinoth Kumar, R., Kumar Ghoshal, A. and Pugazhenthi, G. (2015) Elaboration of Novel Tubular Ceramic Membrane from Inexpensive Raw Materials by Extrusion Method and Its Performance in Microfiltration of Synthetic Oily Wastewater Treatment. <italic>Journal</italic><italic>of</italic><italic>Membrane</italic><italic>Science</italic>, 490, 92-102. https://doi.org/10.1016/j.memsci.2015.04.066 <pub-id pub-id-type="doi">10.1016/j.memsci.2015.04.066</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.memsci.2015.04.066">https://doi.org/10.1016/j.memsci.2015.04.066</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Kumar, R.</string-name>
              <string-name>Ghoshal, A.</string-name>
              <string-name>Pugazhenthi, G.</string-name>
            </person-group>
            <year>2015</year>
            <article-title>Elaboration of Novel Tubular Ceramic Membrane from Inexpensive Raw Materials by Extrusion Method and Its Performance in Microfiltration of Synthetic Oily Wastewater Treatment</article-title>
            <source>Journal of Membrane Science</source>
            <volume>490</volume>
            <pub-id pub-id-type="doi">10.1016/j.memsci.2015.04.066</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B8">
        <label>8.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Chen, Z., Li, J., Liu, C., Liu, Y., Zhu, J. and Lao, C. (2019) Preparation of High Solid Loading and Low Viscosity Ceramic Slurries for Photopolymerization-Based 3D Printing. <italic>Ceramics</italic><italic>International</italic>, 45, 11549-11557. https://doi.org/10.1016/j.ceramint.2019.03.024 <pub-id pub-id-type="doi">10.1016/j.ceramint.2019.03.024</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.ceramint.2019.03.024">https://doi.org/10.1016/j.ceramint.2019.03.024</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Chen, Z.</string-name>
              <string-name>Li, J.</string-name>
              <string-name>Liu, C.</string-name>
              <string-name>Liu, Y.</string-name>
              <string-name>Zhu, J.</string-name>
              <string-name>Lao, C.</string-name>
            </person-group>
            <year>2019</year>
            <article-title>Preparation of High Solid Loading and Low Viscosity Ceramic Slurries for Photopolymerization-Based 3D Printing</article-title>
            <source>Ceramics International</source>
            <volume>45</volume>
            <pub-id pub-id-type="doi">10.1016/j.ceramint.2019.03.024</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B9">
        <label>9.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Papadopoulou, A., Gillissen, J.J.J., Tiwari, M.K. and Balabani, S. (2020) Effect of Particle Specific Surface Area on the Rheology of Non-Brownian Silica Suspensions. <italic>Materials</italic>, 13, Article No. 4628. https://doi.org/10.3390/ma13204628 <pub-id pub-id-type="doi">10.3390/ma13204628</pub-id><pub-id pub-id-type="pmid">33081380</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3390/ma13204628">https://doi.org/10.3390/ma13204628</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Papadopoulou, A.</string-name>
              <string-name>Gillissen, J.J.J.</string-name>
              <string-name>Tiwari, M.K.</string-name>
              <string-name>Balabani, S.</string-name>
            </person-group>
            <year>2020</year>
            <article-title>Effect of Particle Specific Surface Area on the Rheology of Non-Brownian Silica Suspensions</article-title>
            <source>Materials</source>
            <volume>13</volume>
            <elocation-id>No</elocation-id>
            <pub-id pub-id-type="doi">10.3390/ma13204628</pub-id>
            <pub-id pub-id-type="pmid">33081380</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B10">
        <label>10.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Ghouil, B., Harabi, A., Bouzerara, F. and Brihi, N. (2016) Elaboration and Characterization of Ceramic Membrane Supports from Raw Materials Used in Microfiltration. <italic>Desalination</italic><italic>and</italic><italic>Water</italic><italic>Treatment</italic>, 57, 5241-5245. https://doi.org/10.1080/19443994.2015.1021098 <pub-id pub-id-type="doi">10.1080/19443994.2015.1021098</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1080/19443994.2015.1021098">https://doi.org/10.1080/19443994.2015.1021098</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Ghouil, B.</string-name>
              <string-name>Harabi, A.</string-name>
              <string-name>Bouzerara, F.</string-name>
              <string-name>Brihi, N.</string-name>
            </person-group>
            <year>2016</year>
            <article-title>Elaboration and Characterization of Ceramic Membrane Supports from Raw Materials Used in Microfiltration</article-title>
            <source>Desalination and Water Treatment</source>
            <volume>57</volume>
            <pub-id pub-id-type="doi">10.1080/19443994.2015.1021098</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B11">
        <label>11.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Ha, J., Lee, S., Abbas Bukhari, S.Z., Choi, J.R., Lee, J., Song, I., <italic>et al</italic>. (2017) Preparation and Characterization of Alumina-Coated Silicon Carbide Supports. <italic>Ceramics</italic><italic>International</italic>, 43, 9481-9487. https://doi.org/10.1016/j.ceramint.2017.04.126 <pub-id pub-id-type="doi">10.1016/j.ceramint.2017.04.126</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.ceramint.2017.04.126">https://doi.org/10.1016/j.ceramint.2017.04.126</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Ha, J.</string-name>
              <string-name>Lee, S.</string-name>
              <string-name>Bukhari, S.Z.</string-name>
              <string-name>Choi, J.R.</string-name>
              <string-name>Lee, J.</string-name>
              <string-name>Song, I.</string-name>
            </person-group>
            <year>2017</year>
            <article-title>Preparation and Characterization of Alumina-Coated Silicon Carbide Supports</article-title>
            <source>Ceramics International</source>
            <volume>43</volume>
            <pub-id pub-id-type="doi">10.1016/j.ceramint.2017.04.126</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B12">
        <label>12.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Habib, B.A., Abd El-Samiae, A.S., El-Houssieny, B.M. and Tag, R. (2021) Formulation, Characterization, Optimization, and <italic>in</italic>- <italic>Vivo</italic> Performance of Febuxostat Self-Nano-Emulsifying System Loaded Sublingual Films. <italic>Drug</italic><italic>Delivery</italic>, 28, 1321-1333. https://doi.org/10.1080/10717544.2021.1927247 <pub-id pub-id-type="doi">10.1080/10717544.2021.1927247</pub-id><pub-id pub-id-type="pmid">34176376</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1080/10717544.2021.1927247">https://doi.org/10.1080/10717544.2021.1927247</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Habib, B.A.</string-name>
              <string-name>El-Samiae, A.S.</string-name>
              <string-name>El-Houssieny, B.M.</string-name>
              <string-name>Tag, R.</string-name>
              <string-name>Formulation, C</string-name>
            </person-group>
            <year>2021</year>
            <article-title>Formulation, Characterization, Optimization, and in-Vivo Performance of Febuxostat Self-Nano-Emulsifying System Loaded Sublingual Films</article-title>
            <source>Drug Delivery</source>
            <volume>28</volume>
            <pub-id pub-id-type="doi">10.1080/10717544.2021.1927247</pub-id>
            <pub-id pub-id-type="pmid">34176376</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B13">
        <label>13.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Tayefi, M., Razavi-Nouri, M. and Sabet, A. (2020) Using Constrained Mixture Design Method for Optimizing the Properties of Organoclay Filled Ethylene-Octene Copolymer Nanocomposites. <italic>Materials</italic><italic>Research</italic><italic>Express</italic>, 7, Article ID: 015321. https://doi.org/10.1088/2053-1591/ab61aa <pub-id pub-id-type="doi">10.1088/2053-1591/ab61aa</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1088/2053-1591/ab61aa">https://doi.org/10.1088/2053-1591/ab61aa</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Tayefi, M.</string-name>
              <string-name>Razavi-Nouri, M.</string-name>
              <string-name>Sabet, A.</string-name>
            </person-group>
            <year>2020</year>
            <article-title>Using Constrained Mixture Design Method for Optimizing the Properties of Organoclay Filled Ethylene-Octene Copolymer Nanocomposites</article-title>
            <source>Materials Research Express</source>
            <volume>7</volume>
            <fpage>015321</fpage>
            <elocation-id>ID</elocation-id>
            <pub-id pub-id-type="doi">10.1088/2053-1591/ab61aa</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B14">
        <label>14.</label>
        <citation-alternatives>
          <mixed-citation publication-type="report">Natoli, C. (2020) An Introduction to Mixture Design, Statcoe-Report-11-2020.1871-1874.</mixed-citation>
          <element-citation publication-type="report">
            <person-group person-group-type="author">
              <string-name>Natoli, C.</string-name>
              <string-name>Design, S</string-name>
            </person-group>
            <year>2020</year>
            <article-title>An Introduction to Mixture Design, Statcoe-Report-11-2020</article-title>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B15">
        <label>15.</label>
        <citation-alternatives>
          <mixed-citation publication-type="book">Myers and Raymond, H. (2016) Response Surface Methodology; Process and Pro-duction Optimization Using Designed Experiments. 4th Edition, John Willey and Sons, Inc.</mixed-citation>
          <element-citation publication-type="book">
            <person-group person-group-type="author">
              <string-name>Raymond, H.</string-name>
              <string-name>Edition, J</string-name>
              <string-name>Sons, I</string-name>
            </person-group>
            <year>2016</year>
            <article-title>Response Surface Methodology; Process and Pro-duction Optimization Using Designed Experiments</article-title>
            <source>4th Edition</source>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B16">
        <label>16.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Bates, B.M. and Ancey, C. (2017) The Dam-Break Problem for Eroding Viscoplastic Fluids. <italic>Journal</italic><italic>of</italic><italic>Non-Newtonian</italic><italic>Fluid</italic><italic>Mechanics</italic>, 243, 64-78. https://doi.org/10.1016/j.jnnfm.2017.01.009 <pub-id pub-id-type="doi">10.1016/j.jnnfm.2017.01.009</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.jnnfm.2017.01.009">https://doi.org/10.1016/j.jnnfm.2017.01.009</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Bates, B.M.</string-name>
              <string-name>Ancey, C.</string-name>
            </person-group>
            <year>2017</year>
            <article-title>The Dam-Break Problem for Eroding Viscoplastic Fluids</article-title>
            <source>Journal of Non-Newtonian Fluid Mechanics</source>
            <volume>243</volume>
            <pub-id pub-id-type="doi">10.1016/j.jnnfm.2017.01.009</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B17">
        <label>17.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Basumatary, A.K., Kumar, R.V., Ghoshal, A.K. and Pugazhenthi, G. (2015) Synthesis and Characterization of MCM-41-Ceramic Composite Membrane for the Separation of Chromic Acid from Aqueous Solution. <italic>Journal</italic><italic>of</italic><italic>Membrane</italic><italic>Science</italic>, 475, 521-532. https://doi.org/10.1016/j.memsci.2014.10.055 <pub-id pub-id-type="doi">10.1016/j.memsci.2014.10.055</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.memsci.2014.10.055">https://doi.org/10.1016/j.memsci.2014.10.055</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Basumatary, A.K.</string-name>
              <string-name>Kumar, R.V.</string-name>
              <string-name>Ghoshal, A.K.</string-name>
              <string-name>Pugazhenthi, G.</string-name>
            </person-group>
            <year>2015</year>
            <article-title>Synthesis and Characterization of MCM-41-Ceramic Composite Membrane for the Separation of Chromic Acid from Aqueous Solution</article-title>
            <source>Journal of Membrane Science</source>
            <volume>475</volume>
            <pub-id pub-id-type="doi">10.1016/j.memsci.2014.10.055</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B18">
        <label>18.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Sarkar, P., Ghimire, S., Vlasov, S. and Mukhopadhyay, K. (2023) Effect of Clay-Zwitterionic Interactions in Controlling the Viscoelastic Properties in Organomodified Clays. <italic>iScience</italic>, 26, Article ID: 108388. https://doi.org/10.1016/j.isci.2023.108388 <pub-id pub-id-type="doi">10.1016/j.isci.2023.108388</pub-id><pub-id pub-id-type="pmid">38047072</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1016/j.isci.2023.108388">https://doi.org/10.1016/j.isci.2023.108388</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Sarkar, P.</string-name>
              <string-name>Ghimire, S.</string-name>
              <string-name>Vlasov, S.</string-name>
              <string-name>Mukhopadhyay, K.</string-name>
            </person-group>
            <year>2023</year>
            <article-title>Effect of Clay-Zwitterionic Interactions in Controlling the Viscoelastic Properties in Organomodified Clays</article-title>
            <source>iScience</source>
            <volume>26</volume>
            <fpage>108388</fpage>
            <elocation-id>ID</elocation-id>
            <pub-id pub-id-type="doi">10.1016/j.isci.2023.108388</pub-id>
            <pub-id pub-id-type="pmid">38047072</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B19">
        <label>19.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Habib, B.A., Abdeltawab, N.F. and Salah Ad-Din, I. (2022) D-Optimal Mixture Design for Optimization of Topical Dapsone Niosomes: <italic>In Vitro</italic> Characterization and <italic>in Vivo</italic> Activity against <italic>Cutibacterium</italic><italic>acnes</italic>. <italic>Drug</italic><italic>Delivery</italic>, 29, 821-836. https://doi.org/10.1080/10717544.2022.2048131 <pub-id pub-id-type="doi">10.1080/10717544.2022.2048131</pub-id><pub-id pub-id-type="pmid">35266431</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1080/10717544.2022.2048131">https://doi.org/10.1080/10717544.2022.2048131</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Habib, B.A.</string-name>
              <string-name>Abdeltawab, N.F.</string-name>
              <string-name>Ad-Din, I.</string-name>
            </person-group>
            <year>2022</year>
            <article-title>D-Optimal Mixture Design for Optimization of Topical Dapsone Niosomes: In Vitro Characterization and in Vivo Activity against Cutibacterium acnes</article-title>
            <source>Drug Delivery</source>
            <volume>29</volume>
            <pub-id pub-id-type="doi">10.1080/10717544.2022.2048131</pub-id>
            <pub-id pub-id-type="pmid">35266431</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B20">
        <label>20.</label>
        <citation-alternatives>
          <mixed-citation publication-type="journal">Das, D., Baitalik, S., Haldar, B., Saha, R. and Kayal, N. (2017) Preparation and Characterization of Macroporous Sic Ceramic Membrane for Treatment of Waste Water. <italic>Journal</italic><italic>of</italic><italic>Porous</italic><italic>Materials</italic>, 25, 1183-1193. https://doi.org/10.1007/s10934-017-0528-5 <pub-id pub-id-type="doi">10.1007/s10934-017-0528-5</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1007/s10934-017-0528-5">https://doi.org/10.1007/s10934-017-0528-5</ext-link></mixed-citation>
          <element-citation publication-type="journal">
            <person-group person-group-type="author">
              <string-name>Das, D.</string-name>
              <string-name>Baitalik, S.</string-name>
              <string-name>Haldar, B.</string-name>
              <string-name>Saha, R.</string-name>
              <string-name>Kayal, N.</string-name>
            </person-group>
            <year>2017</year>
            <article-title>Preparation and Characterization of Macroporous Sic Ceramic Membrane for Treatment of Waste Water</article-title>
            <source>Journal of Porous Materials</source>
            <volume>25</volume>
            <pub-id pub-id-type="doi">10.1007/s10934-017-0528-5</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
      <ref id="B21">
        <label>21.</label>
        <citation-alternatives>
          <mixed-citation publication-type="other">Jarrar, R., Abbas, M.K.G. and Al-Ejji, M. (2024) Environmental Remediation and the Efficacy of Ceramic Membranes in Wastewater Treatment—A Review. <italic>Emergent</italic><italic>Materials</italic>, 7, 1295-1327. https://doi.org/10.1007/s42247-024-00687-0 <pub-id pub-id-type="doi">10.1007/s42247-024-00687-0</pub-id><ext-link ext-link-type="uri" xlink:href="https://doi.org/10.1007/s42247-024-00687-0">https://doi.org/10.1007/s42247-024-00687-0</ext-link></mixed-citation>
          <element-citation publication-type="other">
            <person-group person-group-type="author">
              <string-name>Jarrar, R.</string-name>
              <string-name>Abbas, M.K.G.</string-name>
              <string-name>Al-Ejji, M.</string-name>
            </person-group>
            <year>2024</year>
            <article-title>Environmental Remediation and the Efficacy of Ceramic Membranes in Wastewater Treatment—A Review</article-title>
            <source>Emergent Materials</source>
            <volume>7</volume>
            <pub-id pub-id-type="doi">10.1007/s42247-024-00687-0</pub-id>
          </element-citation>
        </citation-alternatives>
      </ref>
    </ref-list>
  </back>
</article>