<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJIC</journal-id><journal-title-group><journal-title>Open Journal of Inorganic Chemistry</journal-title></journal-title-group><issn pub-type="epub">2161-7406</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojic.2021.111001</article-id><article-id pub-id-type="publisher-id">OJIC-106719</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Adsorption of Tartrazine onto Activated Carbon Based Cola Nuts Shells: Equilibrium, Kinetics, and Thermodynamics Studies
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Dantio</surname><given-names>Nguela Christian Brice</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ngomo</surname><given-names>Horace Manga</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Bénédoué</surname><given-names>Serge Arnold</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kouotou</surname><given-names>Daouda</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Abega</surname><given-names>Aimé Victoire</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ndongo</surname><given-names>Ndongo Alain Giresse</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Che</surname><given-names>Randy Nangah</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ndi</surname><given-names>Julius Nsami</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Laboratory of Applied Physical and Analytical Chemistry, Department of Inorganic Chemistry, Faculty of Science, University of Yaoundé I, Yaoundé, Cameroon</addr-line></aff><pub-date pub-type="epub"><day>25</day><month>01</month><year>2021</year></pub-date><volume>11</volume><issue>01</issue><fpage>1</fpage><lpage>19</lpage><history><date date-type="received"><day>7,</day>	<month>August</month>	<year>2020</year></date><date date-type="rev-recd"><day>22,</day>	<month>January</month>	<year>2021</year>	</date><date date-type="accepted"><day>25,</day>	<month>January</month>	<year>2021</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The uptake of tartrazine from its aqueous solution by powdered activated carbon prepared from cola nut shells chemically activated with potassium hydroxide (ACK) and phosphoric acid (ACP) has been investigated using kinetics models. Batch isotherm data were analysed with the pseudo-first order, pseudo-second order model as well as the intraparticle diffusion model. For structural elucidation, the materials were characterized using FTIR, XRD and SEM. These analyses revealed that the activated carbons (ACK and ACP) were predominantly mesoporous with several oxygen-containing functional groups dispersed on their surface. The reaction was systematically investigated under various experimental conditions such as contact time, adsorbent dose and pH. For the two adsorbents, the quantity adsorbed of 19.256 mg/g and 18.196 mg/g respectively for ACP and ACK at respective contact times of 5 and 10 min were obtained. The adsorption data were tested with the Langmuir, Freundlich models. Langmuir model was found to best describe the adsorption of tartrate ions with maximum monolayer adsorption capacities of 24.57 and 21.59 mg/g for ACP and ACK, respectively. Results analysis indicated clearly that the pseudo-second order kinetic rate model best fitted the experimental data and therefore was the adsorption controlling mechanism for both adsorbents. Thermodynamic studies revealed that the adsorption process was spontaneous and exothermic for ACP with increased randomness at the solid solution interface, then exothermic but non-spontaneous for ACK. The results show that these activated carbons could be an alternative for more costly adsorbents for the purpose of tartrate ions elimination.
 
</p></abstract><kwd-group><kwd>Cola Nuts Shells</kwd><kwd> Activated Carbon</kwd><kwd> Adsorption</kwd><kwd> Tartrazine</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Though industrial activities have contributed to the development of many countries, they have also generated undesirable by-products, which constitute the main part of the discharged effluents. These industrial effluents are organic (dyes, pesticides) and inorganic (heavy metals) pollutants. Owing to their appearance, coloured organic compounds are easily recognizable pollutants. These chemical pollutants in industrial effluents are mostly non-biodegradable and highly toxic as they affect aquatic ecosystems, destroy wildlife and affect human health, provoking conditions such as rashes, allergic reactions, dysfunction of the kidney, the reproductive system and the central nervous system in humans [<xref ref-type="bibr" rid="scirp.106719-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.106719-ref2">2</xref>].</p><p>Dye under investigation, tartrazine (otherwise known as E102 or FD &amp; C Yellow 5), is a lemon yellow azo dye manufactured from coal-tar derivative and used as a food colouring. It is found in certain brands of fruit squash, fruit cordial, coloured fizzy drinks, instant puddings, cake mixes, custard powder, soups, sauces, ice cream, ice lollies, sweets, chewing gum, marzipan, jam, jelly, marmalade, mustard, yoghurt and many convenience foods [<xref ref-type="bibr" rid="scirp.106719-ref3">3</xref>]. It is cheaper than beta-carotene and therefore used as an alternative to beta-carotene to achieve similar colour [<xref ref-type="bibr" rid="scirp.106719-ref4">4</xref>]. Water-soluble tartrazine is used in drugs, especially shells of medicinal capsules, syrups and cosmetics. The wide use of tartrazine in industry and its water-soluble nature maximize its chances to be found as contaminant in industrial effluents [<xref ref-type="bibr" rid="scirp.106719-ref5">5</xref>]. Tartrazine is also reputed to catalyse hyperactivity [<xref ref-type="bibr" rid="scirp.106719-ref6">6</xref>]. and other behavioural problems [<xref ref-type="bibr" rid="scirp.106719-ref7">7</xref>], asthma [<xref ref-type="bibr" rid="scirp.106719-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.106719-ref9">9</xref>], migraines, thyroid cancer [<xref ref-type="bibr" rid="scirp.106719-ref10">10</xref>]. According to WHO, the acceptable daily intake (ADI) of tartrazine is 7.5 mg/kg of body mass, which classifies it as a very toxic substance. It is therefore important to treat wastewaters containing tartrazine before their injection into the environment.</p><p>Many methods including chemical precipitation, filtration, ion exchange, reverse osmosis, ultra-filtration, biological degradation, membrane separation, solvent extraction and adsorption have been employed to remove pollutants. Adsorption remains the most utilised process because of its simplicity, high efficiency and easy recovery [<xref ref-type="bibr" rid="scirp.106719-ref11">11</xref>]. In the scientific literature, typical adsorbents include zeolite, clay, silica gel, resins, activated alumina and activated carbon [<xref ref-type="bibr" rid="scirp.106719-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.106719-ref13">13</xref>]. Activated carbon (AC) is the most widely used owing to its well-developed pore structure, large active surface area, good mechanical properties and multiple functional groups at their surface [<xref ref-type="bibr" rid="scirp.106719-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.106719-ref15">15</xref>]. There are many precursors from which AC can be prepared some of these include corn cobs [<xref ref-type="bibr" rid="scirp.106719-ref2">2</xref>], apricot stone [<xref ref-type="bibr" rid="scirp.106719-ref16">16</xref>], sugarcane bagasse, coconut shells [<xref ref-type="bibr" rid="scirp.106719-ref17">17</xref>], peanut hull [<xref ref-type="bibr" rid="scirp.106719-ref18">18</xref>], rattan bamboo, sawdust [<xref ref-type="bibr" rid="scirp.106719-ref19">19</xref>], hazelnut bagasse [<xref ref-type="bibr" rid="scirp.106719-ref20">20</xref>], cotton stalk fibre [<xref ref-type="bibr" rid="scirp.106719-ref1">1</xref>], rice husk [<xref ref-type="bibr" rid="scirp.106719-ref21">21</xref>], cola nut shell [<xref ref-type="bibr" rid="scirp.106719-ref11">11</xref>], and olive stone [<xref ref-type="bibr" rid="scirp.106719-ref22">22</xref>].</p><p>The goal of the present study, is to evaluate the adsorption capacities of activated carbon prepared from cola nut shells activated separately with KOH and H<sub>3</sub>PO<sub>4</sub> to remove tartrazine from aqueous solution using batch system and to get an insight into the adsorption controlling mechanism by testing the experimental data with well-known linear and nonlinear kinetic models applied to liquid phase adsorption.</p></sec><sec id="s2"><title>2. Experimental Methods</title><sec id="s2_1"><title>2.1. Preparation of Absorbents</title><p>The procedure for the preparation of the activated carbon (AC) used in this work has-been reported by [<xref ref-type="bibr" rid="scirp.106719-ref23">23</xref>]. The raw material constituted by kola nut shell was collected in the region of the Northwest Cameroon, more exactly in the department of Donga-Mantum; these cola nut shells are classified in the group of lignocellulosic compounds. These shells contain essentially organic, mineral substances and water, thus constitute a real source of agricultural waste, possessing interesting physico-chemical characteristics for the production of activated charcoals.</p><p>The kola nut shells collected are abundantly washed in the current water to eliminate the impurities, rinsed in the distilled water and then dried in air during two weeks. Once dried, they are crushed until the obtaining of fragments having a size between 1.25 and 2.5 mm. These fragments are impregnated with the potassium hydroxide (KOH) and the phosphoric acid (H<sub>3</sub>PO<sub>4</sub>) with a ratio of 1:1 (mass activing agent/mass of raw material).</p><p>After impregnation, these fragments of cola nut shells were dried in the oven room at 110˚C during 24 hours. The carbonization of material was made at 500˚C during 1 hour and cool down until the room temperature.</p><p>After cooling, the activated carbon was washed with distilled water until neutral pH was obtained, then crushed in a mortar by means of a pestle, until the obtaining of the powder.</p><sec id="s2_1_1"><title>2.1.1. Characterization of Activated Carbons</title><p>Samples of activated carbon were characterised using various techniques: Infrared spectroscopy (IR) to probe the surface functional group, Scanning Electron Microscopy (SEM) to investigate the surface morphology, X-ray diffraction (XRD) analysis was to evaluate the crystalline or amorphous structure and the BET method to determine the specific surface area. The iodine number was determined to evaluate the microporosity.</p></sec><sec id="s2_1_2"><title>2.1.2. Preparation of Adsorbate</title><p>The tartrazine stock solution (60 ppm) was prepared by dissolving 0.015 g of tartrazine powder with distilled water in a 250 mL volumetric flask. The solution was stirred for 24 hours to obtain the homogeneity. From this solution, dilute solutions of 1, 3, 5, 7, 9, 11, 13 and 15 mg/L were prepared. 0.1 M hydrochloric acid and 0.1 M sodium hydroxide were also prepared for pH adjustments, by dilution of initial hydrochloric acid of 37% and 2 g of sodium hydroxide in conical flasks.</p></sec></sec><sec id="s2_2"><title>2.2. Batch Adsorption Experiments</title><p>Batch adsorption isotherm study was carried out through several experimental runs. For each run, 20 ml of tartrazine dye of known initial concentration was added to a known mass of adsorbent and agitated for a predetermined time. After agitation, the solution was filtered using which wattman N˚4 filtered paper and the concentration of the supernatant fluid measured using a TECHMEL-TECHMEL S-23A UV-visible spectrophotometer at the wave length of 420 nm. Similar measurements were carried out with varying adsorbent doses, solution pH and initial concentrations of tartrazine.</p><p>The quantity adsorbed (Q<sub>e</sub>) adsorbed per unit mass of adsorbent, and the percentage removal (% R) were calculated using the following equations:</p><p>Q e = ( C 0 − C e ) V m (1)</p><p>R = ( C 0 − C e ) 100 C 0 (2)</p><p>where C<sub>0</sub> is the initial concentration, C<sub>e</sub> the equilibrium concentration, V the volume and m is the mass of the adsorbent.</p></sec></sec><sec id="s3"><title>3. Results and Discussion</title><sec id="s3_1"><title>3.1. On the Characterization of Adsorbent</title><sec id="s3_1_1"><title>3.1.1. Powder X-Ray Diffraction Analysis</title><p>The XRD spectrum of AC recorded between 5 to 70 degrees is presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The region between 7 and 70 degrees indicates the absence of any crystalline structure with the absence of any well-defined peak, which is an indication of an amorphous structure</p><p>This result is in good agreement with the nature of activated carbon prepared by others researchers reported in literature.</p></sec><sec id="s3_1_2"><title>3.1.2. Infrared Spectroscopy Analysis of ACK and ACP</title><p>The FT-IR spectroscopy analysis allows identifying functional groups present on the adsorbents surface. <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref> below shows the FT-IR spectra of both AC before adsorption:</p><p>On the recorded spectra, there are bands at 3321 cm<sup>−</sup><sup>1</sup> and 1574 cm<sup>−</sup><sup>1</sup> corresponding to O-H and C=C stretching vibration of phenolic and aromatic rings, respectively. The bands at 1416 and 1371 cm<sup>−</sup><sup>1</sup> are attributed to the N-H of amines and C-H of benzene bending vibration of respectively; the band at 1163 cm<sup>−</sup><sup>1</sup> cis attributed to C-O stretching vibration, whereas the bands at 873, 802 and 753 cm<sup>−</sup><sup>1</sup> correspond to the C-H stretching vibration of benzene para, meta and ortho-substituted, respectively. The frequencies at of 573, 538 and 515 cm<sup>−</sup><sup>1</sup> are attributed to the O-K stretching vibration coming from the AC activation by KOH.</p><p>On the ACP spectra the bands which appear at 3297 and 1581 cm<sup>−</sup><sup>1</sup> are attributed to O-H and C=C stretching vibration of phenolic and aromatic rings, respectively. The bands at 1416 and 1337 cm<sup>−</sup><sup>1</sup> correspond to N-H of amines and C-H of benzene bending vibration respectively. The band at 1101 cm<sup>−</sup><sup>1</sup> is attributed to C-O stretching vibration, whereas the bands at 872, 778 and 753 cm<sup>−</sup><sup>1</sup> correspond to the C-H stretching vibration of benzene para, meta and ortho-substituted, respectively. The frequencies at of 506, 397 and 387 cm<sup>−</sup><sup>1</sup> are due to the O-P stretching vibration coming from the AC activation by H<sub>3</sub>PO<sub>4</sub> [<xref ref-type="bibr" rid="scirp.106719-ref24">24</xref>].</p></sec><sec id="s3_1_3"><title>3.1.3. SEM Microstructural Analysis of ACP and ACK</title><p>To view the effect of activation on the pore structure of the precursor, SEM micrographs of the precursor before activation and after activation (ACP and ACK) were carried out. <xref ref-type="fig" rid="fig4">Figure 4</xref> illustrates the micrograph of the precursor before activation.</p><p>It is observed that the pores on the surface of the precursor are less developed. This poor pore distribution on its surface makes the precursor an unlikely candidate as an adsorbent. Nevertheless, activation could result to the presence surface functional groups which favoured ion exchange and increased porosity. <xref ref-type="fig" rid="fig5">Figure 5</xref> in turn displays the surfaces of the activated carbons ACP and ACK.</p><p>Compared to the micrograph of the precursor (<xref ref-type="fig" rid="fig4">Figure 4</xref>), the micrographs of ACP and ACK show a highly developed porosity over the entire sample surface resulting from the effect of chemical activation by phosphoric acid and potassium hydroxide. The pores are heterogeneous and not evenly distributed. It can also be seen that the pores of ACK are larger than those of ACP, but ACP has a more developed distribution of pores. This could explain the higher surface area for ACP than ACK (as seen in the BET results below).</p></sec><sec id="s3_1_4"><title>3.1.4. Textural Properties of ACP and ACK</title><p>The textural properties of ACP and ACK were determined by the BET nitrogen adsorption-desorption, BJH analysis and the iodine number. These parameters are shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The pore diameter of ACP and ACK is between 2 and 50 nm, indicating that both materials are mesoporous. Interestingly, the mean pore size of ACK is bigger than that of ACP in good agreement with SEM analysis. The value of the iodine number (513.945 mg/g) for ACK is within the 500 and 1200 mg/g range and indicates the presence of micropores.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Textural properties of the ACP and ACK [<xref ref-type="bibr" rid="scirp.106719-ref23">23</xref>]</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Analysis</th><th align="center" valign="middle" >ACP</th><th align="center" valign="middle" >ACK</th></tr></thead><tr><td align="center" valign="middle" >BET specific surface area (m<sup>2</sup>/g)</td><td align="center" valign="middle" >6.276</td><td align="center" valign="middle" >2.045</td></tr><tr><td align="center" valign="middle" >Pore adsorption cumulative surface area (m<sup>2</sup>/g)</td><td align="center" valign="middle" >3.255</td><td align="center" valign="middle" >0.992</td></tr><tr><td align="center" valign="middle" >Pore desorption cumulative surface area (m<sup>2</sup>/g)</td><td align="center" valign="middle" >0.992</td><td align="center" valign="middle" >2.672</td></tr><tr><td align="center" valign="middle" >Total pore volume (cm<sup>3</sup>/g)</td><td align="center" valign="middle" >0.009</td><td align="center" valign="middle" >0.005</td></tr><tr><td align="center" valign="middle" >Average pore diameter (&#197;)</td><td align="center" valign="middle" >61.000</td><td align="center" valign="middle" >94.000</td></tr><tr><td align="center" valign="middle" >Iodine Number (mg/g)</td><td align="center" valign="middle" >441.612</td><td align="center" valign="middle" >513.945</td></tr></tbody></table></table-wrap></sec></sec><sec id="s3_2"><title>3.2. Adsorption</title><p>All adsorption experiments were carried out at pH 2 because at pH greater than or less than 2, the adsorbed quantities were near to zero. The same results was obtained by Sushmita Banerjee [<xref ref-type="bibr" rid="scirp.106719-ref25">25</xref>] during the Adsorption characteristics for the removal of a toxic dye, tartrazine from aqueous solutions by a low cost agricultural by-product. They found that tartrazine was better adsorbed under acid medium.</p><sec id="s3_2_1"><title>3.2.1. Influence of Contact Time</title><p><xref ref-type="fig" rid="fig6">Figure 6</xref> exhibits the effect of contact time on the adsorption of tartrazine and the experiments were tested by carrying out experimental runs from 5 to 70 min for ACP and ACK, at an initial tartrazine concentration of 20 mg/L, and with a mass of 0.01 g of ACP and ACK.</p><p>The adsorption of tartrazine is seen to rise steadily from 0 to 5 minutes with adsorbed quantities of 19.42 mg/L for ACP and 17.84 mg/L for ACK. This initial spurt may be due to the availability of adsorption sites on the surface of adsorbent materials [<xref ref-type="bibr" rid="scirp.106719-ref16">16</xref>]. After this time, the system is seen to attain equilibrium with the saturation of the active sites of both absorbents. This equilibrium is attained after 5 mins for ACP and 10 mins for ACK.</p></sec><sec id="s3_2_2"><title>3.2.2. Influence of the Mass of Adsorbent</title><p><xref ref-type="fig" rid="fig7">Figure 7</xref> below displays the influence of the adsorbent mass varying from 0.01 g to 0.06 g, at a contact time of 5 min for ACP and 10 mins for ACK and adsorbate dose of 20 mg/L.</p><p>From <xref ref-type="fig" rid="fig7">Figure 7</xref>, the amount adsorbed at equilibrium decreases as the mass of both adsorbents (ACK and ACP) is increased. At higher adsorbent mass, agglomeration of the adsorbent particles occurs due to electrostatic attractive forces between the AC particles. This impedes access to adsorption sites, hence the decrease in adsorbed quantity. This may be also due to the fact that as the amount of the adsorbent increases, the total surface area available for the adsorption of tartrazine molecules reduces as a result of the overlapping or aggregation of adsorption sites [<xref ref-type="bibr" rid="scirp.106719-ref26">26</xref>]. Similar results were obtained by [<xref ref-type="bibr" rid="scirp.106719-ref27">27</xref>] in the study of the adsorption of zinc ions on rice balls [<xref ref-type="bibr" rid="scirp.106719-ref17">17</xref>]. Maximum adsorption was thus recorded at a mass of 0.01 g.</p></sec><sec id="s3_2_3"><title>3.2.3. Influence of Initial Concentration</title><p>The initial concentration of the adsorbate was varied between 5 and 30 mg/L. As seen from <xref ref-type="fig" rid="fig8">Figure 8</xref>, the quantity of tartrazine adsorbed increases from 6.01 to 18.04 mg/g and from 6.4 to 18.19 mg/g respectively for ACP and ACK as the initial concentration rises from 5 to 25 mg/L. This observed increase results from a higher collision rate between tartrazine molecules and the adsorbent surface as the concentration of tartrazine increases [<xref ref-type="bibr" rid="scirp.106719-ref18">18</xref>]. This trend is observed for both adsorbents until an adsorbate concentration of 25 mg/L, beyond which it starts decreasing for ACK. This indicates that at higher concentrations, tartrazine molecules accumulate on the surface of ACK and block the pore openings [<xref ref-type="bibr" rid="scirp.106719-ref19">19</xref>], observed a similar trend for the adsorption of methylene blue on bamboo-based activated carbon.</p><p>From the batch adsorption studies, we note that the quantities adsorbed by the ACP and ACK are almost the same although ACP has a surface area almost three times higher than that of ACK. ACK however, has a higher mean pore diameter and a more pronounced surface heterogeneity than ACP due to the presence of both meso and micropores on its surface, which promote good adsorption. This parameter could therefore justify the near identical adsorbed quantities.</p><p>We also carried out FTIR analysis on the adsorbents after adsorption. The results are represented in <xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0. Here we note the disappearance of the -OH stretching vibration at 3321.01 cm<sup>−</sup><sup>1</sup> after adsorption on the spectrum of ACK (<xref ref-type="fig" rid="fig9">Figure 9</xref>); this disappearance could be as a result of the reaction between the acid group on adsorbents surface and sulphonates functional group of the tartrazine with the release of a water molecule.</p></sec></sec><sec id="s3_3"><title>3.3. Adsorption Isotherms</title><p>The equilibrium data was analysed using the using the following linearized isotherm models as given in Equations (3)-(5).</p><p>Langmuir isotherm</p><p>1 Q e = 1 Q m K C e + 1 Q m (3)</p><p>Freundlich isotherm</p><p>ln Q e = ln K F + ( 1 / n ) ln C e (4)</p><p>Dubinin-Kaganer-Radushkevich isotherm model</p><p>ln Q e = ln Q m − β ε 2 (5)</p><p>where: Q<sub>e</sub> is the amount adsorbed at equilibrium (mg/g), K<sub>F</sub> is the Freundlich constant, 1/n is the heterogeneity factor which is related to the capacity and intensity of the adsorption, C<sub>e</sub> is the equilibrium concentration (mg/L). ε = RTln (1 + 1/C<sub>e</sub>) is the Dubinin-Kaganer-Radushkevich constant. Q<sub>m</sub> = theoretical isotherm saturation capacity (mg/g), β is the Dubinin-Kaganer-Radushkevich isotherm constant (mol/kJ)<sup>2</sup>.</p><p>The adsorption isotherms for ACK and ACP obtained under optimal conditions are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>1.</p><p>The adsorption isotherm of Tartrazine on ACP is type IV, characteristic of a mesoporous adsorbent. The presence of two layers result from the formation of a monolayer followed by a multilayer between the adsorbate and the adsorbent surface [<xref ref-type="bibr" rid="scirp.106719-ref28">28</xref>]. Here, the interaction between the molecules and the surface of the adsorbent are higher than those of the molecules themselves; the adsorption sites of the second layer will begin to be occupied when the first layer is fully saturated. The adsorption isotherm of tartrazine on ACK is also similar but the layers is less pronounced. The constants obtained from the isotherms models are given in <xref ref-type="table" rid="table2">Table 2</xref>.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Langmuir, Freundlich, Dubinin-Kaganer-Radushkevich and Tempkin constants</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Isotherm</th><th align="center" valign="middle" >Constants</th><th align="center" valign="middle" >ACP</th><th align="center" valign="middle" >ACK</th></tr></thead><tr><td align="center" valign="middle"  rowspan="4"  >Langmuir</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.9805</td><td align="center" valign="middle" >0.9824</td></tr><tr><td align="center" valign="middle" >Q<sub>m</sub> (mg∙g<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >24.57</td><td align="center" valign="middle" >21.598</td></tr><tr><td align="center" valign="middle" >K<sub>L</sub> (L∙mg<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >0,165</td><td align="center" valign="middle" >0.222</td></tr><tr><td align="center" valign="middle" >R<sub>L</sub></td><td align="center" valign="middle" >0.183</td><td align="center" valign="middle" >0.143</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >Freundlich</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.9408</td><td align="center" valign="middle" >0.9531</td></tr><tr><td align="center" valign="middle" >K<sub>F</sub> (mg∙g<sup>−</sup><sup>1</sup>) (L/mg)<sup>−</sup><sup>1/n</sup></td><td align="center" valign="middle" >4.912</td><td align="center" valign="middle" >5.289</td></tr><tr><td align="center" valign="middle" >1/n</td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.425</td></tr><tr><td align="center" valign="middle"  rowspan="4"  >DKR</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.9221</td><td align="center" valign="middle" >0.8709</td></tr><tr><td align="center" valign="middle" >β (mol<sup>2</sup>∙J<sup>−</sup><sup>2</sup>)</td><td align="center" valign="middle" >0.549</td><td align="center" valign="middle" >3.973</td></tr><tr><td align="center" valign="middle" >Q<sub>m</sub> (mg∙g<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >16.815</td><td align="center" valign="middle" >15.863</td></tr><tr><td align="center" valign="middle" >E (kJ∙mol<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >0.954</td><td align="center" valign="middle" >0.355</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >Tempkin</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.970</td><td align="center" valign="middle" >0.954</td></tr><tr><td align="center" valign="middle" >K<sub>T</sub> (L∙mg<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >1.623</td><td align="center" valign="middle" >2.079</td></tr><tr><td align="center" valign="middle" >b<sub>T</sub> (kJ∙mol<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >0.456</td><td align="center" valign="middle" >0.513</td></tr></tbody></table></table-wrap><p>The Langmuir model showed good correlation of experimental data indication adsorption is specific (chemisorption) for both adsorbents [<xref ref-type="bibr" rid="scirp.106719-ref1">1</xref>]. This suggest that adsorption takes place at uniform energy sites on the adsorbents surface. This is in good agreement with the results from infrared after adsorption, which shows the formation of a chemical bond between tartrazine molecules and the surface active sites of both adsorbents. The R<sub>L</sub> values of the Langmuir model is between 0 and 1 for both absorbents, hence adsorption is favourable [<xref ref-type="bibr" rid="scirp.106719-ref21">21</xref>]. The Freundlich correlation coefficients values near unity indicates that the equilibrium data is also consistent with this model, to an extent. Thus, a 1/n value between zero and one shows that the surface of both adsorbents are heterogeneous [<xref ref-type="bibr" rid="scirp.106719-ref22">22</xref>]. This heterogeneity could be attributed to the different functional groups present on the adsorbent surface and to the existence of different pore sizes.</p><p>The Dubinin-Kaganer-Radushkevich isotherm adsorption energies are less than 8 kJ/mol for both materials and indicate a physisorption mechanism attributed to the multilayer formation [<xref ref-type="bibr" rid="scirp.106719-ref16">16</xref>], which is in good agreement with type IV isotherm. If this value were greater than 8 kJ/mol chemical adsorption or ion exchange could occur. However, given that the difference between the theoretical and experimental value of quantity adsorbed is large, this model does not accurately describe the adsorption of tartrazine ions on both materials. The value of the b<sub>T</sub> constant of the Tempkin model is also less than 8 kJ/mol indicating that the adsorbent-adsorbate interactions are weak and are characteristic of physisorption in agreement with type IV isotherm [<xref ref-type="bibr" rid="scirp.106719-ref29">29</xref>]. However, the positive value of this constant suggests a gravitational adsorption on the both materials [<xref ref-type="bibr" rid="scirp.106719-ref26">26</xref>].</p></sec><sec id="s3_4"><title>3.4. Study of Kinetic Models</title><p>Adsorption is a time-dependent process, and determining the rate of adsorption is highly significant in the design and evaluation of an adsorbent in removing pollutants from wastewater [<xref ref-type="bibr" rid="scirp.106719-ref29">29</xref>]. The linear equations of the following kinetic models were used to study the adsorption reaction mechanism:</p><p>Pseudo-First order kinetic Model:</p><p>ln C t = C 0 − K 1 t (6)</p><p>Pseudo-second order kinetic model:</p><p>t Q t = 1 K 2 Q e 2 + t Q e (7)</p><p>Intra-particle diffusion model:</p><p>Q t = K i d t 0.5 + C (8)</p><p>Elovich model:</p><p>d Q d t = α e − β q t (9)</p><p>Linearizing equation (9) using the α β ≫ t , Q<sub>t</sub> = 0 to t = 0, Q<sub>t</sub>= Q<sub>t</sub> at t = t, gives:</p><p>Q t = ln ( α β ) + ln t (10)</p><p>where Q<sub>e</sub> and Q<sub>t</sub> are the sorption capacity (mg/g) at equilibrium and at time t respectively. K<sub>1</sub> is the rate constant of pseudo-first order equation (min<sup>−</sup><sup>1</sup>), K<sub>2</sub> is the pseudo-second order rate constant (g∙mg<sup>−</sup><sup>1</sup>∙min<sup>−</sup><sup>1</sup>), K<sub>id</sub> is the intra-particle diffusion constant (mg∙g<sup>−</sup><sup>1</sup>∙min<sup>−</sup><sup>1</sup>), C is a constant, which relates an idea about the boundary layer thickness of the boundary. <xref ref-type="table" rid="table3">Table 3</xref> below provides a comparison of the different kinetic models.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Constants and speed correlation coefficients of kinetic models</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Kinetic Model</th><th align="center" valign="middle" >Constants</th><th align="center" valign="middle" >ACP</th><th align="center" valign="middle" >ACK</th></tr></thead><tr><td align="center" valign="middle"  rowspan="3"  >Pseudo-first order</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.182</td><td align="center" valign="middle" >0.165</td></tr><tr><td align="center" valign="middle" >K<sub>1</sub> (min<sup>−1</sup>)</td><td align="center" valign="middle" >−0.015</td><td align="center" valign="middle" >−0.014</td></tr><tr><td align="center" valign="middle" >C<sub>0</sub> (mg∙L<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >7.326</td><td align="center" valign="middle" >7.472</td></tr><tr><td align="center" valign="middle"  rowspan="4"  >Pseudo-second order</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.995</td><td align="center" valign="middle" >0.999</td></tr><tr><td align="center" valign="middle" >K<sub>2</sub> (g∙min<sup>−</sup><sup>1</sup>∙mg<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >0.605</td><td align="center" valign="middle" >0.076</td></tr><tr><td align="center" valign="middle" >Q<sub>e</sub> (mg∙g<sup>-1</sup>)</td><td align="center" valign="middle" >19.157</td><td align="center" valign="middle" >19.802</td></tr><tr><td align="center" valign="middle" >h (mg∙g<sup>−</sup><sup>1</sup>∙min<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >222.222</td><td align="center" valign="middle" >30.03</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >Intra-particle diffusion</td><td align="center" valign="middle" >R<sup>2</sup></td><td align="center" valign="middle" >0.007</td><td align="center" valign="middle" >0.491</td></tr><tr><td align="center" valign="middle" >K<sub>id</sub> (mg∙g<sup>−</sup><sup>1</sup>∙min<sup>−</sup><sup>1</sup>)</td><td align="center" valign="middle" >46.500</td><td align="center" valign="middle" >41.760</td></tr><tr><td align="center" valign="middle" >C</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >0.031</td></tr></tbody></table></table-wrap><p>From the above table, only the pseudo-second-order model has a correlation coefficient (R<sup>2</sup> value) close to unity for both adsorbents. This indicates that the chemisorption is the rate-limiting step, the same results have been obtained by [<xref ref-type="bibr" rid="scirp.106719-ref27">27</xref>]. Furthermore, the theoretical and experimental adsorbed quantities are close enough and confirm the assertion that was has been made in interpreting the FT-IR spectra after adsorption. The adsorption rate constant for ACK is smaller than for ACP. This could be partly due to faster fixation (t = 5 min) of tartrate ion on ACP than on ACK (t = 10 min) [<xref ref-type="bibr" rid="scirp.106719-ref30">30</xref>]. This could attribute to the fact that ACP possesses higher surface area than ACK which lead to the more available surface active sites at the start of the process. This is also confirmed by the value of initial adsorption rate (h) which shows that the flow of the tartrazine molecules is initially greater for ACP than ACK. Indeed the value of this parameter is seven times higher for ACP than that of ACK.</p></sec><sec id="s3_5"><title>3.5. Thermodynamic Study and Effect of Temperature</title><p>To study the thermodynamic of the adsorption of tartrazine onto ACP and ACK, we carried experimental adsorption runs in which we varied the temperature of the adsorption milieu between the range of 30˚C to 55˚C. The thermodynamic parameters studied are enthalpy (ΔH˚), entropy (ΔS˚) and Gibbs free energy (ΔG˚). The thermodynamic parameters were calculated from the following expressions [<xref ref-type="bibr" rid="scirp.106719-ref31">31</xref>]:</p><p>K d = C a C e (11)</p><p>Δ G = − R T ln K d (12)</p><p>ln K d = Δ S R − Δ H R T (13)</p><p>where, K<sub>d</sub> is equilibrium constant, C<sub>a</sub> the concentration of adsorbate in equilibrium on the adsorbent (mg/L), C<sub>e</sub> the concentration of adsorbate in equilibrium in the solution (mg/L), R the ideal gas constant (8.314 J/K/mol), ΔG˚ (kJ/mol), ΔH˚ (kJ/mol), ΔS˚ (kJ/mol) are the change in free energy, enthalpy and entropy respectively.</p><p>By plotting a graph of lnK<sub>d</sub> versus 1/T (<xref ref-type="fig" rid="fig1">Figure 1</xref>2 and <xref ref-type="fig" rid="fig1">Figure 1</xref>3), the values of ΔH˚ and ΔS˚ can be estimated from correlation coefficient value of ACK and ACP are respectively (R<sup>2</sup> = 0.8736) and (R<sup>2</sup> = 0.9111) indicating good linearity.</p><p><xref ref-type="table" rid="table4">Table 4</xref> shows that the Gibbs energy (ΔG˚) and the enthalpy (ΔH˚) are positive. This indicates that the adsorption is exothermic and spontaneous for ACP, requiring no energy input. By contrast, the reaction is exothermic but non-spontaneous for ACK, hence it requires energy input to start the process. In addition, the negative value of ΔS˚ in both cases shows that the adsorption progresses with increasing disorder in the solid solution interface. We also note that the value of ΔS˚ for ACP is near to zero and shows that there is more disorder during adsorption of the latter, which is in agreement with the constant</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Thermodynamic parameters for adsorption of tartrazine by ACP and ACK</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Adsorbent</th><th align="center" valign="middle" >T (K)</th><th align="center" valign="middle" >ΔG˚ (kJ/mol)</th><th align="center" valign="middle" >ΔH˚ (kJ/mol)</th><th align="center" valign="middle" >ΔS˚ (J/mol∙K)</th></tr></thead><tr><td align="center" valign="middle"  rowspan="4"  >ACP</td><td align="center" valign="middle" >303</td><td align="center" valign="middle" >−7.297</td><td align="center" valign="middle"  rowspan="4"  >−13.871</td><td align="center" valign="middle"  rowspan="4"  >−22.090</td></tr><tr><td align="center" valign="middle" >313</td><td align="center" valign="middle" >−6.745</td></tr><tr><td align="center" valign="middle" >323</td><td align="center" valign="middle" >−6.729</td></tr><tr><td align="center" valign="middle" >328</td><td align="center" valign="middle" >−6.723</td></tr><tr><td align="center" valign="middle"  rowspan="4"  >ACK</td><td align="center" valign="middle" >303</td><td align="center" valign="middle" >3.298</td><td align="center" valign="middle"  rowspan="4"  >−107.832</td><td align="center" valign="middle"  rowspan="4"  >−363.064</td></tr><tr><td align="center" valign="middle" >313</td><td align="center" valign="middle" >3.733</td></tr><tr><td align="center" valign="middle" >323</td><td align="center" valign="middle" >9.658</td></tr><tr><td align="center" valign="middle" >328</td><td align="center" valign="middle" >11.974</td></tr></tbody></table></table-wrap><p>initial velocity model of pseudo-second order (seven times greater than that of ACK), showing a strong affinity between the ACP and tartrazinemolecules. Moreover, examination of values of standard enthalpy of adsorption (&lt; 40 kJ/mol) [<xref ref-type="bibr" rid="scirp.106719-ref32">32</xref>] indicated the presence of physical attractive process make by Van Der Waals interaction during the multilayers formation. Therefore, it is reasonable to conclude that both physical adsorption and chemical adsorption equally participate in the overall process of tartrazine adsorption on ACK and ACP materials.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>Two adsorbents ACP and ACK were prepared and characterized. They were successfully applied to elimination of tartrazine in aqueous solution. Several factors affecting adsorption such as contact time, adsorbent dose, initial concentration of adsorbate and temperature were also studied. The variation of pH and initial concentration gave an optimum pH of 2; the quantity adsorbed increased with increasing initial concentration. We also found that the degree of heterogeneity affected the quantity adsorbed. Kinetic studies showed that chemisorption was the rate-limiting step; however, equilibrium studies revealed the presence of physical adsorption process. Additionally, thermodynamic study revealed that the adsorption was exothermic for both adsorbents, but it was spontaneous for ACP and not for ACK. The results obtained in this work confirm that AC obtained from Cola nutshells could be used for the removal of tartrazine from wastewater.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The authors of this work sincerely wish to thank the members of the Adsorption and Surface “Research Unit” of the Applied Physical and Analytical Chemistry Laboratory of the University of Yaound&#233; I.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Brice, D.N.C., Manga, N.H., Arnold, B.S., Daouda, K., Victoire, A.A., Giresse, N.N.A., Nangah, C.R. and Nsami, N.J. (2021) Adsorption of Tartrazine onto Activated Carbon Based Cola Nuts Shells: Equilibrium, Kinetics, and Thermodynamics Studies. 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