<?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">JCPT</journal-id><journal-title-group><journal-title>Journal of Crystallization Process and Technology</journal-title></journal-title-group><issn pub-type="epub">2161-7678</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jcpt.2018.81002</article-id><article-id pub-id-type="publisher-id">JCPT-81867</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>
 
 
  Migration of Biodegradable Organic Matter in Underlying Soils of Household Waste Dumpsites: A Case Study in Abomey-Calavi, Benin
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Metogbe</surname><given-names>B. Djihouessi</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>Sofiath</surname><given-names>Onifade</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>Martin</surname><given-names>P. Aina</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hervé</surname><given-names>E. Labité</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>François</surname><given-names>de Paule Codo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Institut National de l’Eau (INE), Université d’Abomey-Calavi (UAC), Cotonou, Bénin</addr-line></aff><aff id="aff1"><addr-line>Laboratoire des Sciences et Techniques de l’Eau (LSTE), Institut National de l’Eau, Université d’Abomey-Calavi (UAC), Cotonou, Bénin</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>marnickson@yahoo.fr(MPA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>12</month><year>2017</year></pub-date><volume>08</volume><issue>01</issue><fpage>18</fpage><lpage>32</lpage><history><date date-type="received"><day>28,</day>	<month>November</month>	<year>2017</year></date><date date-type="rev-recd"><day>14,</day>	<month>January</month>	<year>2018</year>	</date><date date-type="accepted"><day>19,</day>	<month>January</month>	<year>2018</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>
 
 
  This paper presented the first part of the studies about the development of a tool for groundwater contamination prediction, conducted by the Laboratory of Sciences and Technology of Water (UAC/Benin). The investigation made consisted in estimating the combined effect of retardation factor and biodegradation on migration processes of leachate, in the underlying soils of household waste dumpsites, without active safety barrier. Leachate infiltration tests for different initial conditions were made on soil columns and the breakthrough curves were traced for electrical conductivity, the 5 day biochemical oxygen demand (BOD
  <sub>5</sub>) and total kjeldahl nitrogen TKN. A mathematical migration model was developed and solved numerically by finite difference method and implemented with Matlab R2013a. Thus, the calibration of the model was made with electric conductivity data by determining the dispersion coefficient of the studied soils (
  <em>D</em> = 0.96 cm
  <sup>2</sup>/min). Simulations for model verification showed that the established model can perfectly predict the migration of biodegradable organic pollution (BOD
  <sub>5</sub>) but did not give conclusive results for the monitoring of nitrogenous organic matter (TKN). The influence of the retardation factor on the migration of biodegradable organic pollutants in soils was linear, while the biodegradation rate of the organic material on migration showed an exponential pattern.
 
</p></abstract><kwd-group><kwd>Waste Dumpsites</kwd><kwd> Pollutants</kwd><kwd> Biodegradability</kwd><kwd> Soil Dispersion</kwd><kwd> Column Test</kwd><kwd> Biodegradable Organic Pollution</kwd><kwd> Nitrogenous Organic Matter</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The migration of solutes in a porous medium is usually controlled by three mechanisms: Convection, molecular diffusion and mechanical dispersion [<xref ref-type="bibr" rid="scirp.81867-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref2">2</xref>] . During transport of a soluble contaminant from soil surface to groundwater, mechanical dispersion is the major migration mechanism [<xref ref-type="bibr" rid="scirp.81867-ref3">3</xref>] . It is well known that the dispersion of a pollutant in a soil, saturated or not, is influenced both by the intrinsic properties of the soil (such as its nature, porosity, tortuosity and grain size distribution), and by the properties of the fluid flow and transportation (such as viscosity, density and velocity of the fluid) [<xref ref-type="bibr" rid="scirp.81867-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref5">5</xref>] . However, independent of these parameters, it is important in the study of the dispersion process to take into account the nature and origin of the pollutant. Whether organic, inorganic, mineral or heavy metals, domestic, industrial, or pesticides, pollutants involve a large number of phenomena and reactions that may significantly influence their migration in soils [<xref ref-type="bibr" rid="scirp.81867-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref7">7</xref>] .</p><p>Major phenomena or reactions encountered during migration of leachates in soil, include: Solubilisation at acidic pH and the precipitation at a basic pH [<xref ref-type="bibr" rid="scirp.81867-ref8">8</xref>] , metal complexation by organic matter [<xref ref-type="bibr" rid="scirp.81867-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref10">10</xref>] , biodegradation of organic matter [<xref ref-type="bibr" rid="scirp.81867-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref12">12</xref>] , adsorption of ions or molecules on the surface of the soil grains [<xref ref-type="bibr" rid="scirp.81867-ref13">13</xref>] and cationic exchange phenomena [<xref ref-type="bibr" rid="scirp.81867-ref14">14</xref>] . Thus, to effectively prevent contamination of groundwater by leachate, it is important to define models which can combine the mechanisms of the fluid flow and transport in soils to the mechanisms related to the pollutants nature.</p><p>In this paper, a risk assessment tool was developed based on a model coupling the convection-dispersion to the biodegradation of organic pollutants during leachate migration processes in soils for the prediction of groundwater contamination in the context of developing countries.</p></sec><sec id="s2"><title>2. Background Concepts</title><sec id="s2_1"><title>2.1. Convection-Dispersion Model</title><p>Generally, the change in concentration of a passive pollutant A between two points of a soil column is considered as a one-dimensional transport problem, which is simultaneously subjected to the phenomena of convection and dispersion [<xref ref-type="bibr" rid="scirp.81867-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref16">16</xref>] . This gives:</p><p>∂ c A ∂ t = D z ∂ 2 c A ∂ z 2 − q z ∂ c A ∂ z + S ( c A ) (2.1)</p><p>where: c A is the concentration of the pollutant A ( M ⋅ L − 3 ) , D z is the overall coefficient of diffusion-dispersion ( L 2 ⋅ T − 1 ) , is the Darcy velocity, ( L ⋅ T − 1 ) , z and t are the spatial (L) and time (T) variables, and S ( c A ) describes the set of reactions and contributions that take place in the porous medium ( M ⋅ L − 3 ) also called source.</p><p>Notice that: c A = c A p + c A s ; with:</p><p>∂ c A p ∂ t = ε ∂ c A ∂ t , change in concentration of A in the soil void; (2.2)</p><p>∂ c A s ∂ t = ( 1 − ε ) ∗ ρ s ∗ K d ∂ c A ∂ t , change in concentration of A at soil grain surface.(2.3)</p><p>where ε is the porosity of the soil expressed in %, ρ s is the density of the solid matrix ( M ⋅ L − 3 ) , and K d is the exchange capacity between the fluid and the solid matrix.</p></sec><sec id="s2_2"><title>2.2. Coupling Biodegradation and Migration Processes</title><p>Assuming that the major reaction taking place in the porous medium is a first- order biodegradation reaction of organic matter by oxidation of organic compounds. The source term of (2.1) is written as follows: S ( c A ) = ∂ c A ∂ t = − λ D ⋅ c A</p><p>[<xref ref-type="bibr" rid="scirp.81867-ref17">17</xref>] . Where λ D is the degradation rate of the pollutant A. Therefore, Equation (2.1) becomes:</p><p>∂ c A ∂ t = D z ε R ∂ 2 c A ∂ z 2 − v z ε R ∂ c A ∂ z − λ D ε R ⋅ c A ;     with   R = 1 + ( 1 − ε ) ε ∗ ρ s ∗ K d (2.4)</p><p>where R is the retardation coefficient reflecting the slowing of studied pollutant; it depends on the affinity that has the pollutant to the solid matrix.</p><p>The Darcy velocity in Equation (2.4) assumes that the pollutant transport takes place in an empty column. However, the column is filled with a soil of porosity. Therefore, the Darcy velocity is replaced with the interstitial velocity: u z = q z / ε , and then the effective dispersion coefficient appears and is expressed as: D = D z / ε .</p><p>For solute transfer in soil, the diffusivity is usually smaller than the dispersion [<xref ref-type="bibr" rid="scirp.81867-ref2">2</xref>] . For a small ratio of the diameter to the length of a soil column (d/L) and for a large fluid velocity, the radial dispersion may be neglected in comparison with</p><p>the axial dispersion [<xref ref-type="bibr" rid="scirp.81867-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref19">19</xref>] . Thus, with: λ = λ D ε R , the migration mechanisms</p><p>of a dissolved biodegradable organic substance in the granular porous medium is expressed by:</p><p>∂ c A ∂ t = D R ∂ 2 c A ∂ z 2 − u z R ∂ c A ∂ z − λ ⋅ c A (2.5)</p><p>Equation (2.5) expresses the coupling “biodegradation - convection dispersion”, taking place during the migration of soluble contaminants in soil. The finite difference method or the finite volume solves this equation.</p></sec></sec><sec id="s3"><title>3. Materials and Methods</title><p>Model calibration and verification often require some selected initial values and certain key parameter values. In this study, experimental tests of injections of leachate on soil column were performed according to the protocol for measuring the axial dispersion [<xref ref-type="bibr" rid="scirp.81867-ref4">4</xref>] . Measured data were used to set up inputs to drive the model and provide a basis for adjusting model parameters, in particular dispersion, D.</p><sec id="s3_1"><title>3.1. Inputs Values: Experimental Tests</title><p>The columns of sampled soils were monolithic type. Identification of soil sampling location was made according to ISO 15175:2004 standard, applied to all dumpsites of the municipality of Abomey-Calavi in Benin. The studied soil is a loamy soil. The geotechnical characteristics of the soil of the samples are shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The characteristics of the leachate used for infiltration tests are presented in <xref ref-type="table" rid="table2">Table 2</xref>. It was a synthetic leachate obtained after leach tests performed by method in batch (cf. [<xref ref-type="bibr" rid="scirp.81867-ref20">20</xref>] ) on the household waste from the main dumpsites of the municipality of Abomey-Calavi. During the tests, electrical conductivity, BOD<sub>5</sub> and TKN were measured. These data were used to trace the breakthrough curves of these parameters. The biodegradation rate of dissolved organic carbon was determined according to the method presented in [<xref ref-type="bibr" rid="scirp.81867-ref21">21</xref>] and [<xref ref-type="bibr" rid="scirp.81867-ref22">22</xref>] : λ = 0.000037 d<sup>−1</sup>.</p></sec><sec id="s3_2"><title>3.2. Model Discretization</title><p>The discretization of Equation (2.5) was made here by the finite difference method on uniform mesh. Consider that along a vertical soil column with sufficiently large length L, a liquid with initial concentration C 0 flows with interstitial velocity u z . At a moment t 0 , a pollutant of concentration C is injected at the upper end of the column and migrates in the axial direction towards the lower end. It is convenient to define the appropriate boundary conditions (Dirichlet conditions here):</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Geotechnical characteristics of the soil</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Porosity</th><th align="center" valign="middle" >Macro-pores</th><th align="center" valign="middle" >Permeability. k (m/s)</th><th align="center" valign="middle" >Hydraulic Grad. I</th><th align="center" valign="middle" >Darcy Velocity (m/s)</th><th align="center" valign="middle" >Interstitial Velocity (m/s)</th></tr></thead><tr><td align="center" valign="middle" >27.5%</td><td align="center" valign="middle" >21%</td><td align="center" valign="middle" >2.36E−06</td><td align="center" valign="middle" >8.8</td><td align="center" valign="middle" >2.08E−06</td><td align="center" valign="middle" >7.55E−06</td></tr><tr><td align="center" valign="middle" >ASTM D4404-10</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >ISO 17312:2005</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Physical and Chemical Characteristics of the leachate</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameters</th><th align="center" valign="middle" >Unit</th><th align="center" valign="middle" >Max</th><th align="center" valign="middle" >Min</th><th align="center" valign="middle" >Mean</th><th align="center" valign="middle" >SD</th><th align="center" valign="middle" >Precision</th><th align="center" valign="middle" >Methods standard</th></tr></thead><tr><td align="center" valign="middle" >pH</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >4.09</td><td align="center" valign="middle" >3.84</td><td align="center" valign="middle" >3.93</td><td align="center" valign="middle" >0.14</td><td align="center" valign="middle" >&#177;0.001</td><td align="center" valign="middle" >ISO 10523:2008</td></tr><tr><td align="center" valign="middle" >Elec. Cond.</td><td align="center" valign="middle" >(&#181;S/cm)</td><td align="center" valign="middle" >3812</td><td align="center" valign="middle" >3361</td><td align="center" valign="middle" >3554</td><td align="center" valign="middle" >232</td><td align="center" valign="middle" >&#177;1</td><td align="center" valign="middle" >ISO 7888:1985</td></tr><tr><td align="center" valign="middle" >COD</td><td align="center" valign="middle" >(mg O<sup>2</sup>/l)</td><td align="center" valign="middle" >14,086</td><td align="center" valign="middle" >12,017</td><td align="center" valign="middle" >13,218</td><td align="center" valign="middle" >1074</td><td align="center" valign="middle" >&#177;1</td><td align="center" valign="middle" >ASTM D1252</td></tr><tr><td align="center" valign="middle" >BOD<sub>5</sub></td><td align="center" valign="middle" >(mg O<sup>2</sup>/l)</td><td align="center" valign="middle" >6301</td><td align="center" valign="middle" >5326</td><td align="center" valign="middle" >5822</td><td align="center" valign="middle" >488</td><td align="center" valign="middle" >&#177;1</td><td align="center" valign="middle" >NFT 90-103</td></tr><tr><td align="center" valign="middle" >TKN</td><td align="center" valign="middle" >(mg/l)</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >18</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >&#177;1</td><td align="center" valign="middle" >ASTM D3590 ? 11</td></tr></tbody></table></table-wrap><p>C ( 0 , t ) = C ;     C ( ∞ , t ) = C 0 ;     C ( z , 0 ) = C 0 . (3.2)</p><p>The differentiation schemes used are:</p><p>{ ( ∂ C ∂ t ) i j = C i j + 1 − C i j Δ t ( ∂ 2 C ∂ z 2 ) i j = C i + 1 j − 2 C i j + C i − 1 j Δ z 2 ( ∂ C ∂ z ) i j = C i + 1 j − C i − 1 j 2 Δ z (3.3)</p><p>where: L is divided into N intervals with ends or nodes z i , i ranges from 1 to N + 1; C i j is the concentration at the node z i = i Δ z at t = j Δ t . Thus Equation (2.5) is equivalent to the set of:</p><p>C i j + 1 = ( α + β ) C i − 1 j + ( 1 − 2 α − γ ) C i j + ( α − β ) C i + 1 j with     { α = D Δ t R Δ z 2 β = u z Δ t 2 R Δ z γ = λ Δ t (3.4)</p><p>i ranges from 1 to N − 1.</p><p>The system (3.4) has been implemented by the successive over-relaxation method. The calculations were performed with Matlab R2013a. The initial values were: length of the column (𝐿), time of simulation (𝑇), space step (∆z), time step (∆𝑡), flow velocity ( u z ), retardation factor (𝑅), initial concentration (C) and a starting value for axial dispersion coefficient (D).</p><p>The retardation factor R of the pollutant over a water molecule is defined by the quotient of the residence time of the pollutant ( t s ) over the residence time of the water molecule [<xref ref-type="bibr" rid="scirp.81867-ref23">23</xref>] . In this study, where the flow permanent and uniform flow, R is determined by Equation (3.5). The residence times of pollutants and water molecule were measured experimentally by injections of leachate on soil columns. Thus, the mean value for the retardation coefficient was calculated and is equal to 2.5.</p><p>R = t s L θ ⋅ v z</p><p>where: L is the length of the column; θ is water content in the column and v z the Darcy velocity in column input [<xref ref-type="bibr" rid="scirp.81867-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.81867-ref25">25</xref>]</p></sec><sec id="s3_3"><title>3.3. Model Calibration</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the algorithm to solve Equation (2.5) following the method of finite differences. The program performed an adjustment of the given initial value for axial dispersion coefficient in order to optimize the comparison of model results to measured data. The initial value of the axial dispersion coefficient for the implementation was chosen in accordance with the values found in the literature for the dispersion in loamy soils and was equal to 0.048 cm<sup>2</sup>/min [<xref ref-type="bibr" rid="scirp.81867-ref26">26</xref>] .</p><p>To quantify the model’s prediction, the Relative Root-mean-square Error (RRE) was used to compare simulated versus observed values, with the best fitting simulation returning the lowest RRE.</p></sec><sec id="s3_4"><title>3.4. Model Verification</title><p>The dispersion coefficient obtained after model calibration was used as input for the verification of the model (<xref ref-type="fig" rid="fig1">Figure 1</xref>). The result obtained after simulation was compared with the measured data. Model was approved when the RRE obtained after verification was close to the RRE for model calibration.</p></sec></sec><sec id="s4"><title>4. Results and Discussion</title><p>The measured data were separated into two subsets: one subset for model calibration and another subset for model validation. 48 infiltration tests were carried out on soil columns A of 30 cm length. The subset for the model calibration encompassed the electrical conductivity (EC) data of the columns A. The simulated parameters for model verification include BOD<sub>5</sub> and TKN, registered at the outlet of columns A.</p><sec id="s4_1"><title>4.1. Infiltration Rate</title><p>The influence of the hydraulic gradient on the leachate infiltration rate was</p><p>shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. This figure showed that the evolution of the infiltration speed according to the hydraulic gradient had two phases: The first branch where the infiltration rate increased rapidly for small changes of the hydraulic gradient and the second branch where the infiltration rate was less sensitive to the change of the hydraulic gradient.</p><p>Note that for a hydraulic gradient of 8.8, the actual infiltration rate measured when characterizing the soil ( 7.55 &#215; 10 − 4 cm / s ) was close to the one obtained experimentally ( 8.07 &#215; 10 − 4 cm / s ). Thus, the rate of flow of leachate in soils for subsequent simulations was taken as 8 &#215; 10 − 4 cm / s .</p></sec><sec id="s4_2"><title>4.2. Model Calibration</title><p>The time of simulation was computed to simulate one-month leachate migration during the rainy season. A time step of 1 second (s) was used throughout the simulations. The simulated Breakthrough curves and the experimentally-derived breakthrough curve for model calibration are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> RRE for model calibration</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Simulations</th><th align="center" valign="middle" >Sim1 D = 0.048</th><th align="center" valign="middle" >Sim2 D = 0.48</th><th align="center" valign="middle" >Sim3 D = 0.96</th><th align="center" valign="middle" >Sim4 D = 1.2</th><th align="center" valign="middle" >Sim5 D = 1.28</th></tr></thead><tr><td align="center" valign="middle" >RRE (in %)</td><td align="center" valign="middle" >40.96</td><td align="center" valign="middle" >17.78</td><td align="center" valign="middle" >11.22</td><td align="center" valign="middle" >11.45</td><td align="center" valign="middle" >11.67</td></tr></tbody></table></table-wrap><p>A comparison of model results to measured data, illustrated by RRE (<xref ref-type="table" rid="table3">Table 3</xref>), showed that simulation 1 (Sim1 D = 0.048), performed with the initial value of dispersion coefficient derived from the literature ( D = 0.048   cm 2 / min ) , gave an unsatisfactory fit (RRE = 40.96). Gradually, as the value of the dispersion coefficient was incrementally increased, the simulation curve better approximated the experimental curve. Simulation 3 (Sim3 D = 0.96) provided the optimum fit, with a RRE of 11.22% between model results and measured data. However, the value of the dispersion obtained at the end of the simulation (2378 &#181;S/cm) is less than the experimental value (3174 &#181;S/cm). Note that the experimental curve had a first concavity due to change of solute concentration in effluent at the column outlet at early time between 275 and 600 min. This rapid change of concentration is followed by a bearing between 650 and 890 min. This pattern was probably due to preferential paths in soil columns. Indeed, the preferential flow paths are reflected in very rapid change of solute concentration in effluent at early times. The monolithic soil columns (as the one used in this study) generally have macropores which can promote preferential flows [<xref ref-type="bibr" rid="scirp.81867-ref3">3</xref>] . Thus, before a generalization of these results can be made, the status of the macropores distribution in the soil columns should be investigated. For this case study, the average proportion of macro-pores inside the soil columns was 21%. A correction of about 21% of the experimental result approached the simulated (predicted) value. The calibrated value of the dispersion coefficient for this study was D = 0.96   cm 2 / min .</p></sec><sec id="s4_3"><title>4.3. Model Verification</title><p>For the model verification, a longer time step was selected. This time was calculated to correspond to a simulation of the amount of leachate produced during the long rainy season (from March to June) in southern Benin. The verification process involves running the model with the calibrated dispersion coefficient D = 0.96   cm 2 / min and comparing the results to the independent data set for model verification.</p><sec id="s4_3_1"><title>4.3.1. Organic Matter (BOD<sub>5</sub>) Migration Model</title><p>In the numerical simulation of BOD<sub>5</sub> migration, the biodegradation rate of the studied leachate was considered, which is 0.000037 d<sup>−1</sup>. This value was taken equal to zero upon insertion of input parameters for the model calibration with the electrical conductivity. <xref ref-type="fig" rid="fig4">Figure 4</xref> showed the results obtained for experimental investigation and numerical simulations with dispersion coefficient D = 0.96   cm 2 / min . The RRE between model results and measured data was 11.14%.</p><p>As in the case of electrical conductivity data for model calibration, a bearing was clearly observed on the measured BOD<sub>5</sub> data for model verification between 660 and 990 min. The end result for BOD<sub>5</sub> simulation (4197 mg O<sub>2</sub>/l) was less than measured outcome (4914 mg O<sub>2</sub>/l), with a simulation result correction of 21% again approximating the experimental result. The calibrated dispersion coefficient (D) adequately modelled the diffusion of organic pollution for the studied soil. The verification of the migration model for the transport of organic matter in soil (BOD<sub>5</sub>) gave satisfactory results.</p></sec><sec id="s4_3_2"><title>4.3.2. Nitrogenous Organic Matter (TKN) Migration Model</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the simulated and measured breakthrough curves of TKN in soil</p><p>columns. As can be seen, the calibrated dispersion coefficient did not reflect the experimental evolution of the nitrogenous organic matter, and ammonia/ ammonium in the soil. The verification of the migration of TKN in soil columns A was not conclusive.</p><p>The analysis of the breakthrough curve of measured TKN showed a reduction of 99.65% of the nitrogenous organic matter at the end of the experimentation, which was above the recorded reductions for electrical conductivity (10.69%) and BOD<sub>5</sub> (15.69%). Usually, TKN is mostly made up of biodegradable organic compounds and therefore, a similar behavior to BOD would be expected. The failure of the validation of the TKN migration model could come from the difference recorded in the reductions of TKN and BOD. A low ratio of organic nitrogen to NH<sub>3</sub>/ NH 4 + could explain this difference in the reductions. Therefore it can be inferred that the retardation phenomena and biodegradation of organic matter reactions are not sufficient to model the migration of TKN in soil. The model should look at the different components of TKN separately. In another hand, since the retardation coefficient R was calculated based on EC measurements, it might be that the model works for large humic macromolecule (forming part of BOD, for instance), rather than for much smaller molecules as ammonia (in TKN).</p><p>At this stage of the study, the designed model properly evaluate the effect of retardation factor on the migration of macromolecules contained in leachate. For much smaller molecules as ammonia, a recalibration of the retardation factor seem to be necessary. A proper model of migration of biodegradable organic matter in the underlying soils would then require a coupling of two retardation factors: one for the macromolecules contained in the leachate and another one for the smaller monovalent ion (such as Na<sup>+</sup> in EC) or ammonia,</p></sec></sec><sec id="s4_4"><title>4.4. Influence of Measured Input Parameters</title><sec id="s4_4_1"><title>4.4.1. Influence of the Retardation Factor on Organic Matter Migration Model</title><p>Retardation coefficient (R) represents the delay accused by a pollutant molecule with respect to the water molecule introduced at the same time at the inlet of a soil column. The value for the retardation factor coefficient taken for model calibration and verification in this study was 2.5. <xref ref-type="fig" rid="fig6">Figure 6</xref> showed simulated breakthrough curves of BOD<sub>5</sub> migration for different values of retardation factor.</p><p>The analysis of the curves in <xref ref-type="fig" rid="fig6">Figure 6</xref> revealed that the migration of BOD<sub>5</sub> in soil columns was slowed by the increased retardation factor. The simulation of the dispersion of organic matter with R = 2.5 was the one that best approximates the measured results. Therefore the method used to measure the retardation coefficient is effective. For a non-delayed migration of pollutants, expressed by a retardation factor equal to 1, the simulated results are far removed from experimental result. The retardation factor is an essential parameter in modelling the migration of biodegradable organic matter in soils of waste dumpsites.</p><p>The influence of the retardation factor in the migration of biodegradable organic pollutants in soils was linear, and expressed in the present experimental study by the following equation: (<xref ref-type="fig" rid="fig7">Figure 7</xref>)</p><p>y = − 0.13 x + 1.05 (4.1)</p></sec><sec id="s4_4_2"><title>4.4.2. Influence of Biodegradation Rate on Organic Matter Migration Model</title><p>The biodegradation rate expresses the speed of consumption of organic pollution by aerobic and anaerobic bacteria. Numerical simulations (<xref ref-type="fig" rid="fig8">Figure 8</xref>) showed that an assumption of zero biodegradation (BC = 0) better approximated the experimental result than prediction with BC = 0.000037j − 1, as used for BOD<sub>5</sub> model calibration. This can be explained by the fact that the organic matter biodegradation kinetics is an exponential function, thus, at the resolution of the experimentation, it is difficult to observe the effects of the biodegradion for short times of 1 and 2 days. An increase of around 10<sup>−</sup><sup>4</sup> of biodegradation rate causes a halving of organic pollution at the outlet of the soil columns. It could be</p><p>the interesting to test longer times/longer columns in order to properly evaluate the biodegradation effect. For a practical point of view, it would be then beneficial to proceed to a bacteria activation of the soil before the deposit of household waste.</p><p>The influence of the rate of biodegradation on migration of biodegradable organic pollutants in our experimental investigation (<xref ref-type="fig" rid="fig9">Figure 9</xref>) was expressed by the equation:</p><p>y = − 0.76 ⋅ e − 1688 x (4.2)</p></sec></sec></sec><sec id="s5"><title>5. Conclusion</title><p>The phenomenon of natural biodegradation of organic matter was combined with the principle of convection-dispersion to model migration of leachates in soil. The resolution of this model by the finite difference method showed that the migration in soil of macromolecules contained in leachate can be predicted based on retardation factor determine by infiltration test on soil columns. For much smaller molecules as ammonia, a recalibration of the retardation factor is necessary. Therefore a model that aims to predict the migration in soil of both macro and micromolecule of leachate seem to require a coupling of two type of retardation factor: one for macromolecule such as BOD and one for micro molecule such as ammonia. The model at this stage failed to predict the biodegradation during of organic matter during the migration of leachate in the soil. Longer test times and longer test columns are required in order to properly evaluate the biodegradation effect of leachate during it migration in soils. Increasing the bacterial activity of the underlying soils of garbage dumpsites could be a solution for natural reduction of pollutants migrating to groundwater.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors gratefully acknowledge the International Foundation for Science (IFS), Stockholm, for supporting the present work under the IFS Grant W/5840-1.</p></sec><sec id="s7"><title>Conflict of Interest Disclosure</title><p>The author(s) declare(s) that there is no conflict of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Djihouessi, M.B., Onifade, S., Aina, M.P., Labit&#233;, H.E. and de Paule Codo, F. (2018) Migration of Biodegradable Organic Matter in Underlying Soils of Household Waste Dumpsites: A Case Study in Abomey-Calavi, Benin. 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