<?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">JWARP</journal-id><journal-title-group><journal-title>Journal of Water Resource and Protection</journal-title></journal-title-group><issn pub-type="epub">1945-3094</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jwarp.2015.713089</article-id><article-id pub-id-type="publisher-id">JWARP-59771</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Use of Evapotranspiration (ET) Landfill Covers to Reduce Methane Emissions from Municipal Solid Waste Landfills
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>arek</surname><given-names>Abichou</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tarek</surname><given-names>Kormi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Cheng</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Haykel</surname><given-names>Melaouhia</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>Terry</surname><given-names>Johnson</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Stephen</surname><given-names>Dwyer</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Argonne National Laboratory, Chicago, IL, USA.</addr-line></aff><aff id="aff4"><addr-line>Waste Management, Minneapolis, MN, USA.</addr-line></aff><aff id="aff5"><addr-line>Dwyer Engineering, Albuquerque, NM, USA</addr-line></aff><aff id="aff2"><addr-line>Ecole Nationale d’ Ingenieurs de Gabes, Department de Genie Civil, Gabes, Tunisia, LASMAP, Ecole Polytechnique de Tunisie, University of Carthage, Tunisia</addr-line></aff><aff id="aff1"><addr-line>Department of Civil Engineering, Florida State University, Tallahassee, FL, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>abichou@eng.fsu.edu(AA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>09</month><year>2015</year></pub-date><volume>07</volume><issue>13</issue><fpage>1087</fpage><lpage>1097</lpage><history><date date-type="received"><day>24</day>	<month>August</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>15</month>	<year>September</year>	</date><date date-type="accepted"><day>21</day>	<month>September</month>	<year>2015</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>
 
 
  Solid waste landfills need to have final covers to 1) reduce the infiltration of rainfall into the waste mass and 2) reduce surface greenhouse gas emissions. Most regulations require that such final covers include hydraulic barriers, such as compacted clays with or without geomembrane. Significant research has been undertaken to allow the use of evapotranspiration-based covers (often termed: Evapotranspiration (ET) Cover, Water Balance Covers, or Phyto Covers) as an alternative to the barrier concept covers. ET covers are designed so that they have the capacity to store water by the soil and also have plants or vegetation to remove the stored water. In ET covers, plant roots can enhance the aeration of soil by creating secondary macropores which improve the diffusion of oxygen into soil. Therefore, biological methane oxidation (a natural process in landfill soils) can be improved considerably by the soil structuring processes of vegetation, along with the increase of organic biomass in the soil associated with plant roots. This paper summarizes a study to investigate the capacity of an ET cover to reduce surface greenhouse gas emissions when implemented on a solid waste landfill. This study consisted of using a numerical model to estimate methane emission and oxidation through an ET cover under average climatic conditions in Bennignton, Nebraska, USA. Different simulations were performed using different methane loading flux (5 to 200 gm
  <sup>-2</sup>&#183;d
  <sup>-1</sup>) as the bottom boundary. For all simulations, surface emissions were the lowest during the growing season and during warmer days of the year. Percent oxidation is the highest during the growing season and during warmer days. The lowest modeled surface emissions were always obtained during the growing season. Finally, correlations between percent oxidation and methane loading into simulated ET covers were proposed to estimate methane emissions and methane oxidation in ET covers.
 
</p></abstract><kwd-group><kwd>Evapotranspiration Covers</kwd><kwd> Methane Oxidation</kwd><kwd> Landfills</kwd><kwd> Greenhouse Gas Emissions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><sec id="s1_1"><title>1.1. Background</title><p>Final covers are used to reduce the quantity of water that infiltrates into waste deposits at landfills. Reducing the volume of infiltrating water reduces the amount of leachate that is generated and the risk of groundwater contamination. Generally, the applicable rules and regulations require that landfill covers employ resistive principles, i.e., layers having low saturated hydraulic conductivity such as compacted clay barriers, geosynthetic clay liners with or without a geomembrane. This design philosophy is often referred to as “raincoat”, barrier, or “umbrella” approach. Barrier type covers, such as compacted clay covers, have been shown to loose their impermeable qualities over time because of the influence of climate variations on the integrity of the soil layer [<xref ref-type="bibr" rid="scirp.59771-ref1">1</xref>] . The United States Environmental Protection Agency (USEPA) final cover regulations require a provision for the use of alternative final covers as long as they provide: 1) an infiltration layer that provides equivalent reduction in infiltration to that of the prescribed cover and 2) an erosion layer that provides equivalent protection from wind and water erosion as the one of the prescribed cover. One type of an alternative is to design landfill covers to exploit the water storage capacity of finer textured soils and the water removal capability of vegetation [<xref ref-type="bibr" rid="scirp.59771-ref2">2</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref6">6</xref>] . This type of cover is referred to as an evapotranspiration or ET cover.</p><p>Evapotranspiration (ET) covers are earthen final covers that control the percolation of infiltrating rainwater into the waste by balancing the water storage capacity of finer textured soils and the ability of plants to extract the water stored. They are designed to transmit equal or less percolation than the conventional resistive covers built with low hydraulic conductivity materials. Evapotranspiration (ET) covers (also referred to as: water balance covers, “store and release” covers, phyto-covers) are designed to have a capacity to store water by the soil and also to have the capacity to remove the stored water. Therefore, ET covers are essentially well-de- signed-vegetated soil landfill covers. The soil layer (s) of an ET cover stores moisture during rain events, and the sun and plants remove the water from the soil by evaporation and evapotranspiration, returning the moisture to the atmosphere.</p><p>Under landfill setting, final covers are also exposed to landfill gases from the waste mass below. Landfill gas is composed of 50% by volume of methane. Landfill gas is transported by diffusive and convective flux mechanisms from the anaerobic zone toward the atmosphere. The microbiological process of oxidizing CH<sub>4</sub> to CO<sub>2</sub> by methanotrophs is called microbial CH<sub>4</sub> oxidation. Several previous studies on landfill CH<sub>4</sub> oxidation in soil cover layers have demonstrated the ability of methane oxidation as a mechanism to reduce CH<sub>4</sub> emissions from landfill surfaces [<xref ref-type="bibr" rid="scirp.59771-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref13">13</xref>] . However, the capacity of landfill cover soil to oxidize CH<sub>4</sub> depends on both the physical and the chemical properties of landfill cover materials such as soil type, moisture content, density, organic and nutrient content, etc. Additionally, environmental conditions such as temperature and precipitation can also impact the performance of landfill cover soils in terms of oxidizing CH<sub>4</sub>.</p><p>In ET cover context, methane oxidation is impacted by vegetation, water content and soil temperature. The soil water content and the soil temperature in the soil profile govern gas transport and therefore methane oxidation in ET covers. Water content in the ET cover soil profile is a very important factor affecting CH<sub>4</sub> oxidation in landfill cover soils. First, the optimum environment for CH<sub>4</sub>-oxidizing bacteria (methanotrophic) is obtained within a specific water content range. Second, water content affects the penetration of O<sub>2</sub> into cover soils and O<sub>2</sub> is the main reactor for CH<sub>4</sub> oxidation. As water content increases in soil, O<sub>2</sub> diffusion into the soil is hindered. Third, water content affects the air-filled porosity of soil thus influences gas transport. As water fills up voided pores within the cover soil, it blocks the flow of gas upward. [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] and others correlated microbial activity with water content. Soil temperature also affects the bacterial activity of methane oxidizing bacteria. [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] and others correlated soil temperature to bacterial methane oxidation. In ET cover setting, these water content and soil temperature are dynamic and vary with time and with depth as a function of climatic conditions, vegetation, and soil hydraulic properties. In order to accurately predict methane oxidation in ET covers, landfill covers, the changing water content and temperature inside a cover has to be accounted for. In order to better predict gas emissions and methane oxidation in landfill covers, the changing water content and temperature inside the soil profile has to be accounted for in any numerical solution.</p></sec><sec id="s1_2"><title>1.2. Motivations and Objectives</title><p>The potential superior capability of ET covers to reduce fugitive release of methane to the atmosphere is an additional characteristic that should be considered to encourage the use of the types of covers. The basis of ET cover design is the predictive capabilities of the water balance modeling and the ability to quantify the maximum water infiltration from the atmosphere into the waste mass below the ET cover. ET covers provide a unique opportunity to introduce a modeling approach to methane oxidation in landfill covers since the modeling approach is already undertaken during the water balance assessment of the design. The objective of this study is to use a similar modeling methodology for methane oxidation to extend the water balance modeling-based design associated with ET covers to estimate gas transport and methane oxidation in and across an ET cover. The modeling approach consists of modeling gas transport using our existing gas transport and oxidation model. Our model accounts for dynamic parameters associated with the change in water content and temperature caused by change in climatic conditions at the upper boundary of the ET cover. The model also incorporates the changing temperature and water content to methanotrophic activity in the soil. The numerical model (FSU Model) is developed by our research team at Florida State University and combines water and heat flow with a gas transport and oxidation [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref18">18</xref>] . The modeling methodology is applied to an actual ET cover test section being assessed for hydraulic equivalency in Bennington Nebraska, USA.</p></sec></sec><sec id="s2"><title>2. Methods</title><sec id="s2_1"><title>2.1. Site Description</title><p>An ET cover was constructed and monitored as a demonstration project in Bennington, Nebraska. Bennington, NE, receives760 mm of rain per year. Snowfall is 740 mm. The number of days with any measurable precipitation is 92. On average, there are 216 sunny days per year in Bennington, NE. The July high temperature is around 30˚C. The January low is −11˚C. The project was intended to demonstrate that an ET cover as constructed in the demonstration project is functionally equivalent to the regulatory default cover based on water balance performance. The cover demonstration profile was constructed and instrumented in 2008. The instrumentation was activated during December 2008. The demonstration cover surface was then seeded in 2009. Surface vegetation and underlying rooting have been established. The soil moisture measurement equipment utilized on this project includes water content sensors and water potential sensors (soil suction). There were two sets of probes installed in instrumentation nests. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the placement and depth spacing for the probes installed in each nest. Instrumentation nests were installed in two locations (Nest A and B). Each nest consists of 7 water content sensors and 7 water potential sensors. A water content and water potential sensor is installed at each depth indicated in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Nest A was installed in the demonstration cover profile with a gentle slope (3.33%) that attempts to mimic the top surface of the landfill and is within that recommended by RCRA of 2 to 5%. Nest B was placed in the profile on a steeper slope (25% or 4:1) in an attempt to mimic steeper side slopes of the landfill. All of the nests of probes were connected to a central data logger. The weather station is co-lo- cated with the data logger. The equipment at this central location was mounted on a tripod in a weather resistant enclosure and lighting protection. The water balance aspect of the collected data is not addressed in this paper. Only the soil water content and potential data collected at each depth of Nest A and Nest B were averaged and used to estimate the Van Genunchten parameters describing the unstaured hydraulic properties of the ET cover layers as described later.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Plan view and profile of instrumentation nests installed in ET cover</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x6.png"/></fig></sec><sec id="s2_2"><title>2.2. Model Description</title><p>A numerical model (FSU Model) was developed by our research team at Florida State University that combined water and heat flow with a gas transport and oxidation model [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref18">18</xref>] . The latest version of the FSU model was bundled via a graphical user interface and was renamed the Landfill Surface Emission Model (Land SEM).</p><p>The new Land SEM model comprises four major modules, bundled via a graphical user interface:</p><p> A climate module which generates daily minimum and maximum air temperature along with daily rainfall based on the landfill site geographical location.</p><p> A soil property generation module which generates soil properties, e.g. saturated hydraulic conductivity, porosity, and methane oxidation capacity based on a built-in database of soil property data from the literature. The user can also input measured soil properties, if available.</p><p> A soil water content and temperature simulation module which uses the landfill site location, soil texture information and the climate generation data developed in the first two steps and then predicts the daily soil moisture and temperature at any depth of the soil cover profile for an average climatic year.</p><p> A core computational module, based on [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref18">18</xref>] , which simulates the concentration and flux of the gas components including methane in the landfill cover soil profile.</p><p>The climate simulator is a module adopted from the models Global Temp SIM and Global Rain [<xref ref-type="bibr" rid="scirp.59771-ref19">19</xref>] , including an air temperature simulation and precipitation simulation. The air temperature generation predicts the daily average air temperature based on a 30-year (1961-1990) temperature records and calculate the daily maximum and minimum air temperature. The global rainfall module estimates daily rainfall patterns for a yearly cycle based on a 30-year (1961-1990) global average monthly precipitation records. The information obtained from these modules together with the soil properties are used in the soil water content and temperature simulators. Global Temp SIM and Global Rain were used to estimate daily average air temperatures and average daily precipitation for Bennington, Nebraskausing the climate generation module with the USA postal service Zip Code as the main input.</p><p>The continuity equation describing the reactive transport of gas component i in landfill cover soils can be written [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>]</p><disp-formula id="scirp.59771-formula468"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x7.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x8.png" xlink:type="simple"/></inline-formula> is air-filled porosity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x10.png" xlink:type="simple"/></inline-formula>is the molar concentration of gas component i<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x11.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x12.png" xlink:type="simple"/></inline-formula>is the flux of gas component i due to advection and diffusion<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x14.png" xlink:type="simple"/></inline-formula>is the bulk density of soil<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x15.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x16.png" xlink:type="simple"/></inline-formula> is the production rate of gas component I<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x17.png" xlink:type="simple"/></inline-formula>. In Equation (1), the first</p><p>time on right hand side represents the transport process while the second term accounts for the soil gas reaction (oxidation for methane).</p><p>The flux <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x18.png" xlink:type="simple"/></inline-formula> can be determined by</p><disp-formula id="scirp.59771-formula469"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x19.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x20.png" xlink:type="simple"/></inline-formula> is the diffusion coefficient of component i in soil<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x22.png" xlink:type="simple"/></inline-formula>is the flow velocity of gas mixture in the soil (m/s).</p><p>The diffusion coefficient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x23.png" xlink:type="simple"/></inline-formula> can be calculated from its relationship with the diffusion coefficient in gas mixture,</p><disp-formula id="scirp.59771-formula470"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x24.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x25.png" xlink:type="simple"/></inline-formula> is the relative diffusion coefficient of gas in a tortuous void space in soil and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x26.png" xlink:type="simple"/></inline-formula> is the diffusion coefficient of gas component i in gas mixture. The relative diffusion coefficient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x27.png" xlink:type="simple"/></inline-formula> has been found to be independent to the gas itself [<xref ref-type="bibr" rid="scirp.59771-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.59771-ref21">21</xref>] . Although several formulation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x28.png" xlink:type="simple"/></inline-formula> based on air content in soils have been proposed (e.g. [<xref ref-type="bibr" rid="scirp.59771-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.59771-ref23">23</xref>] ), the following equations by [<xref ref-type="bibr" rid="scirp.59771-ref24">24</xref>] is used in this research,</p><disp-formula id="scirp.59771-formula471"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x29.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x30.png" xlink:type="simple"/></inline-formula> is total porosity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x31.png" xlink:type="simple"/></inline-formula>.</p><p>The gas flow velocity is due to advection and is assumed to follow Darcy’s law.</p><disp-formula id="scirp.59771-formula472"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x32.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x33.png" xlink:type="simple"/></inline-formula> is the intrinsic permeability of soil (m<sup>2</sup>), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x34.png" xlink:type="simple"/></inline-formula>is the gas-mixture viscosity, P is pressure (Pa) which is calculated based on the ideal gas law</p><disp-formula id="scirp.59771-formula473"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x35.png"  xlink:type="simple"/></disp-formula><p>where R is the universal gas constant (8.314<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x36.png" xlink:type="simple"/></inline-formula>) and T is absolute temperature (K).</p><p>The reaction rate of CH<sub>4</sub> is given</p><disp-formula id="scirp.59771-formula474"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x37.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x38.png" xlink:type="simple"/></inline-formula> is the maximum methane consumption rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x39.png" xlink:type="simple"/></inline-formula>; and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x41.png" xlink:type="simple"/></inline-formula> are the half-saturation constants of CH<sub>4</sub> and O<sub>2<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x42.png" xlink:type="simple"/></inline-formula></sub>, respectively. Methane oxidation is affected by many fac-</p><p>tors among which soil temperature and moisture content are more significant. Temperature, moisture, and scaling correction factors were considered for the kinetic parameters in Equation (7) as described in [<xref ref-type="bibr" rid="scirp.59771-ref18">18</xref>] . [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] developed a mechanism to relate in situ rates of oxidation to those measured in laboratory incubation experiments on homogenized and sieved soil samples under fixed environmental conditions. Their study used combined laboratory and field measurements to develop field scale Michaelis-Menten parameters to be used in conjunction with numerical models to predict methane emissions and oxidation in landfill covers and under field conditions. More details about the model can be found in [<xref ref-type="bibr" rid="scirp.59771-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.59771-ref18">18</xref>] . Since the surface of the phytocap is open to the atmosphere, the gas composition above the surface node of the model was assumed to be the atmospheric gas compositions (background), which are 21.2%v/v oxygen, 1.8 ppmv methane, 385.0 ppmv carbon dioxide and 78.8%v/v nitrogen.</p></sec><sec id="s2_3"><title>2.3. Simulations</title><p>The simulated ET cover was divided into five30-cm-thick layers with different soil properties. The top layer was assumed to be 30 cm thick and represented by the 15 cm deep soil water and soil suction sensors. The second layer was also assumed to be 30 cm thick and be represented by the sensors buried at 45 cm, etc. The top 60 cm ET cover soil was assumed to have undergone several freeze-thaw and desiccation cycles. The long-term saturated hydraulic conductivity of the top 30-cm-thick layer was assigned to be 1 &#215; 10<sup>−4</sup> cm/s. The second layer was a signed to have a saturated hydraulic conductivity of 1 &#215; 10<sup>−5</sup> cm/s. The third layer was assumed to have a 10 times lower saturated hydraulic conductivity. The hydraulic conductivity of the lowest layer was measured from an undisturbed sample as 2.7 &#215; 10<sup>−7</sup> cm/s. The hydraulic conductivity of the second layer from the bottom was assumed to be 5 times higher than the bottom layer. The porosity of the soil profile was assumed as follow: from top to down 0.45, 0.42, 0.40, 0.38, and 0.38. The long term unsaturated soil properties are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. The collected daily moisture content (moisture content sensor) and soil suction (matric potential sensor) value for a given elevation (each probe depth) were used to directly measure a field determined soil water characteristic curve (<xref ref-type="fig" rid="fig2">Figure 2</xref>). The in situ determination of a SWCC for the soil is more representative of the actual conditions than the SWCC developed in the laboratory. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the soil properties used as input into the model for all the simulated layers of the ET cover and three examples of field determined SWCCs.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Examples of measured and fitted SWCC obtained using collected data, along with all soil properties used for each layer of the simulated ET cover</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x43.png"/></fig><p>One of the major inputs to the gas transport model is the maximum methane oxidation capacity (a lab measured quantity V<sub>max</sub>) of the soil. This quantity represents the maximum capacity of bacteria in the soil to oxidize methane at room temperature. Based on our experience with measuring V<sub>max</sub> on landfill cover soils and for the purpose of this document, different simulations of two different values of V<sub>max</sub> (150, 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil) were performed. Several simulations were performed using different rates of methane loading into the ET cover. For each V<sub>max</sub>, several simulations were performed using methane loading varying from 2 to 200 gm<sup>−2</sup>∙d<sup>−1</sup>. The landfill gas entering the bottom of soil profile was partitioned equally to CH<sub>4</sub> and CO<sub>2</sub> v/v.</p></sec></sec><sec id="s3"><title>3. Results and Analysis</title><p>The output of the gas transport model consists of daily surface emissions of methane and daily percent oxidized for each simulation performed with each methane loading flux (MLF) during the modelled average one year period in Bennignton, NE. The daily simulations was repeated for different MLFs (2, 5, 10, 20, 50, 100, 200 gm<sup>−2</sup>∙d<sup>−1</sup>) and with each V<sub>max</sub>. <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> show the daily surface emissions and daily percent methane oxidation for all the simulations with different MLFs and with V<sub>max</sub> of 150and 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil, respectively.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> show that for MLF values of 2 to 5 gm<sup>−2</sup>∙d<sup>−1</sup>, noneto very little surface emissions occur during the entire year. The ET cover seems to be able to oxidize all of the incoming methane from below each day of the year, even during cold seasons and inside and outside the growing season. Complete oxidation (100%) occurs every day of the year when the MLF is lower than around 5 gm<sup>−2</sup>∙d<sup>−1</sup>. For simulations with a higher MLF values, the highest daily surface emissions and lower percent oxidation occur outside the growing season and</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Surface emissions, percent oxidized for several methane loading fluxes with V<sub>max</sub> = 150 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x44.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Surface emissions, percent oxidized for several methane loading fluxes with V<sub>max</sub> = 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> soil</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x45.png"/></fig><p>during colder periods of the year. The higher percent oxidation and the lowest surface emissions occur during the growing season and during the spring and summer seasons indicating the effects of soil temperature and water contents on surface emissions and therefore methane oxidation.</p><p>The data presented in <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> were then used to calculate average yearly methane oxidation rate and average yearly percent oxidation for each simulated methane loading. The average yearly methane oxidation rate in gm<sup>-2</sup>d<sup>-1</sup>was determined for each MLF and plotted in <xref ref-type="fig" rid="fig5">Figure 5</xref>. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows that at lower MLFs, oxidation rate is equal to the MLF and increases with increasing MLF. In this region, the ET cover is able to oxidize all of the methane coming from below. In this region, the slope of the curve shown in <xref ref-type="fig" rid="fig5">Figure 5</xref> is 1:1. In this region of low MLFs, there is no difference between the simulations with 150 and 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soilsince both ET covers can oxidize all of the incoming methane. There seems to be an MLF below which methane oxidation is total (around 7 - 8 gm<sup>−2</sup>∙d<sup>−1</sup> for both V<sub>max</sub> values). The methane loading flux at which the cover can oxidize all of the incoming methane can be considered as the MLF below which no surface emissions are measurable (No surface emissions). Above this MLF, the ET cover is not able to oxidize all of the incoming methane but still can oxidize more and more methane as the MLF increases. <xref ref-type="fig" rid="fig5">Figure 5</xref> also shows that each ET cover soil seems to have a maximum capacity to oxidize the incoming methane depending on V<sub>max</sub>. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows that for each V<sub>max</sub>, there is a point where the ET cover will not oxidize any more methane, which indicates a certain capacity of the cover soil (around 13 gm<sup>−2</sup>∙d<sup>−1</sup> and 19 gm<sup>−2</sup>∙d<sup>−1</sup> for V<sub>max</sub> of 150 and 300 respectively). <xref ref-type="fig" rid="fig5">Figure 5</xref> also shows that oxidation rate starts to decrease after a certain MLF. We believe that this is due to the fact that these results are obtained using a pressure based model. The pressure below the landfill cover is increased to increase the MLF into the cover soil. At a certain pressure (depending on the cover) the incoming flux of methane starts to inhibit the diffusion of oxygen from the upper boundary and limit the amount of methane that can be oxidized.</p><p>The shape of the graph in <xref ref-type="fig" rid="fig5">Figure 5</xref> resembles a Michaelis-Menten enzyme kinetic plot of a biological reactions response to increasing concentrations of a substrate. In landfill ET cover, soil methane oxidation is conducted by a biological system and it behaves as such. When substrate (CH<sub>4</sub>) is supplied, the cover’s rate of CH<sub>4</sub> uptake is linear to a point, and then the system apparently becomes saturated. This response must be due to the oxygen levels to which the bacteria are exposed in addition to temporal variability in soil temperature and moisture.</p><p>The same simulation results were used to calculate the average percent year methane oxidation, and plotted versus MLF for each V<sub>max</sub> in <xref ref-type="fig" rid="fig6">Figure 6</xref>. <xref ref-type="fig" rid="fig6">Figure 6</xref> shows that there seems to be a methane loading rate below which methane oxidation is equal to 100%. Above this methane loading, the cover is not able to oxidize all of the incoming methane. Therefore, percent oxidation starts to decrease as the methane loading increases. As expected, at any given MLF, ET covers with higher V<sub>max</sub> have higher percent methane oxidation.</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Methane oxidation rate versus MLF for simulations with V<sub>max</sub> = 150 and 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x46.png"/></fig></sec><sec id="s4"><title>4. Conclusions and Practical Implications</title><p>One way to estimate uncontrolled emissions or fugitive emissions from the surface of landfills is to use the AP- 42 protocol proposed by the United States Environmental Protection Agency (USEPA, 1997). AP-42, when applied to landfill methane surface emissions, can be written as follows:</p><disp-formula id="scirp.59771-formula475"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-9402667x47.png"  xlink:type="simple"/></disp-formula><p>where CM<sub>P</sub> is the controlled mass emissions of methane (kg/year), UM<sub>P</sub> is the methane generation from the waste mass in kg/year (estimated by LANDGEM or any other allowed model), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x48.png" xlink:type="simple"/></inline-formula>is the collection efficiency of the landfill gas collection system. The collection efficiency of the gas collection system can be assumed the default values of 75% assigned for soil covers. The remaining 25% of the generated methane can be assumed to escape through the landfill ET cover such as the one simulated in this study, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x49.png" xlink:type="simple"/></inline-formula>is the percent oxidation or fraction of methane oxidized in the cover soil. The USEPA has also allowed the use of 10% to account for methane oxidation that can occur in landfill cover soils.</p><p>One application of this model is to be used in conjunction of AP-42 guidelines but with a modeled methane oxidation, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x50.png" xlink:type="simple"/></inline-formula>instead of the default value of 10% typically assumed in AP-42. The use of the correlations of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-9402667x51.png" xlink:type="simple"/></inline-formula>, shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>, can encourage the use of ET covers and provide an estimate of fugitive methane emis-</p><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Percent methane oxidation versus MLF for simulations with V<sub>max</sub> = 150 and 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x52.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Correlation of Percent methane oxidation versus MLF for simulations with V<sub>max</sub> = 150 and 300 nmol∙s<sup>−1</sup>∙g<sup>−1</sup> dry soil</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-9402667x53.png"/></fig><p>sions, along with quantifying the improvement of performance (emissions and oxidation) of ET covers. Such protocol can help decision makers quantify additional methane oxidation capabilities of ET covers. The modeled percent oxidation for each V<sub>max</sub> was expressed as a power function of methane loading flux (MLF) as shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. The methane loading flux is estimated as the 25% of generation (methane escaping the gas collection system) divided by the surface area of the ET covered landfill.</p></sec><sec id="s5"><title>Cite this paper</title><p>TarekAbichou,TarekKormi,ChengWang,HaykelMelaouhia,TerryJohnson,StephenDwyer, (2015) Use of Evapotranspiration (ET) Landfill Covers to Reduce Methane Emissions from Municipal Solid Waste Landfills. Journal of Water Resource and Protection,07,1087-1097. doi: 10.4236/jwarp.2015.713089</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.59771-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Albrecht, B. and Benson, C. (2001) Effect of Desiccation on Compacted Natural Clays. J. of Geotech. and Geoenv. Eng., ASCE, 127, 67-76.</mixed-citation></ref><ref id="scirp.59771-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Benson, C. and Khire, M. (1995) Earthen Covers for Semi-Arid and Arid Climates, ASCE 1995 National Convention on Landfill Closures-Environmental Protection and Land Recovery. Geotechnical Special Publication No. 53, 201-217.</mixed-citation></ref><ref id="scirp.59771-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Stormont, J. and Morris, C. (1998) Method to Estimate Water Storage Capacity of Capillary Barriers. 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