<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>2071-0054</journal-id>
<journal-title><![CDATA[Revista Ciencias Técnicas Agropecuarias]]></journal-title>
<abbrev-journal-title><![CDATA[Rev Cie Téc Agr]]></abbrev-journal-title>
<issn>2071-0054</issn>
<publisher>
<publisher-name><![CDATA[Universidad Agraria de La Habana]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S2071-00542012000400001</article-id>
<title-group>
<article-title xml:lang="es"><![CDATA[Simulación Numérica de la Interacción Suelo-Apero Mediante el Método de Elementos Discretos]]></article-title>
<article-title xml:lang="en"><![CDATA[Numerical Simulation of Soil-Tool Interaction by Discrete Element Method]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[López Bravo]]></surname>
<given-names><![CDATA[Elvis]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Herrera Suárez]]></surname>
<given-names><![CDATA[Miguel]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[González Cueto]]></surname>
<given-names><![CDATA[Omar]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Tijskens]]></surname>
<given-names><![CDATA[Engelbert]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Ramon]]></surname>
<given-names><![CDATA[Herman]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Central de las Villas  ]]></institution>
<addr-line><![CDATA[Villa Clara ]]></addr-line>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>12</month>
<year>2012</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>12</month>
<year>2012</year>
</pub-date>
<volume>21</volume>
<numero>4</numero>
<fpage>05</fpage>
<lpage>11</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://scielo.sld.cu/scielo.php?script=sci_arttext&amp;pid=S2071-00542012000400001&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://scielo.sld.cu/scielo.php?script=sci_abstract&amp;pid=S2071-00542012000400001&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://scielo.sld.cu/scielo.php?script=sci_pdf&amp;pid=S2071-00542012000400001&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[Discrete Element Method (DEM) was used to simulate the soil-tool interaction. The model is based on the action of normal, shear, cohesion and friction forces into the cohesive granular medium, calculated as a function of micro-mechanical properties. Macro-mechanical properties of soil-soil and soil-metal were used to determining the micro parameters on the model. In order simulate the tillage operations a soil virtual block was generated in hexagonal compacted array using 45 000 spherical particles forming a cohesive block. A soil-bin installation was conditioned to measuring the draft force in hard-dry and soft-wet soil condition to compare the results with simulation tests. The comparison showed a small under predicted behavior of the model for soft-wet soil; however the results become more accurate toward hard-dry soil conditions. The density changes during simulations and pressures distributions below the tillage tool path is showed, given a dynamic representation of soil internal tension and loosening after tillage operation.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[El método de elementos discretos (DEM) fue utilizado para simular la interacción del suelo con la herramienta de labranza. El mismo se basa en la acción que ejercen las fuerzas normal, tangencial, cohesión y fricción en un medio granular cohesivo, a partir de su determinación a escala micro-mecánicas. Las propiedades macroscópicas que intervienen en el contacto suelo-suelo sirven como parámetros macros los cuales son usados para determinar los parámetros micros del modelo. Para la simulación de la labranza se realizó la generación virtual de un bloque de suelo con un total de 45 000 partículas esféricas, formando un bloque cohesivo. Para verificar los resultados de la simulación se acondicionó un canal de suelo para dos condiciones extremas: seco-endurecido y húmedo-suelto. Los resultados mostraron una tendencia del modelo a sobreestimar la magnitud de la fuerza de tiro para el suelo suelto y con alta humedad, Sin embargo el modelo resultó más preciso para la condición de alta densidad. Se obtuvieron además las distribuciones de densidad del suelo en las diferentes secciones del bloque virtual así como los resultados de la distribución de fuerzas en las capas comprimidas debido al paso de la herramienta de labranza.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Tillage]]></kwd>
<kwd lng="en"><![CDATA[modeling]]></kwd>
<kwd lng="en"><![CDATA[draft force]]></kwd>
<kwd lng="en"><![CDATA[density]]></kwd>
<kwd lng="es"><![CDATA[labranza]]></kwd>
<kwd lng="es"><![CDATA[modelo]]></kwd>
<kwd lng="es"><![CDATA[fuerza de tiro]]></kwd>
<kwd lng="es"><![CDATA[densidad]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[ <p align="right"><b><font size="2" face="Verdana">ARTÍCULO ORIGINAL</font></b></p>    <p align="right">&nbsp;</p>    <p align="justify"><b><span class="medium-text">  <font size="4" face="Verdana">Numerical Simulation of Soil-Tool Interaction by  Discrete Element Method</font></span></b></p>    <p align="justify">&nbsp;</p>    <p align="justify"><b><font face="Verdana">Simulación  Numérica de la Interacción Suelo-Apero Mediante el Método de Elementos Discreto</font></b></p>    <p align="justify">&nbsp;</p>    <p align="justify">&nbsp;</p>    <p align="justify"><b><font size="2" face="Verdana">M.Sc.  Elvis López Bravo<sup>1</sup>, Dr. C. Miguel Herrera Suárez<sup>1</sup>, Dr. C.  Omar González Cueto<sup>1</sup>,&nbsp; Prof. Engelbert Tijskens, Herman Ramon</font></b><sup><b><font face="Verdana" size="2">2</font></b></sup></p>    <p class="titulos-articulo"><font size="2" face="Verdana">I.  Universidad Central de Las Villas, Dpto. Mecanización Agropecuaria, Villa Clara,  Cuba.    <br> II. Division of Mechatronics, Biostatistics and Sensors (MeBioS), Department  of Biosystems, Faculty of Bioscience Engineering, Kasteelpark Arenberg 30, B-3001  Heverlee, Belgium.</font></p>    ]]></body>
<body><![CDATA[<p class="titulos-articulo">&nbsp;</p>    <p class="titulos-articulo">&nbsp;</p><hr>      <p class="resumen-ingles"><b><font size="2" face="Verdana"> ABSTRAC</font></b></p>    <p class="resumen-ingles" style="margin-top: 0; margin-bottom: 0">  <font size="2" face="Verdana">Discrete Element Method (DEM) was used to simulate  the soil-tool interaction. The model is based on the action of normal, shear,  cohesion and friction forces into the cohesive granular medium, calculated as  a function of micro-mechanical properties. Macro-mechanical properties of soil-soil  and soil-metal were used to determining the micro parameters on the model. In  order simulate the tillage operations a soil virtual block was generated in hexagonal  compacted array using 45 000 spherical particles forming a cohesive block. A soil-bin  installation was conditioned to measuring the draft force in hard-dry and soft-wet  soil condition to compare the results with simulation tests. The comparison showed  a small under predicted behavior of the model for soft-wet soil; however the results  become more accurate toward hard-dry soil conditions. The density changes during  simulations and pressures distributions below the tillage tool path is showed,  given a dynamic representation of soil internal tension and loosening after tillage  operation.</font></p>    <p class="resumen-ingles" style="margin-top: 0; margin-bottom: 0">&nbsp;</p>    <p class="resumen-ingles" style="margin-top: 0; margin-bottom: 0"><FONT FACE="Verdana" SIZE="2"><b>Keywords:</b>  Tillage, modeling, draft force, density.</FONT></p><hr>     <p class="resumen-espa-ol"><b><font size="2" face="Verdana">RESUMEN</font></b></p>    <p class="resumen-espa-ol"><font size="2" face="Verdana">El  método de elementos discretos (DEM) fue utilizado para simular la interacción  del suelo con la herramienta de labranza. El mismo se basa en la acción que ejercen  las fuerzas normal, tangencial, cohesión y fricción en un medio granular cohesivo,  a partir de su determinación a escala micro-mecánicas. Las propiedades macroscópicas  que intervienen en el contacto suelo-suelo sirven como parámetros macros los cuales  son usados para determinar los parámetros micros del modelo. Para la simulación  de la labranza se realizó la generación virtual de un bloque de suelo con un total  de 45 000 partículas esféricas, formando un bloque cohesivo. Para verificar los  resultados de la simulación se acondicionó un canal de suelo para dos condiciones  extremas: seco-endurecido y húmedo-suelto. Los resultados mostraron una tendencia  del modelo a sobreestimar la magnitud de la fuerza de tiro para el suelo suelto  y con alta humedad, Sin embargo el modelo resultó más preciso para la condición  de alta densidad. Se obtuvieron además las distribuciones de densidad del suelo  en las diferentes secciones del bloque virtual así como los resultados de la distribución  de fuerzas en las capas comprimidas debido al paso de la herramienta de labranza.</font></p>    <p class="resumen-espa-ol"><font size="2" face="Verdana"><b>Palabras  clave:</b> labranza, modelo, fuerza de tiro, densidad.</font></p><hr>     <p class="resumen-espa-ol">&nbsp;</p>    ]]></body>
<body><![CDATA[<p class="resumen-espa-ol">&nbsp;</p>    <p class="resumen-espa-ol"><b><font face="Verdana">INTRODUCTION</font></b></p>    <p class="resumen-espa-ol"><font size="2" face="Verdana">Draft  force prediction, clod sizes distribution and damages by erosion have been some  of the motivation topics for modeling soil-tillage interaction. Data from field  process and lab experiments are combined on mathematical models; supporting by  the increment on informatics resources more accurate, fasters and extended prognostics  are performed. Computational techniques as well as finite element methods (FEM),  discrete element methods (DEM), artificial neural network (ANN) and computational  fluid dynamics (CFD) are indistinctly used with different purposes in soil simulation.  Important approaching of rheological soil behavior is the result of transition  from quasi-static to dynamic analysis (Karmakar &amp; Kushwaha, 2006). Optimization  for tillage tools focused on geometrical modification has been carried out on  moldboard ploughs, obtaining significant draft force reduction required to move  the tool through different soil conditions (Shrestha et al., 2001; Godwin, 2007).  Field performance of the implements for futures applications in soil-ecosystem  were evaluated in the nineties decade, testing several variant of tools shapes  and operations speed and getting the draft forces requirement. The most efficient  tools designs were evaluated at farm level correlating the energy supply and seedbed  quality (Perdok &amp; Kouwenhoven, 1994). Prediction of draught requirements by  ANN for three designs of moldboard plows, tested in sandy loam soil under different  operating ranges and soil conditions, showed a good correlation in comparison  with results obtaining from prediction equations (Roul et al., 2009). Considering  the soil as a continuum medium, several constitutive models have been created  and improved. Modified Cam-Clay model was implemented focus on deriving time dependent  effect, the model included soil anisotropic and creep behavior, as a result gyration  and expansion of load affected the principal stress redirection, confirmation  of simulation was made using un-drained shear and creep test (Ahmari &amp; Ahmadi,  2009). Von-Mises yield criterion on perfectly plastic model was applied using  Lagrangian method; including strain-softening and rate dependent, the authors  present a numerical model for cone penetration into soft clay soil, the influence  of stiffness index, in-situ stress anisotropy and roughness were theoretically  correlated and compared with the cavity expansion theory (Liyanapathirana, 2009).    <br>      <br> Several studies by FEM have been conducted using simples and complexes geometries  of tools projected in two and three dimensions, with the objective of determining  the effect of cutting speed and blade angles related to draft force variation  during soil-tool interaction (Mouazen &amp; Neményi, 1999; Mootaz et al., 2003;  Abo-Elnor et al., 2004; Sahu &amp; Raheman, 2006; Gebregziabher et al., 2007;  Davoudi et al., 2008).    <br>     <br> Several studies have been carried out to simulating  the soil behavior in Cuban soil focus in tillage operation and soil management.  The methodology to determine from mechanical soil test the parameters needed to  fill the FEM model was used to predicting the result of soil tensional state(Herrera,  2001). The parameters of the model for soil tool interaction was determined and  proof the accurate of elastic-plastics formulation obtaining best results using  a Drucker-Prager model (Herrera et al., 2008). Triaxial compression test and shear  test have been simulated in different Cuban soils to predict the soil behavior  related to compaction by the action of the inflate wheel pressures and transporting  load (Gonzalez et al., 2007; Gonzalez et al., 2009).    <br>     <br> Discrete medium  is widely applied for simulation of dynamic process, having an extend field in  soils engineering applications. The principal vantage over continuum methods is  the capacity to represent the interaction among particles happen in granular medium  (Tadesse, 2004). Many contact models can be included depending on how each element  interacts with each other, these contacts models rules the behavior of the overall  medium, the micro-properties parameters for the model will be deduced from soil  mechanical properties. The rheological simulation can result on an accurate prognostic  about soil behavior and draft force requirements.    <br>     ]]></body>
<body><![CDATA[<br> The goal for the present  study is to simulate the soil-tool interaction to predicting the draft forces  and soil particles behavior in tillage operations by mean of macro-scale model  implemented on Discrete Element Method.</font></p>    <p class="resumen-espa-ol">&nbsp;</p>    <p class="subtitulo-1"><b><font face="Verdana">METHODS</font></b></p>    <p class="normal" align="justify"><font size="2" face="Verdana">Model  description. Classical DEM model proposed by Cundall and Strack (Cundall &amp;  Strack, 1979), is used to compute the interaction between soil particles and tillage  tool, two kinds of contacts were implemented: soil-soil and soil-tool, for both  calculations the same contact scheme is applied, changing only cause of mechanical  properties which are obtained from regression equation according to the specifics  soil physical desire condition (López, 2011), The macroscopic parameters included  in the model bring a physic-mechanical characterization of the soil namely: Elastic  Young’s modulus (E), Poisson ratio (n), cohesion (c), adhesion (ca), internal  friction (f) and metal-soil friction (d). The model dealing with normal, shear,  gravity, cohesion and friction forces (<a href="#">Figure 1</a>).</font></p>    <p class="normal" align="center"><A NAME=""></A>  <img border="0" src="/img/revistas/rcta/v34n1/img/f011412.gif" width="625" height="290"></p>    
<p class="normal">&nbsp;</p>    <p class="normal"><font size="2" face="Verdana">The  micro parameters for the model are dynamic calculated from equations that working  with geometrical elements and macro-properties of the particles in contact at  each time step using. The force in normal direction is calculated by:</font></p>    <p class="normal" align="right">&nbsp;</p>    <p align="right" class="formulas">  <font size="2" face="Verdana"><span class="normal"><font size="2" face="Verdana"><a name="e1"></a></font></span>  <img border="0" src="/img/revistas/rcta/v34n1/img/e0101412.gif" width="383" height="23"></font></p>    
<p class="donde"><font size="2" face="Verdana">Where  kn mean the normal spring, Dun is the variation of normal overlapping, hn is the  viscous damping and Dt is the time step variation.</font></p>    ]]></body>
<body><![CDATA[<p class="normal"><font size="2" face="Verdana">The  equation to calculate normal spring encloses the relationship between elastic  properties and dimensional parameters, it is written, as:</font></p>    <p class="normal" align="right"><font size="2" face="Verdana"><a name="e2"></a></font>  <img border="0" src="/img/revistas/rcta/v34n1/img/e0201412.gif" width="400" height="41"></p>    
<p class="donde"><font size="2" face="Verdana">Where  Eab is the equivalent Young’s modulus of the two contact materials, Aint is the  interior area of the contact and Deq is the equivalent distance between the two  objects, the other part of the equation is the relationship between poison’s ratio  n with loading path coefficient ak, softening factor bk and interaction range  gk (Hentz et al., 2004).</font></p>    <p class="normal"><font size="2" face="Verdana">The  force in tangential direction is calculated by:</font></p>    <p class="formulas" align="right"><font size="2" face="Verdana"><a name="e3"></a></font>  <img border="0" src="/img/revistas/rcta/v34n1/img/e0301412.gif" width="389" height="21"></p>    
<p class="donde"><font size="2" face="Verdana">Where  ks is the shear spring, Dus is the variation of tangential overlapping and hs  represents the viscous damping in tangential direction. The value of ks depends  on kn, been obtained by:</font></p>    <p class="formulas" align="right"><font size="2" face="Verdana"><span class="normal"><font size="2" face="Verdana"><a name="e4"></a></font></span>&nbsp;</font><img border="0" src="/img/revistas/rcta/v34n1/img/e0401412.gif" width="353" height="29"></p>    
<p class="normal"><font size="2" face="Verdana">The  viscous damping in normal and tangential direction is determined by:</font></p>    <p class="formulas" align="right"><span class="donde"><font size="2" face="Verdana"><a name="e5"></a></font></span>  <img border="0" src="/img/revistas/rcta/v34n1/img/e0501412.gif" width="356" height="39"></p>    
<p class="donde"><font size="2" face="Verdana">Where  b is the viscous damping coefficient; ma and mb are the mass of the two objects  in contact.</font></p>    ]]></body>
<body><![CDATA[<p class="normal"><font size="2" face="Verdana">Inter-particles  cohesion force acts when overlap increases over the soil Cauchy strain obtaining  a attraction force which keeping the particles together. The relation between  micro-friction and micro-cohesion is captured by interpolation procedure obtaining  the following power relationship (Utili &amp; Nova, 2008):</font></p>    <p class="formulas" align="right"><font size="2" face="Verdana"><span class="normal"><font size="2" face="Verdana"><a name="e6"></a></font></span>&nbsp;</font><img border="0" src="/img/revistas/rcta/v34n1/img/e0601412.gif" width="362" height="39"></p>    
<p class="donde"><font size="2" face="Verdana">Where  c is the cohesion between two objects in contact from lab experiment, fm is micro-friction  coefficient, k3 and k4 are two material constants related with porosity and particles  sizes distribution in the simulated medium.</font></p>    <p class="subt-tulo"><b><font size="2" face="Verdana">Soil  block generation</font></b></p>    <p class="normal"><font size="2" face="Verdana">Soil  block at 650 x 400 x 300 mm was generated filling a rectangular box with 45 000  spherical particles (<a href="#">Figure 2a</a>). The hexagonal compacted spatial  array was used as the methods to get the efficient distribute of particles. The  whole particles were submitted to free fall into the mentioned box, the second  step was pressing from the top to the bottom. The horizontal press (red color  plane) is moved at constant velocity at 0,2 m/min reducing the space into the  container and getting the desire specimen density (<a href="#">Figure 2b</a>).  Sizes of particles were distributed on three different layers with radius at 8-10;  6-5 and 3-4 mm at the top, center, and bottom respectively.</font></p>    <p class="normal" align="center"><A NAME=""></A>  <img border="0" src="/img/revistas/rcta/v34n1/img/f0201412.gif" width="580" height="181"></p>    
<p class="estilo-de-fotos-y-figuras">&nbsp;</p>    <p class="cuerpo-de-texto"><font size="2" face="Verdana">The  soil block was generated in three different physical condition by mean of modifies  in water contents (u) and soil bulk densities (</font><span style="font-size: 10.0pt; line-height: 115%; font-family: Symbol">g)</span><font size="2" face="Verdana">.  The conditions obtained by simulation represent soft-wet (r = 1,1 g/cm3, u = 30%),  friable (r = 1,2 g/cm3, u = 18%) and hard-dry soil (r = 1,4, g/cm3, u = 10%).  The parameters used for each simulation is showing in <A HREF="#t1">Table1</A>.</font></p>    <p class="titulo-tablas" align="center"><span class="subt-tulo"><b><font size="2" face="Verdana"><a name="t1"></a></font></b></span>  <img border="0" src="/img/revistas/rcta/v34n1/img/T0101412.gif" width="460" height="162"></p>    
<p class="subt-tulo"><b><font size="2" face="Verdana">Soil  Bin test</font></b></p>    ]]></body>
<body><![CDATA[<p class="normal" align="justify"><font size="2" face="Verdana">In  order to compare the draft forces obtained by simulation in soft-wet and hard-dry  soil conditions a 1,5 per 8 m soil-bin was conditioned, filled by Vertisol soil,  the same material used to carry out the lab test explained above (<a href="#">Figure  3a</a>). The force reactions in longitudinal and vertical direction are measured  by an extended orthogonal ring transducer fixed and calibrated between tool and  trolley (<a href="#">Figure 3b</a>). The CrioData acquisition system was configured  using the LabView application and running in a HP laptop, taking 200 samples per  second along the measurement time.</font></p>    <p class="normal" align="center"><A NAME=""></A>  <img border="0" src="/img/revistas/rcta/v34n1/img/f0301412.gif" width="523" height="302"></p>    
<p class="subtitulo-1">&nbsp;</p>    <p class="subtitulo-1">&nbsp;</p>    <p class="subtitulo-1"><b><font face="Verdana">RESULTS  AND DISCUSSION</font></b></p>    <p class="subtitulo-sin-espacio"><b><font size="2" face="Verdana">Comparison  between soil-bin and simulation test</font></b></p>    <p class="normal" align="justify"><font size="2" face="Verdana">The  average draft force obtained during the soil-bin test in soft-wet condition represented  by the dash blue line in <a href="#f4">Figure 4</a>, shows the small under-prediction  quality of the model for relative low range of force demanding system. The draft  force measured by the measuring system (red color line) in the lab condition was  bigger than the force obtained in simulation test. Nevertheless the error of 97  N is an acceptable value considering the spatial huge variation of soil physical  properties and the corresponding over-dimension of tiller in agricultural practices.  On the other hand 1,41 kN draft force average measured in hard-dry soil condition  (green dash line), shows more close force prediction by the model exhibiting a  standard error of 34 N.</font></p>    <p class="normal" align="justify"><font size="2" face="Verdana">One  of the reasons why draft force decrease is the particle packing which affects  the strength of the simulated soil. The cylindrical shapes for all particles and  a limited sizes distribution increase the empties spaces into the virtual block  of soil, it is coherent with soil porosity, however in real soil large amount  of small particles are filled a considerable intergranular spaces what increase  the soil stiffness. For hard-soil the overlap become larger and bulk density also  increase obtaining a proportional pore homogenization and a consequently strength  increment.</font></p>    <p class="normal" align="center"><a name="f4"></a> <img border="0" src="/img/revistas/rcta/v34n1/img/f0401412.gif" width="433" height="283"></p>    
<p class="subt-tulo"><b><font size="2" face="Verdana">Tillage  simulation for different soil conditions</font></b></p>    ]]></body>
<body><![CDATA[<p class="normal" align="justify"><font size="2" face="Verdana">The  comparison among draft forces results from soft-wet, friable and hard-dry conditions  obtained from tillage simulations with cultivator tool (<a href="#">Figure 5</a>),  shows an increment respect one another. The smaller draft force belong to soft-wet  condition as was expected, the content of water and soil bulk density affect all  macro-mechanical properties and consequently the micro-properties in the model,  however the predominant effect is attributably of high moisture. Inversely the  higher force magnitude was reached on hard-dry soil condition as a consequence  of the increment in soil stiffness.</font></p>    <p class="normal" align="center"><A NAME=""></A>  <img border="0" src="/img/revistas/rcta/v34n1/img/f0501412.gif" width="538" height="274"></p>    
<p class="estilo-de-fotos-y-figuras">&nbsp;</p>    <p class="normal" align="justify"><font size="2" face="Verdana">Particles  compression and decompression take places during movement of the tool through  the soil, as a result the fluctuation forces patter with different proportion  for each soil conditions appear, the amount of bonds broken up at the same time  determine the minimum and maximum values of the force. The fluctuation force on  hard-dry condition is also larger than two other treatments, caused by more fragility  among particles. Patter of plastic flow characterizes the soil movement on soft-wet  condition, while fragile patter is more representative on hard-dry soil followed  by larger number of clods formation.</font></p>    <p class="normal" align="justify"><font size="2" face="Verdana">Variation  on particles bulk density calculated from seven parallels blocks (<a href="#f6">Figure  6a</a>), arranged in longitudinal direction after tillage simulation shows a different  patter of increment (<a href="#f6">Figure 6b</a>).</font></p>    <p class="estilo-de-fotos-y-figuras" align="center"><a name="f6"></a>  <img border="0" src="/img/revistas/rcta/v34n1/img/f0601412.gif" width="457" height="255"></p>    
<p class="normal" align="justify"><font size="2" face="Verdana">In  hard-dry soil condition bulk density decrease mainly at the center of the section  (<a href="#f6">Figure 6b),</a> by the action of the main body of the tool, for  the section above lateral blades bulk density remain with discrete reduction.  That behavior is also showed for simulation in friable soil condition, though  more uniform density was obtained along transversal section of the tool meaning  a rising in the soil loosing index. Under wet-soil condition the action of the  lateral blades become nil, only small amount of particles loosening were found  at the wedge position section of the tool while the other part of the block remain  undisturbed.</font></p>    <p class="normal" align="justify"><font size="2" face="Verdana">Graphical  representation of particles forces on the horizontal plane below the tool path  in the trajectory of 600mm from left to right obtained in the simulation of dry-hard  and friable soil condition highlight the bigger particles tension register in  the most compacted soil (<a href="#">Figure 7a</a>), the amount of particles submitted  to pressure also grown up and some picks are obtaining at the current tool position.</font></p>    <p class="normal" align="center"><A NAME=""></A>  <img border="0" src="/img/revistas/rcta/v34n1/img/f0701412.gif" width="541" height="252"></p>    
<p class="normal"><font size="2" face="Verdana">Less  forces values and quite reduction in pressured area characterize the resultant  forces for soil in friable conditions (<a href="#">Figure 7b</a>).Accordingly  the bigger particles force the consequent increment on internal tension and plow  pan formation.</font></p>    ]]></body>
<body><![CDATA[<p class="normal">&nbsp;</p>    <p class="subtitulo-1"><b><font face="Verdana">CONCLUSIONS</font></b></p>    <p><font size="2" face="Verdana">The  discrete element method provides the fundamental formulation and geometrical tools  to implementing the particles contacts in a macro-scale representation, deriving  from soil macro-properties the micro properties for the model.    <br>     <br> The experimental  measurements in a soil-bin using a tool designed according to agricultural treatments  of soil cultivation allow determining the draft forces requirement for a tool  in tillage operations submitted to different conditions of moistures and bulk  densities.    <br>     <br> Comparison between tillage draft forces obtained from soil-bin  and discrete simulation in soft-wet (r = 1,1 g/cm3, u = 30%), and hard-dry (r  = 1,4, g/cm3, u = 10%) soil conditions showed an adequate prediction forces with  standard error at 97 and 34 N respectively, the model tended to under-predict  the magnitude of the force in soft-wet condition attributable to larger amount  of pores wish reduces the soil strength.    <br>     <br> By mean of soil tillage simulation  by cultivator tool in soft-wet, friable and hard-dry soil conditions can be evaluated  the variation of draft forces, the results obtained by simulation are consistent  with the soil physical conditions giving a criteria of soil fragility and plasticity  according to the pattern of force-displacement curve.    <br>     ]]></body>
<body><![CDATA[<br> Soil loosening  depending on the position of the implement shows a maximum level in friable (r  = 1,2 g/cm3, u = 18%) soil, the bulk density level off from 1,2 to 1,12g/cm3 at  the center of the tool decreasing gradually toward both sides, a different pattern  was found in soft-wet soil where the bulk density decrease slightly only at the  center tool path.    <br>     <br> Particles forces distribution obtained in the plane  below to the path of the tool in the simulated soil block show rising values for  dry-hard soil, denoting maximum pressures at the current tool position, also the  tension surface increase in comparison with friable soil condition becoming this  area prone to plow pan formation.</font></p>    <p>&nbsp;</p>    <p class="subtitulo-1"><b><font face="Verdana">REFERENCES</font></b></p>    <p><font size="2" face="Verdana">1.  ABO-ELNOR, M.; R. HAMILTON &amp; J. T. 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<body><![CDATA[<p>&nbsp;</p><font size="2" face="Verdana"> </font>     <p class="texto-nota-pie"><font size="2" face="Verdana">Recibido:  15 de mayo de 2011    <br> Aprobado: 20 de julio de 2012</font></p>    <p class="texto-nota-pie">&nbsp;</p>    <p class="texto-nota-pie">&nbsp;</p>    <p class="texto-nota-pie"><i><font size="2" face="Verdana">Elvis  López Bravo, </font></i><font face="Verdana"><font size="2">Prof. Auxiliar, Universidad  Central de Las Villas, Dpto. Mecanización Agropecuaria, Villa Clara, CP: 54830.  Correo electrónico: </font> <a href="mailto:elvislb@uclv.edu.cu"><font size="2">elvislb@uclv.edu.cu</font></a></font></p>&nbsp;       ]]></body><back>
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