<?xml version='1.0' encoding='utf-8'?>
<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:contributor>Frank W. Schwartz</dc:contributor>
  <dc:contributor>Warren W. Wood</dc:contributor>
  <dc:contributor>S. P. Garabedian</dc:contributor>
  <dc:contributor>D.R. LeBlanc</dc:contributor>
  <dc:creator>Hubao Zhang</dc:creator>
  <dc:date>1998</dc:date>
  <dc:description>&lt;p&gt;&lt;span&gt;A multispecies numerical code was developed to simulate flow and mass transport with kinetic adsorption in variable-density flow systems. The two-dimensional code simulated the transport of bromide (Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;), a nonreactive tracer, and lithium (Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;), a reactive tracer, in a large-scale tracer test performed in a sand-and-gravel aquifer at Cape Cod, Massachusetts. A two-fraction kinetic adsorption model was implemented to simulate the interaction of Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;with the aquifer solids. Initial estimates for some of the transport parameters were obtained from a nonlinear least squares curve-fitting procedure, where the breakthrough curves from column experiments were matched with one-dimensional theoretical models. The numerical code successfully simulated the basic characteristics of the two plumes in the tracer test. At early times the centers of mass of Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;and Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;sank because the two plumes were closely coupled to the density-driven velocity field. At later times the rate of downward movement in the Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume due to gravity slowed significantly because of dilution by dispersion. The downward movement of the Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume was negligible because the two plumes moved in locally different velocity regimes, where Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;transport was retarded relative to Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;. The maximum extent of downward transport of the Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume was less than that of the Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume. This study also found that at early times the downward movement of a plume created by a three-dimensional source could be much more extensive than the case with a two-dimensional source having the same cross-sectional area. The observed shape of the Br&lt;/span&gt;&lt;sup&gt;−&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume at Cape Cod was simulated by adding two layers with different hydraulic conductivities at shallow depth across the region. The large dispersion and asymmetrical shape of the Li&lt;/span&gt;&lt;sup&gt;+&lt;/sup&gt;&lt;span&gt;&lt;span&gt;&amp;nbsp;&lt;/span&gt;plume were simulated by including kinetic adsorption-desorption reactions.&lt;/span&gt;&lt;/p&gt;</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>10.1029/97WR02918</dc:identifier>
  <dc:language>en</dc:language>
  <dc:publisher>American Geophysical Union</dc:publisher>
  <dc:title>Simulation of variable-density flow and transport of reactive and nonreactive solutes during a tracer test at Cape Cod, Massachusetts</dc:title>
  <dc:type>article</dc:type>
</oai_dc:dc>