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	<id>https://www.enviro.wiki/index.php?action=history&amp;feed=atom&amp;title=Dispersion_and_Diffusion</id>
	<title>Dispersion and Diffusion - Revision history</title>
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	<updated>2026-04-15T09:59:59Z</updated>
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	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14219&amp;oldid=prev</id>
		<title>Jhurley: Redirected page to Groundwater Flow and Solute Transport</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14219&amp;oldid=prev"/>
		<updated>2020-12-21T22:17:51Z</updated>

		<summary type="html">&lt;p&gt;Redirected page to &lt;a href=&quot;/index.php?title=Groundwater_Flow_and_Solute_Transport&quot; title=&quot;Groundwater Flow and Solute Transport&quot;&gt;Groundwater Flow and Solute Transport&lt;/a&gt;&lt;/p&gt;
&lt;a href=&quot;https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;amp;diff=14219&amp;amp;oldid=14204&quot;&gt;Show changes&lt;/a&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14204&amp;oldid=prev</id>
		<title>Jhurley: /* Matrix Diffusion */</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14204&amp;oldid=prev"/>
		<updated>2020-12-21T18:19:17Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Matrix Diffusion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 18:19, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l123&quot; &gt;Line 123:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 123:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt;Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;3&lt;/del&gt;). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 4.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt;Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;4&lt;/ins&gt;). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 4. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;In some cases, matrix diffusion can maintain contaminant concentrations in more permeable zones at greater than target cleanup goals for decades or even centuries after the primary sources have been addressed&amp;lt;ref&amp;gt;Chapman, S.W. and Parker, B.L., 2005. Plume persistence due to aquitard back diffusion following dense nonaqueous phase liquid source removal or isolation. Water Resources Research, 41(12): W12411.&amp;#160; [https://doi.org/10.1029/2005WR004224 DOI: 10.1029/2005WR004224] &amp;amp;nbsp;&amp;amp;nbsp; Free access article from [https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2005WR004224 American Geophysical Union]&amp;lt;/ref&amp;gt; &lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
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&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14203&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14203&amp;oldid=prev"/>
		<updated>2020-12-21T18:08:45Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 18:08, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l116&quot; &gt;Line 116:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 116:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;3&lt;/del&gt;. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;[[File:ADRFig2.PNG | thumb | right | 350px | Figure 3. Predicted variation in macrodispersivity with distance for varying &amp;#039;&amp;#039;σ&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;Y&amp;#039;&amp;#039; and correlation length = 3 m.]]&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;4&lt;/ins&gt;. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;2 &lt;/del&gt;shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values were in the range of 0.5 to 5 m.&amp;#160; Zech, et al. (2015)&amp;lt;ref&amp;gt;Zech, A., Attinger, S., Cvetkovic, V., Dagan, G., Dietrich, P., Fiori, A., Rubin, Y. and Teutsch, G., 2015. Is unique scaling of aquifer macrodispersivity supported by field data? Water Resources Research, 51(9), pp.7662-7679.&amp;#160; [https://doi.org/10.1002/2015WR017220 DOI: 10.1002/2015WR017220]&amp;amp;nbsp;&amp;amp;nbsp; Free access article from [https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1002/2015WR017220 American Geophysical Union]&amp;lt;/ref&amp;gt; presented moderate and high reliability measurements of longitudinal macrodispersivity versus distance. Typical values of the longitudinal macrodispersivity varied from 0.1 to 10 m, with much lower values for transverse and vertical dispersivities. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;3 &lt;/ins&gt;shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values were in the range of 0.5 to 5 m.&amp;#160; Zech, et al. (2015)&amp;lt;ref&amp;gt;Zech, A., Attinger, S., Cvetkovic, V., Dagan, G., Dietrich, P., Fiori, A., Rubin, Y. and Teutsch, G., 2015. Is unique scaling of aquifer macrodispersivity supported by field data? Water Resources Research, 51(9), pp.7662-7679.&amp;#160; [https://doi.org/10.1002/2015WR017220 DOI: 10.1002/2015WR017220]&amp;amp;nbsp;&amp;amp;nbsp; Free access article from [https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1002/2015WR017220 American Geophysical Union]&amp;lt;/ref&amp;gt; presented moderate and high reliability measurements of longitudinal macrodispersivity versus distance. Typical values of the longitudinal macrodispersivity varied from 0.1 to 10 m, with much lower values for transverse and vertical dispersivities. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt;Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;3&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt;Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;4&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14202&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
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		<updated>2020-12-21T17:59:29Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 17:59, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l119&quot; &gt;Line 119:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 119:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure 2 shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values were in the range of 0.5 to 5 m.&amp;#160; Zech, et al. (2015) presented moderate and high reliability measurements of longitudinal macrodispersivity versus distance. Typical values of the longitudinal macrodispersivity varied from 0.1 to 10 m, with much lower values for transverse and vertical dispersivities. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure 2 shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values were in the range of 0.5 to 5 m.&amp;#160; Zech, et al. (2015)&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;ref&amp;gt;Zech, A., Attinger, S., Cvetkovic, V., Dagan, G., Dietrich, P., Fiori, A., Rubin, Y. and Teutsch, G., 2015. Is unique scaling of aquifer macrodispersivity supported by field data? Water Resources Research, 51(9), pp.7662-7679.&amp;#160; [https://doi.org/10.1002/2015WR017220 DOI: 10.1002/2015WR017220]&amp;amp;nbsp;&amp;amp;nbsp; Free access article from [https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1002/2015WR017220 American Geophysical Union]&amp;lt;/ref&amp;gt; &lt;/ins&gt;presented moderate and high reliability measurements of longitudinal macrodispersivity versus distance. Typical values of the longitudinal macrodispersivity varied from 0.1 to 10 m, with much lower values for transverse and vertical dispersivities. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14201&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14201&amp;oldid=prev"/>
		<updated>2020-12-21T17:43:22Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 17:43, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l119&quot; &gt;Line 119:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 119:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure 2 shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;are &lt;/del&gt;in the range of 0.5 to 5 m.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to better represent the observed large-scale spreading of plumes&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient, eventually approaching an asymptotic value&amp;lt;ref name=&amp;quot;Gelhar1979&amp;quot;&amp;gt;Gelhar, L.W., Gutjahr, A.L. and Naff, R.L., 1979. Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp.1387-1397.&amp;#160; [https://doi.org/10.1029/WR015i006p01387 DOI:10.1029/WR015i006p01387]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Gelhar1983&amp;quot;&amp;gt;Gelhar, L.W. and Axness, C.L., 1983. Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion for solute transport in anisotropic heterogeneous aquifers. Water Resources Research, 24(9), pp.1491-1500.&amp;#160; [https://doi.org/10.1029/WR024i009p01491 DOI:10.1029/WR024i009p01491]&amp;lt;/ref&amp;gt;.&amp;#160; Figure 2 shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;were &lt;/ins&gt;in the range of 0.5 to 5 m&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.&amp;#160; Zech, et al. (2015) presented moderate and high reliability measurements of longitudinal macrodispersivity versus distance. Typical values of the longitudinal macrodispersivity varied from 0.1 to 10 m, with much lower values for transverse and vertical dispersivities&lt;/ins&gt;. &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;===Matrix Diffusion===&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14200&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14200&amp;oldid=prev"/>
		<updated>2020-12-21T17:34:12Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 17:34, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l119&quot; &gt;Line 119:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 119:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;help match &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;apparent &lt;/del&gt;large-scale spreading of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;the plume&lt;/del&gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;However&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;there is limited theoretical support for using large mechanical dispersion coefficients&lt;/del&gt;&amp;lt;ref name=&amp;quot;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Payne2008&lt;/del&gt;&amp;quot;&amp;gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Payne&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;F&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;C&lt;/del&gt;., &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Quinnan&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;J&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;A&lt;/del&gt;. and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Potter&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;S&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;T&lt;/del&gt;., &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;2008&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Remediation hydraulics&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;CRC Press&lt;/del&gt;. [https://&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;www&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;crcpress&lt;/del&gt;.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;com&lt;/del&gt;/&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Remediation-Hydraulics/Payne-Quinnan-Potter&lt;/del&gt;/&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;9780849372490 ISBN:978-1-4200-0684-1&lt;/del&gt;]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Hadley2014&lt;/del&gt;&amp;quot;&amp;gt; &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Hadley&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;P&lt;/del&gt;.W. and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Newell&lt;/del&gt;, C., &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;2014&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The new potential &lt;/del&gt;for &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;understanding groundwater contaminant &lt;/del&gt;transport. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Groundwater&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;52&lt;/del&gt;(&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;2&lt;/del&gt;), pp.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;174&lt;/del&gt;-&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;186&lt;/del&gt;. [&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;http&lt;/del&gt;://&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;dx.&lt;/del&gt;doi.org/10.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;1111&lt;/del&gt;/&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;gwat.12135 doi&lt;/del&gt;:10.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;1111&lt;/del&gt;/&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;gwat.12135&lt;/del&gt;]&amp;lt;/ref&amp;gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;In transmissive zones, macrodispersion coefficients &lt;/del&gt;are &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;often orders &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;magnitude greater than molecular diffusion coefficients, leading some &lt;/del&gt;to &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;conclude that molecular diffusion can be ignored&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;better represent &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;observed &lt;/ins&gt;large-scale spreading of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;plumes&lt;/ins&gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot;/&amp;gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Theoretical studies suggest that macrodispersivity will increase with distance near the source, and then increase more slowly farther downgradient&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;eventually approaching an asymptotic value&lt;/ins&gt;&amp;lt;ref name=&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Gelhar1979&lt;/ins&gt;&amp;quot;&amp;gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Gelhar&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;L&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;W&lt;/ins&gt;., &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Gutjahr&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;A&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;L&lt;/ins&gt;. and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Naff&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;R&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;L&lt;/ins&gt;., &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1979&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Stochastic analysis of macrodispersion in a stratified aquifer. Water Resources Research, 15(6), pp&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1387-1397&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;[https://&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;doi&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;org/10&lt;/ins&gt;.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1029&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;WR015i006p01387 DOI:10.1029&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;WR015i006p01387&lt;/ins&gt;]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Gelhar1983&lt;/ins&gt;&amp;quot;&amp;gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Gelhar&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;L&lt;/ins&gt;.W. and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Axness&lt;/ins&gt;, C&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;.L&lt;/ins&gt;., &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1983&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Three‐dimensional stochastic analysis of macrodispersion in aquifers. Water Resources Research, 19(1), pp.161-180.&amp;#160; [https://doi.org/10.1029/WR019i001p00161 DOI:10.1029/WR019i001p00161]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;&amp;gt;Dagan, G., 1988. Time‐dependent macrodispersion &lt;/ins&gt;for &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;solute &lt;/ins&gt;transport &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;in anisotropic heterogeneous aquifers&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Water Resources Research&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;24&lt;/ins&gt;(&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;9&lt;/ins&gt;), pp.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1491&lt;/ins&gt;-&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1500&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;[&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;https&lt;/ins&gt;://doi.org/10.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1029&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;WR024i009p01491 DOI&lt;/ins&gt;:10.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;1029&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;WR024i009p01491&lt;/ins&gt;]&amp;lt;/ref&amp;gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; Figure 2 shows values of macrodispersivity calculated using the theory of Dagan&amp;lt;ref name=&amp;quot;Dagan1988&amp;quot;/&amp;gt; with an autocorrelation length of 3 m and several different values of the variance of &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; (σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;) where &amp;#039;&amp;#039;Y&amp;#039;&amp;#039; = Log &amp;#039;&amp;#039;K&amp;#039;&amp;#039;. The calculated macrodispersivity increases more rapidly and approaches higher asymptotic values for more heterogeneous aquifers with greater variations in &amp;#039;&amp;#039;K&amp;#039;&amp;#039; (larger σ&amp;lt;small&amp;gt;&amp;lt;sup&amp;gt;2&amp;lt;/sup&amp;gt;&amp;lt;sub&amp;gt;&amp;#039;&amp;#039;Y&amp;#039;&amp;#039;&amp;lt;/sub&amp;gt;&amp;lt;/small&amp;gt;).&amp;#160; The maximum predicted dispersivity values &lt;/ins&gt;are &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;in the range &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;0.5 &lt;/ins&gt;to &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;5 m&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Payne2008&lt;/del&gt;&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;ITRC2011&lt;/del&gt;&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;===Matrix Diffusion===&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;ITRC2011&lt;/ins&gt;&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Payne2008&lt;/ins&gt;&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https:&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;/www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&lt;/ins&gt;&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;&amp;gt;Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http:&lt;/ins&gt;/&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;/dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&lt;/ins&gt;&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14199&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
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		<updated>2020-12-21T17:13:20Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 17:13, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l117&quot; &gt;Line 117:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 117:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure 3. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure 3. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at the monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives the appearance of a plume with a very large dispersion coefficient. This spreading of the solute caused by large-scale heterogeneities in the aquifer and the associated spatial variations in advective transport velocity is referred to as macrodispersion.&amp;#160; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;In some groundwater modeling projects, large values of the dispersion coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14198&amp;oldid=prev</id>
		<title>Jhurley: /* Macrodispersion */</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=14198&amp;oldid=prev"/>
		<updated>2020-12-21T16:33:04Z</updated>

		<summary type="html">&lt;p&gt;‎&lt;span dir=&quot;auto&quot;&gt;&lt;span class=&quot;autocomment&quot;&gt;Macrodispersion&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 16:33, 21 December 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l117&quot; &gt;Line 117:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 117:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;==Macrodispersion==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure 3. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[File:NewThinkingAboutDispersion.mp4 |thumbnail|right|500px|Figure 3. Matrix diffusion processes and their effects on plume persistence and attenuation.]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Macrodispersion&amp;amp;nbsp;is&amp;amp;nbsp;&lt;/del&gt;the&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;amp;nbsp;name given to &lt;/del&gt;the plume spreading caused by large-scale aquifer &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;heterogeneities &lt;/del&gt;and associated spatial variations in advective transport velocity. In some groundwater modeling projects, large values of the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;macrodispersion &lt;/del&gt;coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Spatial variations in hydraulic conductivity can increase the apparent spreading of solute plumes observed in groundwater monitoring wells. For example, in an aquifer composed of alternating layers of lower hydraulic conductivity (&amp;#039;&amp;#039;K&amp;#039;&amp;#039;) silty sand and higher &amp;#039;&amp;#039;K&amp;#039;&amp;#039; sandy gravel layers, the dissolved solute rapidly migrates downgradient through the sandy gravel layers resulting in relatively high concentration fingers surrounded by relatively uncontaminated material. Over time, contaminants in lower &amp;#039;&amp;#039;K&amp;#039;&amp;#039; layers eventually breakthrough at &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;monitoring well, causing a more gradual further increase in measured concentrations.&amp;#160; This rapid breakthrough followed by gradual increases in solute concentrations gives &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;appearance of a &lt;/ins&gt;plume &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;with a very large dispersion coefficient. This &lt;/ins&gt;spreading &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;of the solute &lt;/ins&gt;caused by large-scale &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;heterogeneities in the &lt;/ins&gt;aquifer and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;the &lt;/ins&gt;associated spatial variations in advective transport velocity &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;is referred to as macrodispersion&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/ins&gt;In some groundwater modeling projects, large values of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;dispersion &lt;/ins&gt;coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Jhurley</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=13989&amp;oldid=prev</id>
		<title>Admin at 18:38, 24 September 2020</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=13989&amp;oldid=prev"/>
		<updated>2020-09-24T18:38:39Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
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				&lt;col class=&quot;diff-marker&quot; /&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 18:38, 24 September 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l7&quot; &gt;Line 7:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*[[Plume Response Modeling]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*[[Plume Response Modeling]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;CONTRIBUTOR(S):&amp;#039;&amp;#039;&amp;#039; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;CONTRIBUTOR(S):&amp;#039;&amp;#039;&amp;#039; [[Dr. Charles Newell, P.E.|Dr. Charles Newell]] and [[Dr. Robert Borden, P.E.|Dr. Robert Borden]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;*&lt;/del&gt;[[Dr. Charles Newell, P.E.|Dr. Charles Newell]] and [[Dr. Robert Borden, P.E.|Dr. Robert Borden]]&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Key Resource(s):&amp;#039;&amp;#039;&amp;#039;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Key Resource(s):&amp;#039;&amp;#039;&amp;#039;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
		
	</entry>
	<entry>
		<id>https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=13987&amp;oldid=prev</id>
		<title>Admin at 18:37, 24 September 2020</title>
		<link rel="alternate" type="text/html" href="https://www.enviro.wiki/index.php?title=Dispersion_and_Diffusion&amp;diff=13987&amp;oldid=prev"/>
		<updated>2020-09-24T18:37:12Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 18:37, 24 September 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l9&quot; &gt;Line 9:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 9:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;CONTRIBUTOR(S):&amp;#039;&amp;#039;&amp;#039; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;CONTRIBUTOR(S):&amp;#039;&amp;#039;&amp;#039; &amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*[[Dr. Charles Newell, P.E.|Dr. Charles Newell]]&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;*[[Dr. Charles Newell, P.E.|Dr. Charles Newell]] &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;and &lt;/ins&gt;[[Dr. Robert Borden, P.E.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;|Dr. Robert Borden&lt;/ins&gt;]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;*&lt;/del&gt;[[Dr. Robert Borden, P.E.]]&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;#160;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Key Resource(s):&amp;#039;&amp;#039;&amp;#039;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Key Resource(s):&amp;#039;&amp;#039;&amp;#039;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l122&quot; &gt;Line 122:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 121:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Macrodispersion&amp;amp;nbsp;is&amp;amp;nbsp;the&amp;amp;nbsp;name given to the plume spreading caused by large-scale aquifer heterogeneities and associated spatial variations in advective transport velocity. In some groundwater modeling projects, large values of the macrodispersion coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Macrodispersion&amp;amp;nbsp;is&amp;amp;nbsp;the&amp;amp;nbsp;name given to the plume spreading caused by large-scale aquifer heterogeneities and associated spatial variations in advective transport velocity. In some groundwater modeling projects, large values of the macrodispersion coefficient are used as an adjustment factor to help match the apparent large-scale spreading of the plume&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;. However, there is limited theoretical support for using large mechanical dispersion coefficients&amp;lt;ref name=&amp;quot;Payne2008&amp;quot;&amp;gt;Payne, F.C., Quinnan, J.A. and Potter, S.T., 2008. Remediation hydraulics. CRC Press. [https://www.crcpress.com/Remediation-Hydraulics/Payne-Quinnan-Potter/9780849372490 ISBN:978-1-4200-0684-1]&amp;lt;/ref&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot;&amp;gt; Hadley, P.W. and Newell, C., 2014. The new potential for understanding groundwater contaminant transport. Groundwater, 52(2), pp.174-186. [http://dx.doi.org/10.1111/gwat.12135 doi:10.1111/gwat.12135]&amp;lt;/ref&amp;gt;. In transmissive zones, macrodispersion coefficients are often orders of magnitude greater than molecular diffusion coefficients, leading some to conclude that molecular diffusion can be ignored.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 &lt;del class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/del&gt;video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Recently, an alternate conceptual model for describing large-scale plume spreading in heterogeneous soils has been proposed&amp;lt;ref name=&amp;quot;Payne2008&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;ITRC2011&amp;quot; /&amp;gt;&amp;lt;ref name=&amp;quot;Hadley2014&amp;quot; /&amp;gt;. In this approach, solute transport in the transmissive zones is reasonably well described by the advection-dispersion equation using relatively small dispersion coefficients representing mechanical dispersion. However, overtime, molecular diffusion slowly transports solutes into lower permeability zones (Figure 3). As the transmissive zones are remediated, these solutes slowly diffuse back out, causing a long extended tail to the flushout curve. This process, referred to as [[Matrix Diffusion |matrix diffusion]], is controlled by [[wikipedia: Molecular diffusion | molecular diffusion]] and the presence of geologic heterogeneity with sharp contrasts between transmissive and low permeability media&amp;lt;ref&amp;gt;Sale, T.C., Illangasekare, T., Zimbron, J., Rodriguez, D., Wilkins, B. and Marinelli, F., 2007. AFCEE source zone initiative. Report Prepared for the Air Force Center for Environmental Excellence by Colorado State University and Colorado School of Mines. [//www.enviro.wiki/images/0/08/AFCEE-2007-Sale.pdf Report pdf]&amp;lt;/ref&amp;gt; as discussed in the [//www.enviro.wiki/images/8/8a/NewThinkingAboutDispersion.mp4 video] shown in Figure 3.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;br clear=&amp;quot;left&amp;quot; /&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class=&#039;diff-marker&#039;&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Admin</name></author>
		
	</entry>
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