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	<title>Effective diffusion coefficient - Revision history</title>
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	<updated>2026-10-26T14:45:18Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>http://debianws.lexgopc.com/wiki143/index.php?title=Effective_diffusion_coefficient&amp;diff=8704819&amp;oldid=prev</id>
		<title>imported&gt;Chongkian: no need these</title>
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		<updated>2023-10-19T05:27:22Z</updated>

		<summary type="html">&lt;p&gt;no need these&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Diffusion coefficient through the pore space of a porous media}}{{Context|date=September 2022}}&lt;br /&gt;
{{Refimprove|date=September 2022}}&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;effective diffusion coefficient&amp;#039;&amp;#039;&amp;#039; of a {{What|text=diffusant|date=September 2022}} in [[atomic diffusion]] of solid [[polycrystalline]] materials like [[metal alloy]]s is often represented as a [[weighted average]] of the [[grain boundary diffusion coefficient]] and the [[lattice diffusion coefficient]].&amp;lt;ref name=Heitjans&amp;gt;P. Heitjans, J. Karger, Ed, “Diffusion in condensed matter: Methods, Materials, Models,” 2nd edition, Birkhauser, 2005, pp. 1-965.&amp;lt;/ref&amp;gt;  Diffusion along both the grain boundary and in the lattice may be modeled with an [[Arrhenius equation]]. The ratio of the grain boundary diffusion activation energy over the lattice diffusion activation energy is usually 0.4–0.6, so as temperature is lowered, the grain boundary diffusion component increases.&amp;lt;ref name=Heitjans /&amp;gt;  Increasing temperature often allows for increased grain size, and the lattice diffusion component increases with increasing temperature, so often at 0.8&amp;amp;nbsp;T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; (of an alloy), the grain boundary component can be neglected.&lt;br /&gt;
&lt;br /&gt;
==Modeling==&lt;br /&gt;
The effective diffusion coefficient can be modeled using Hart&amp;#039;s equation when lattice diffusion is dominant (type A kinetics):&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; D_\text{eff} = f D_\text{gb} + (1-f) D_\ell &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;lt;math&amp;gt;D_\text{eff} = {}&amp;lt;/math&amp;gt;effective diffusion coefficient&lt;br /&gt;
:&amp;lt;math&amp;gt;D_\text{gb} = {}&amp;lt;/math&amp;gt;grain boundary diffusion coefficient&lt;br /&gt;
:&amp;lt;math&amp;gt;D_\ell = {}&amp;lt;/math&amp;gt;lattice diffusion coefficient&lt;br /&gt;
:&amp;lt;math&amp;gt;f = \frac{q \delta}{d}&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; q = {}&amp;lt;/math&amp;gt;value based on grain shape, 1 for parallel grains, 3 for square grains&lt;br /&gt;
:&amp;lt;math&amp;gt; d = {}&amp;lt;/math&amp;gt;average grain size&lt;br /&gt;
:&amp;lt;math&amp;gt;\delta = {}&amp;lt;/math&amp;gt;grain boundary width, often assumed to be 0.5 nm&lt;br /&gt;
&lt;br /&gt;
Grain boundary diffusion is significant in [[face-centered cubic]] metals below about 0.8 T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; (Absolute). Line dislocations and other [[Crystallographic defect|crystalline defects]] can become significant below ~0.4 T&amp;lt;sub&amp;gt;melt&amp;lt;/sub&amp;gt; in FCC metals.&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Kirkendall effect]]&lt;br /&gt;
* [[Mass diffusivity]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Diffusion]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{Metallurgy-stub}}&lt;br /&gt;
{{Materials-stub}}&lt;/div&gt;</summary>
		<author><name>imported&gt;Chongkian</name></author>
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