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	<updated>2026-08-12T22:58:54Z</updated>
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		<id>https://en.formulasearchengine.com/w/index.php?title=Jacobi_form&amp;diff=24570</id>
		<title>Jacobi form</title>
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		<updated>2013-08-11T17:30:36Z</updated>

		<summary type="html">&lt;p&gt;165.124.167.212: /* Definition */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;effective diffusion coefficient&#039;&#039;&#039; (also referred to as the apparent diffusion coefficient) of a diffusant 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 0.8T&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&#039;s equation when only grain boundary and lattice diffusion are dominant:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; {D^{\mathrm{eff}}} = f&amp;lt;/math&amp;gt; D&amp;lt;sub&amp;gt;gb&amp;lt;/sub&amp;gt; &amp;lt;math&amp;gt; + (1-f) &amp;lt;/math&amp;gt;D&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
where&lt;br /&gt;
:&amp;lt;math&amp;gt; {D^{\mathrm{eff}}} = &amp;lt;/math&amp;gt; effective diffusion coefficient.&lt;br /&gt;
:D&amp;lt;sub&amp;gt;gb&amp;lt;/sub&amp;gt; = grain boundary diffusion coefficient.&lt;br /&gt;
:D&amp;lt;sub&amp;gt;l&amp;lt;/sub&amp;gt; = lattice diffusion coefficient.&lt;br /&gt;
:&amp;lt;math&amp;gt; f = \tfrac{q}{d} &amp;lt;/math&amp;gt;.δ&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;
:δ &amp;lt;math&amp;gt; = &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;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
{{refbegin}}&lt;br /&gt;
{{refend}}&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Kirkendall effect]]&lt;br /&gt;
* [[Phase transformations in solids]]&lt;br /&gt;
* [[Mass diffusivity]]&lt;br /&gt;
&lt;br /&gt;
[[Category:Diffusion]]&lt;/div&gt;</summary>
		<author><name>165.124.167.212</name></author>
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