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		<title>en&gt;Citation bot: [442]Add: title, year, last1, first1, last2, first2, last3, first3, last4, first4, last5, first5, last6, first6, journal, pages. Tweak: last2, last3, last4, last5, last6.  User-activated.</title>
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		<updated>2013-10-23T18:54:22Z</updated>

		<summary type="html">&lt;p&gt;[442]Add: title, year, last1, first1, last2, first2, last3, first3, last4, first4, last5, first5, last6, first6, journal, pages. Tweak: last2, last3, last4, last5, last6.  &lt;a href=&quot;/w/index.php?title=WP:UCB&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;WP:UCB (page does not exist)&quot;&gt;User-activated&lt;/a&gt;.&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Wagner model&amp;#039;&amp;#039;&amp;#039; is a [[rheology|rheological]] model developed for the prediction of the [[Viscoelasticity|viscoelastic]] properties of polymers. It might be considered as a simplified practical form of the [[Bernstein-Kearsley-Zapas]] model. The model was developed by German rheologist [[Manfred Wagner]].&lt;br /&gt;
&lt;br /&gt;
For the [[Isothermal process|isothermal]] conditions the model can be written as:&lt;br /&gt;
:&amp;lt;math&amp;gt;\mathbf{\sigma}(t) = -p \mathbf{I} + \int_{-\infty}^{t} M(t-t&amp;#039;)h(I_1,I_2)\mathbf{B}(t&amp;#039;)\, dt&amp;#039;&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
*&amp;lt;math&amp;gt;\mathbf{\sigma}(t)&amp;lt;/math&amp;gt; is the [[Cauchy stress tensor]] as function of time &amp;#039;&amp;#039;t&amp;#039;&amp;#039;,&lt;br /&gt;
*&amp;#039;&amp;#039;p&amp;#039;&amp;#039; is the pressure&lt;br /&gt;
*&amp;lt;math&amp;gt;\mathbf{I}&amp;lt;/math&amp;gt; is the unity tensor&lt;br /&gt;
*&amp;#039;&amp;#039;M&amp;#039;&amp;#039; is the memory function showing, usually expressed as a sum of exponential terms for each mode of [[Relaxation (physics)|relaxation]]:&lt;br /&gt;
:&amp;lt;math&amp;gt;M(x)=\sum_{k=1}^m \frac{g_i}{\theta_i}\exp(\frac{-x}{\theta_i})&amp;lt;/math&amp;gt;, where for each mode of the relaxation, &amp;lt;math&amp;gt;g_i&amp;lt;/math&amp;gt; is the relaxation modulus and &amp;lt;math&amp;gt;\theta_i&amp;lt;/math&amp;gt; is the relaxation time;&lt;br /&gt;
*&amp;lt;math&amp;gt;h(I_1,I_2)&amp;lt;/math&amp;gt; is the &amp;#039;&amp;#039;strain damping&amp;#039;&amp;#039; function that depends upon the first and second [[Invariants of tensors|invariants]] of [[Finite deformation tensors#Finger tensor|Finger tensor]] &amp;lt;math&amp;gt;\mathbf{B}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;strain damping function&amp;#039;&amp;#039; is usually written as:&lt;br /&gt;
:&amp;lt;math&amp;gt;h(I_1,I_2)=m^*exp(-n_1 \sqrt{I_1-3})+(1-m^*)exp(-n_2 \sqrt{I_2-3})&amp;lt;/math&amp;gt;,&lt;br /&gt;
The strain hardening function equal to one, then the deformation is small and approaching zero, then the deformations are large.&lt;br /&gt;
&lt;br /&gt;
The Wagner equation can be used in the non-isothermal cases by applying [[time-temperature shift factor]].&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
*M.H. Wagner &amp;#039;&amp;#039;Rheologica Acta&amp;#039;&amp;#039;, v.15, 136 (1976)&lt;br /&gt;
*M.H. Wagner &amp;#039;&amp;#039;Rheologica Acta&amp;#039;&amp;#039;, v.16, 43, (1977)&lt;br /&gt;
*B. Fan, D. Kazmer, W. Bushko, &amp;#039;&amp;#039;Polymer Engineering and Science&amp;#039;&amp;#039;, v44, N4 (2004)&lt;br /&gt;
&lt;br /&gt;
[[Category:Non-Newtonian fluids]]&lt;/div&gt;</summary>
		<author><name>en&gt;Citation bot</name></author>
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