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	<title>FAQ:General:AveragingofConductivitiesatElementBoundaries - Versionsgeschichte</title>
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		<title>SebSta: hat „FAQ General:AveragingofConductivitiesatElementBoundaries“ nach „FAQ:General:AveragingofConductivitiesatElementBoundaries“ verschoben</title>
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		<updated>2013-06-13T12:34:52Z</updated>

		<summary type="html">&lt;p&gt;hat „&lt;a href=&quot;/mediawiki/index.php?title=FAQ_General:AveragingofConductivitiesatElementBoundaries&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;FAQ General:AveragingofConductivitiesatElementBoundaries (Seite nicht vorhanden)&quot;&gt;FAQ General:AveragingofConductivitiesatElementBoundaries&lt;/a&gt;“ nach „&lt;a href=&quot;/mediawiki/index.php?title=FAQ:General:AveragingofConductivitiesatElementBoundaries&quot; title=&quot;FAQ:General:AveragingofConductivitiesatElementBoundaries&quot;&gt;FAQ:General:AveragingofConductivitiesatElementBoundaries&lt;/a&gt;“ verschoben&lt;/p&gt;
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				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Nächstältere Version&lt;/td&gt;
				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Version vom 13. Juni 2013, 14:34 Uhr&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-notice&quot; lang=&quot;de&quot;&gt;&lt;div class=&quot;mw-diff-empty&quot;&gt;(kein Unterschied)&lt;/div&gt;
&lt;/td&gt;&lt;/tr&gt;&lt;/table&gt;</summary>
		<author><name>SebSta</name></author>
	</entry>
	<entry>
		<id>https://www.wufi-wiki.com/mediawiki/index.php?title=FAQ:General:AveragingofConductivitiesatElementBoundaries&amp;diff=796&amp;oldid=prev</id>
		<title>Len: Die Seite wurde neu angelegt: = (22): Averaging of Conductivities at Element Boundaries =  &lt;B&gt;For the numerical solution of the transport equations the component must be divided into a series of gri...</title>
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		<updated>2008-10-06T09:34:30Z</updated>

		<summary type="html">&lt;p&gt;Die Seite wurde neu angelegt: = (22): Averaging of Conductivities at Element Boundaries =  &amp;lt;B&amp;gt;For the numerical solution of the transport equations the component must be divided into a series of gri...&lt;/p&gt;
&lt;p&gt;&lt;b&gt;Neue Seite&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= (22): Averaging of Conductivities at Element Boundaries =&lt;br /&gt;
&lt;br /&gt;
&amp;lt;B&amp;gt;For the numerical solution of the transport equations the component must be divided&lt;br /&gt;
into a series of grid elements for whose midpoints the resulting temperatures and water&lt;br /&gt;
contents are computed at each time step, and across whose element boundaries the heat&lt;br /&gt;
and moisture fluxes required by the equations are flowing. In order to arrive at correct&lt;br /&gt;
fluxes across the boundaries, effective conductivities have to be assigned to the&lt;br /&gt;
boundaries which represent the integral effect of the conductivities between the&lt;br /&gt;
midpoints of the two elements. The investigations reported in [1] show that the results&lt;br /&gt;
do in fact depend on the way these effective heat and moisture conductivities are&lt;br /&gt;
determined from the real conductivities of the two elements: obviously linear&lt;br /&gt;
interpolation between the neighboring conductivities is preferable within a material&lt;br /&gt;
layer, and a resistance formulation is more appropriate for boundaries between layers&lt;br /&gt;
with different materials. How does WUFI treat these element boundary&lt;br /&gt;
conductivities?&amp;lt;/B&amp;gt;&amp;lt;BR&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;P&amp;gt;&lt;br /&gt;
It is obvious that at element boundaries where materials with possibly very different&lt;br /&gt;
conductivities are in contact with each other a simple average of the conductivities&lt;br /&gt;
(or resistances) cannot result in a realistic effective conductivity to describe the&lt;br /&gt;
fluxes between the elements. Take as an example a material with very low resistance&lt;br /&gt;
which borders on a material with very high resistance. The flux flowing between the&lt;br /&gt;
midpoints of the two elements is determined by the sum of the two successively&lt;br /&gt;
encountered resistances, not by the arithmetical average of the conductivities.&amp;lt;BR&amp;gt;&lt;br /&gt;
One might suppose now that this physically motivated reasoning also applies to&lt;br /&gt;
smaller differences between the neighboring elements and that therefore the resistance&lt;br /&gt;
formulation (i.e. the harmonic mean of the conductivities) should always be used&lt;br /&gt;
within the entire component. However, test calculations during the development&lt;br /&gt;
of WUFI&amp;#039;s numerics showed that this is not the case. Within a material the&lt;br /&gt;
arithmetical mean of the conductivities yielded better results (compared with&lt;br /&gt;
experimental data), so that WUFI uses harmonic averages at material boundaries and&lt;br /&gt;
arithmetical averages within a material, in agreement with the cited investigation.&lt;br /&gt;
The derivation of the resistance formulation assumes equal fluxes in the two element&lt;br /&gt;
halves, but this need not be the case if transient processes in materials with heat&lt;br /&gt;
or moisture storage capacities are considered.&lt;br /&gt;
&amp;lt;/P&amp;gt;&lt;br /&gt;
&amp;lt;P&amp;gt;&lt;br /&gt;
[1] Galbraith, G.H. et al.: Evaluation of Discretized Transport Properties for&lt;br /&gt;
Numerical Modelling of Heat and Moisture Transfer in Building Structures,&amp;lt;BR&amp;gt;&lt;br /&gt;
Journal of Thermal Env. &amp;amp; Bldg. Sci., Vol. 24, Jan. 2001 &lt;br /&gt;
&amp;lt;/P&amp;gt;&lt;/div&gt;</summary>
		<author><name>Len</name></author>
	</entry>
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