[cig-commits] commit 2055 by bangerth to /var/svn/dealii/aspect
dealii.demon at gmail.com
dealii.demon at gmail.com
Tue Nov 26 05:24:23 PST 2013
Revision 2055
Provide alternative descriptions of the thermal expansion coefficient
and the compressibility.
U trunk/aspect/include/aspect/material_model/interface.h
http://www.dealii.org/websvn/revision.php?repname=Aspect+Repository&path=%2F&rev=2055&peg=2055
Diff:
Modified: trunk/aspect/include/aspect/material_model/interface.h
===================================================================
--- trunk/aspect/include/aspect/material_model/interface.h 2013-11-25 17:55:08 UTC (rev 2054)
+++ trunk/aspect/include/aspect/material_model/interface.h 2013-11-26 13:23:40 UTC (rev 2055)
@@ -333,7 +333,7 @@
const NonlinearDependence::Dependence dependence) const;
/**
- * Return the partial derivative of the compressibility function on the
+ * Return the partial derivative of the compressibility function on the
* variable indicates as last argument.
*
* The default implementation of this function returns zero
@@ -657,6 +657,10 @@
* Return the compressibility coefficient
* $rac 1
ho rac{\partial
ho}{\partial p}$ of the model as a
* function of temperature, pressure and position.
+ *
+ * The compressibility can equivalently be computed as
+ * $-rac 1V rac{\partial V}{\partial p}$. Note the difference
+ * in sign.
*/
virtual double compressibility (const double temperature,
const double pressure,
@@ -679,6 +683,10 @@
* $lpha=-rac{1}{
ho} rac{d
ho}{dT}$. Since the density
* <i>decreases</i> with temperature for almost all models,
* $lpha$ is usually positive.
+ *
+ * The thermal expansion coefficient can equivalently be computed as
+ * $rac 1V rac{\partial V}{\partial T}$. Note the difference
+ * in sign.
*
* This function has a default implementation that computes $lpha$
* through its definition above, using the density() and density_derivative()
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