[cig-commits] commit 1992 by bangerth to /var/svn/dealii/aspect

[dealii.demon at gmail.com]

Revision 1992

Remove the cantera sections from the input files (unused anyway) so that we can run them on systems without cantera installed.

U   trunk/aspire/tests/simple_1.prm
U   trunk/aspire/tests/simple_2.prm
U   trunk/aspire/tests/simple_3.prm


http://www.dealii.org/websvn/revision.php?repname=Aspect+Repository&path=%2F&rev=1992&peg=1992

Diff:
Modified: trunk/aspire/tests/simple_1.prm
===================================================================
--- trunk/aspire/tests/simple_1.prm	2013-10-25 12:48:13 UTC (rev 1991)
+++ trunk/aspire/tests/simple_1.prm	2013-10-25 12:58:25 UTC (rev 1992)
@@ -8,14 +8,14 @@
 # not located in one of the directories listed in the LD_LIBRARY_PATH
 # environment variable. In order to load a library in the current directory,
 # use <./myplugin.so> instead.
-# 
+#
 # The typical use of this parameter is to so that you can implement additional
 # plugins in your own directories, rather than in the ASPECT source
 # directories. You can then simply compile these plugins into a shared library
 # without having to re-compile all of ASPECT. See the section of the manual
 # discussing writing extensions for more information on how to compile
 # additional files into a shared library.
-set Additional shared libraries         = 
+set Additional shared libraries         =
 
 # In computations, the time step $k$ is chosen according to $k = c \min_K
 # rac{h_K}{\|u\|_{\infty,K} p_T}$ where $h_K$ is the diameter of cell $K$,
@@ -49,7 +49,7 @@
 # equals the norm of the right hand side. A given tolerance of 0 would mean
 # that the linear system has to be solved exactly, since this is the only way
 # to obtain a zero residual.
-# 
+#
 # In practice, you should choose the value of this parameter to be so that if
 # you make it smaller the results of your simulation do not change any more
 # (qualitatively) whereas if you make it larger, they do. For most cases, the
@@ -125,12 +125,12 @@
     # that describes the function, rather than having to use its numeric value
     # everywhere the constant appears. These values can be defined using this
     # parameter, in the form `var1=value1, var2=value2, ...'.
-    # 
+    #
     # A typical example would be to set this runtime parameter to
     # `pi=3.1415926536' and then use `pi' in the expression of the actual
     # formula. (That said, for convenience this class actually defines both
     # `pi' and `Pi' by default, but you get the idea.)
-    set Function constants  = 
+    set Function constants  =
 
     # The formula that denotes the function you want to evaluate for
     # particular values of the independent variables. This expression may
@@ -141,7 +141,7 @@
     # true, and to the third argument otherwise. For a full overview of
     # possible expressions accepted see the documentation of the fparser
     # library.
-    # 
+    #
     # If the function you are describing represents a vector-valued function
     # with multiple components, then separate the expressions for individual
     # components by a semicolon.
@@ -166,16 +166,16 @@
 
 subsection Boundary temperature model
   # Select one of the following models:
-  # 
+  #
   # `constant': Implementation of a model in which the boundary temperature
   # values are constant throughout the whole boundary.
-  # 
+  #
   # `box': A model in which the temperature is chosen constant on all the
   # sides of a box.
-  # 
+  #
   # `function': Implementation of a model in which the boundary temperature
   # values are given by a function.
-  set Model name = constant # default: 
+  set Model name = constant # default:
 
 
   subsection Box
@@ -202,12 +202,12 @@
     # that describes the function, rather than having to use its numeric value
     # everywhere the constant appears. These values can be defined using this
     # parameter, in the form `var1=value1, var2=value2, ...'.
-    # 
+    #
     # A typical example would be to set this runtime parameter to
     # `pi=3.1415926536' and then use `pi' in the expression of the actual
     # formula. (That said, for convenience this class actually defines both
     # `pi' and `Pi' by default, but you get the idea.)
-    set Function constants  = 
+    set Function constants  =
 
     # The formula that denotes the function you want to evaluate for
     # particular values of the independent variables. This expression may
@@ -218,7 +218,7 @@
     # true, and to the third argument otherwise. For a full overview of
     # possible expressions accepted see the documentation of the fparser
     # library.
-    # 
+    #
     # If the function you are describing represents a vector-valued function
     # with multiple components, then separate the expressions for individual
     # components by a semicolon.
@@ -258,12 +258,12 @@
     # that describes the function, rather than having to use its numeric value
     # everywhere the constant appears. These values can be defined using this
     # parameter, in the form `var1=value1, var2=value2, ...'.
-    # 
+    #
     # A typical example would be to set this runtime parameter to
     # `pi=3.1415926536' and then use `pi' in the expression of the actual
     # formula. (That said, for convenience this class actually defines both
     # `pi' and `Pi' by default, but you get the idea.)
-    set Function constants  = 
+    set Function constants  =
 
     # The formula that denotes the function you want to evaluate for
     # particular values of the independent variables. This expression may
@@ -274,7 +274,7 @@
     # true, and to the third argument otherwise. For a full overview of
     # possible expressions accepted see the documentation of the fparser
     # library.
-    # 
+    #
     # If the function you are describing represents a vector-valued function
     # with multiple components, then separate the expressions for individual
     # components by a semicolon.
@@ -316,7 +316,7 @@
   # First, the sum of the fields to be normalized is calculated at every point
   # and the global maximum is determined. Second, the compositional fields to
   # be normalized are divided by this maximum.
-  set List of normalized fields = 
+  set List of normalized fields =
 
   # The number of fields that will be advected along with the flow field,
   # excluding velocity, pressure and temperature.
@@ -326,7 +326,7 @@
 
 subsection Compositional initial conditions
   # Select one of the following models:
-  # 
+  #
   # `function': Composition is given in terms of an explicit formula
   set Model name = function
 
@@ -336,12 +336,12 @@
     # that describes the function, rather than having to use its numeric value
     # everywhere the constant appears. These values can be defined using this
     # parameter, in the form `var1=value1, var2=value2, ...'.
-    # 
+    #
     # A typical example would be to set this runtime parameter to
     # `pi=3.1415926536' and then use `pi' in the expression of the actual
     # formula. (That said, for convenience this class actually defines both
     # `pi' and `Pi' by default, but you get the idea.)
-    set Function constants  = 
+    set Function constants  =
 
     # The formula that denotes the function you want to evaluate for
     # particular values of the independent variables. This expression may
@@ -352,7 +352,7 @@
     # true, and to the third argument otherwise. For a full overview of
     # possible expressions accepted see the documentation of the fparser
     # library.
-    # 
+    #
     # If the function you are describing represents a vector-valued function
     # with multiple components, then separate the expressions for individual
     # components by a semicolon.
@@ -396,7 +396,7 @@
   # expense of a larger number of degrees of freedom (true), or to go with a
   # cheaper discretization that does not locally conserve mass, although it is
   # globally conservative (false).
-  # 
+  #
   # When using a locally conservative discretization, the finite element space
   # for the pressure is discontinuous between cells and is the polynomial
   # space $P_{-q}$ of polynomials of degree $q$ in each variable separately.
@@ -408,12 +408,12 @@
   # i.e., for each cell inflow and outflow exactly balance each other as one
   # would expect for an incompressible medium. In other words, the velocity
   # field is locally conservative.
-  # 
+  #
   # On the other hand, if this parameter is set to ``false'', then the finite
   # element space is chosen as $Q_q$. This choice does not yield the local
   # conservation property but has the advantage of requiring fewer degrees of
   # freedom. Furthermore, the error is generally smaller with this choice.
-  # 
+  #
   # For an in-depth discussion of these issues and a quantitative evaluation
   # of the different choices, see