Remove some unnecessary files
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Ray Speth
parent
258fb8ed57
commit
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5 changed files with 0 additions and 1717 deletions
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#!/bin/sh
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#
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#
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/bin/rm -rf build/test
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#
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#
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scons test-clean
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#
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#
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#!/bin/sh
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#
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#
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CUR=`pwd`
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CANTERA_SRC_ROOT=${CANTERA_SRC_ROOT:="$CUR"}
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/bin/rm -rf build/docs/doxygen
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cd $CANTERA_SRC_ROOT
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#doxygen doc/doxygen/Doxyfile
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doxygen doc/doxygen/Doxyfile.tested
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#!/bin/sh
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#
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#
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location='build'
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CUR=`pwd`
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# echo $CUR
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CANTERA_SRC_ROOT=${CANTERA_SRC_ROOT:="$CUR"}
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echo hhh = $CANTERA_SRC_ROOT
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CANTERA_INSTALL_DIR=${CANTERA_INSTALL_ROOT:="$CUR"}
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if test $# -gt 0
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then
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locat=$1
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echo locat = $locat
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if [ $locat == 'install' ]
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then
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location='install'
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fi
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if [ $locat == 'build' ]
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then
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location='build'
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fi
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fi
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startpg=$CANTERA_SRC_ROOT/build/docs/doxygen/html/index.html
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if [ $location == 'build' ]
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then
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startpg=$CANTERA_SRC_ROOT/build/docs/doxygen/html/index.html
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elif [ $location == 'install' ]
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then
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startpg=$CANTERA_INSTALL_DIR/share/cantera/doc/doxygen/html/index.html
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fi
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#
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#
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firefox $startpg &
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exit 0;
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File diff suppressed because it is too large
Load diff
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@ -1,95 +0,0 @@
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/**
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\page thermopage Thermodynamic Properties
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%Cantera can be used to compute thermodynamic properties of pure
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substances, solutions, and mixtures of various types, including ones
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containing multiple phases. The first step is to create an object that
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represents each phase.
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A simple complete program that creates an object representing a gas mixture and prints its temperature is shown below.
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\include ex1.cpp
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Class \link Cantera::ThermoPhase ThermoPhase \endlink
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is the base class for %Cantera classes that represent
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phases of matter. It defines the public interface for all classes that
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represent phases. For example, it specifies that they all have a
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method \c temperature() that returns the current temperature, a method
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\c setTemperature(double T) that sets the temperature, a method \c
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getChemPotentials(double* mu) that writes the species chemical
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potentials into array \c mu, and so on.
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Class ThermoPhase can be used to represent the intensive state of any
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single-phase solution of multiple species. The phase may be a bulk,
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three-dimensional phase (a gas, a liquid, or a solid), or may be a
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two-dimensional surface phase, or even a one-dimensional "edge"
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phase. The specific attributes of each type of phase are specified by
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deriving a class from ThemoPhase and providing implementations for the
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virtual methods of ThermoPhase.
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\section The Intensive Thermodynamic State
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Class ThermoPhase and classes derived from it work only with the
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intensive thermodynamic state. That is, all extensive properties
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(enthalpy, entropy, internal energy, volume, etc.) are computed for a
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unit quantity (on a mass or mole basis). For example, there is a
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method enthalpy_mole() that returns the molar enthalpy (J/kmol), and a
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method enthalpy_mass() that returns the specific enthalpy (J/kg), but
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no method enthalpy() that would return the total enthalpy (J). This is
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because class ThermoPhase does not store the total amount (mass or
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mole) of the phase.
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From thermodynamics, it may be shown that the intensive state of a
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single-component phase in equilibrium is fully specified by the values
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of any r+1 independent thermodynamic properties, where r is the number
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of reversible work modes. If the only reversible work mode is
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compression (a "simple compressible substance"), then two properties
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suffice to specify the intensive state.
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In principle, any two independent p
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specified, the values of all other intensive properties may be
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computed. For example, specifying the pressure and molar entropy
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consisting of a solution of K species
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in equilibrium is fully specified by the values of any two independent
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thermodynamic properties, in addition to in
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Class ThermoPhase stores internally the values of the temperature, the
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mass density, and the mass fractions of all species. These values are
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sufficient to fix the intensive thermodynamic state of the phase. All
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properties for a unit amount (on a mass or mole basis) are determined
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once the intensive state is specified. For the extensive properties, class ThermoPhase provides methods that return property values on a molar basis (e.g. enthalpy_mole(), with units J/kmol) or on a mass basis (e.g. enthalpy_mass(), with units J/kg). Since the total mass or total number of moles is not stored,
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Note that the total mass or number of moles is not stored
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Given these values, any other intensive thermodynamic property may
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Note that the total mass or total number of moles is not stored -- therefore the values of all extensive properties (mass, volume, energy) are
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This choice is arbitrary, and for most purposes you can't tell which properties are stored and which are computed.
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The classes that derive from ThermoPhase compute o
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For example, suppose we want to create a class to use to compute the properties of ideal gas mixtures.
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Many of the methods of ThermoPhase are declared virtual, and are meant to be
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overloaded in classes derived from ThermoPhase. For example, class \link Cantera::IdealGasPhase IdealGasPhase \endlink
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derives from ThermoPhase, and represents ideal gas mixtures.
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Although class ThermoPhase defines the interface for all classes
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representing phases, it only provides implementations for a few of the
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methods. This is because ThermoPhase does not actually know the
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equation of state of any phase -- this information is provided by
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classes that derive from ThermoPhase.
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The methods implemented by ThermoPhase are ones that apply to all phases, independent of
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the equation of state. For example, it implements methods temperature() and setTemperature(),
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since the temperature value is stored internally. Also, the mass density is stored internally, so
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There is a list of classes which inherit from the ThermoPhase class (see \ref
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thermoprops "Thermodynamic Properties")
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There is a list of classes which handle standard states for species (see
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\ref spthermo "Species Standard-State Thermodynamic Properties").
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*/
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