.TH "serif::discretization::blocks::enthalpy" 3 "Version v0.0.1a" "SERiF" \" -*- nroff -*-
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.SH NAME
serif::discretization::blocks::enthalpy \- The enthalpy field is a scalar field is a C0 continuous scalar field\&. Note that this field likely will not survive the transition to the more general non-barotropic case\&. In the barotropic case the gradient of enthalpy is parallel to the gradient of the pressure\&. This make enthalpy a particularly useful quantity as we can represent the 0 pressure surface condition as the 0 enthalpy condition and we can break down mass constraint into a game of optimizing the Bernoulli constant\&.  

.SH SYNOPSIS
.br
.PP
.PP
\fR#include <fields\&.hpp>\fP
.PP
Inherits \fBserif::discretization::blocks::field\fP\&.
.SS "Classes"

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.ti -1c
.RI "struct \fBspecific\fP"
.br
.RI "the specific enthalpy is the term we specifically work with rather than the total enthalpy of dof\&. In fact heuristically I would say that generally we should always work in specific quantities rather than total quantities as there is not a well defined amount of material at some dof\&. "
.in -1c
.SS "Public Types"

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.ti -1c
.RI "using \fBTerms\fP = \fButils::types::TypeList\fP<\fBspecific\fP>"
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.RI "Type list of terms for compile time reflection and iteration over the terms of the field\&. "
.in -1c
.SS "Static Public Attributes"

.in +1c
.ti -1c
.RI "static constexpr std::string_view \fBname\fP = \fBmeta::type_name\fP<\fBenthalpy\fP>()"
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.RI "Compile time reflected name of the field\&. "
.ti -1c
.RI "static constexpr \fBspecific\fP \fBspecific_term\fP {}"
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.RI "Static constexpr instance of the specific term\&. This is used to access the term in the discretization\&. "
.in -1c
.SH "Detailed Description"
.PP 
The enthalpy field is a scalar field is a C0 continuous scalar field\&. Note that this field likely will not survive the transition to the more general non-barotropic case\&. In the barotropic case the gradient of enthalpy is parallel to the gradient of the pressure\&. This make enthalpy a particularly useful quantity as we can represent the 0 pressure surface condition as the 0 enthalpy condition and we can break down mass constraint into a game of optimizing the Bernoulli constant\&. 
.SH "Member Typedef Documentation"
.PP 
.SS "using \fBserif::discretization::blocks::enthalpy::Terms\fP = \fButils::types::TypeList\fP<\fBspecific\fP>"

.PP
Type list of terms for compile time reflection and iteration over the terms of the field\&. 
.SH "Member Data Documentation"
.PP 
.SS "std::string_view serif::discretization::blocks::enthalpy::name = \fBmeta::type_name\fP<\fBenthalpy\fP>()\fR [static]\fP, \fR [constexpr]\fP"

.PP
Compile time reflected name of the field\&. 
.SS "\fBspecific\fP serif::discretization::blocks::enthalpy::specific_term {}\fR [static]\fP, \fR [constexpr]\fP"

.PP
Static constexpr instance of the specific term\&. This is used to access the term in the discretization\&. 

.SH "Author"
.PP 
Generated automatically by Doxygen for SERiF from the source code\&.