form(2rheolef)
πΈ form(2rheolef) πΈ
okay bestie, sit down, hydrate, because we're about to talk about the form class from rheolef-7.2 and it's honestly giving main character energy π
β¨ NAME β¨
form β finite element bilinear form (rheolef-7.2) π¦
π DESCRIPTION π
so. the form class is literally a glow-up container that groups four sparse matrices together, all associated to a bilinear form defined on two finite element spaces:
a: Uh*Vh ----> IR
(uh,vh) +---> a(uh,vh)
and the A operator that's associated to the bilinear form is defined like this:
A: Uh ----> Vh
uh +---> A*uh
where uh is a field(2), and vh=A*uh in Vh is such that a(uh,vh)=dual(A*uh,vh) for all vh in Vh β and dual(.,.) is the duality product between Vh and its dual, no cap. and since Vh is a finite dimensional space, its dual is identified to Vh itself and the duality product is the euclidean product in IR^dim(Vh). also the linear operator can be represented by a matrix. periodt β¨
and like, in practice? bilinear forms are created by using the integrate(3) function. that's the move π«Ά
π ALGEBRA π
forms, as matrix, support standard algebra β slay. adding or subtracting two forms writes a+b and a-b respectively, while multiplying by a scalar lambda writes lambda*a and multiplying two forms writes a*b. also, multiplying a form by a field uh writes a*uh. π
the form inversion is not as direct as e.g. as inv(a), since forms are very large matrix in practice: form inversion can be obtained via the solver(4) class. a notable exception is the case of block-diagonal forms at the element level: in that case, a direct inversion is possible during the assembly process, see integrate_option(3). iykyk π§
π REPRESENTATION π
the degrees of freedom (see space(2)) are splited between unknowns and blocked, i.e. uh=[uh.u,uh.b] for any field uh in Uh. conversely, vh=[vh.u,vh.b] for any field vh in Vh. so then the form-field vh=a*uh operation is formally equivalent to the following matrix-vector block operations:
[ vh.u ] [ a.uu a.ub ] [ uh.u ]
[ ] = [ ] [ ]
[ vh.b ] [ a.bu a.bb ] [ uh.n ]
or, after expansion:
vh.u = a.uu*uh.u + a.ub*vh.b
vh.b = a.bu*uh.b + a.bb*vh.b
i.e. the A matrix also admits a 2x2 block structure. so the form class is represented by four sparse matrix and the csr(4) compressed format is used. note that the previous formal relations for vh=a*uh writes equivalently within the Rheolef library as:
vh.set_u() = a.uu()*uh.u() + a.ub()*uh.b();
vh.set_b() = a.bu()*uh.u() + a.bb()*uh.b();
literally iconic β¨
π IMPLEMENTATION π
this documentation has been generated from file main/lib/form.h π
the form class is simply an alias to the form_basic class:
typedef form_basic<Float,rheo_default_memory_model> form;
the form_basic class provides an interface to four sparse matrix:
template<class T, class M>
class form_basic {
public :
// typedefs:
typedef typename csr<T,M>::size_type size_type;
typedef T value_type;
typedef typename scalar_traits<T>::type float_type;
typedef geo_basic<float_type,M> geo_type;
typedef space_basic<float_type,M> space_type;
// allocator/deallocator:
form_basic ();
form_basic (const form_basic<T,M>&);
form_basic<T,M>& operator= (const form_basic<T,M>&);
template<class Expr, class Sfinae = typename std::enable_if<details::is_form_lazy<Expr>::value, Expr>::type>
form_basic (const Expr&);
template<class Expr, class Sfinae = typename std::enable_if<details::is_form_lazy<Expr>::value, Expr>::type>
form_basic<T,M>& operator= (const Expr&);
// allocators from initializer list (c++ 2011):
form_basic (const std::initializer_list<details::form_concat_value<T,M> >& init_list);
form_basic (const std::initializer_list<details::form_concat_line <T,M> >& init_list);
// accessors:
const space_type& get_first_space() const;
const space_type& get_second_space() const;
const geo_type& get_geo() const;
bool is_symmetric() const;
void set_symmetry (bool is_symm = true) const;
bool is_definite_positive() const;
void set_definite_positive (bool is_dp = true) const;
bool is_symmetric_definite_positive() const;
void set_symmetric_definite_positive() const;
const communicator& comm() const;
// linear algebra:
form_basic<T,M> operator+ (const form_basic<T,M>& b) const;
form_basic<T,M> operator- (const form_basic<T,M>& b) const;
form_basic<T,M> operator* (const form_basic<T,M>& b) const;
form_basic<T,M>& operator*= (const T& lambda);
field_basic<T,M> operator* (const field_basic<T,M>& xh) const;
field_basic<T,M> trans_mult (const field_basic<T,M>& yh) const;
float_type operator () (const field_basic<T,M>& uh, const field_basic<T,M>& vh) const;
// io:
odiststream& put (odiststream& ops, bool show_partition = true) const;
void dump (std::string name) const;
// accessors & modifiers to unknown & blocked parts:
const csr<T,M>& uu() const { return _uu; }
const csr<T,M>& ub() const { return _ub; }
const csr<T,M>& bu() const { return _bu; }
const csr<T,M>& bb() const { return _bb; }
csr<T,M>& set_uu() { return _uu; }
csr<T,M>& set_ub() { return _ub; }
csr<T,M>& set_bu() { return _bu; }
csr<T,M>& set_bb() { return _bb; }
};
template<class T, class M> form_basic<T,M> trans (const form_basic<T,M>& a);
template<class T, class M> field_basic<T,M> diag (const form_basic<T,M>& a);
template<class T, class M> form_basic<T,M> diag (const field_basic<T,M>& dh);
π AUTHOR π
Pierre Saramito <Pierre.Saramito@imag.fr> π«Ά
πΈ COPYRIGHT πΈ
Copyright (C) 2000-2018 Pierre Saramito <Pierre.Saramito@imag.fr> GPLv3+: GNU GPL version 3 or later <http://gnu.org/licenses/gpl.html>. This is free software: you are free to change and redistribute it. There is NO WARRANTY, to the extent permitted by law.
bestie the NO WARRANTY is not a vibe, it's a legal fact β read it, love it, respect it π
okay that's the whole page, no notes π
this was rheolef Version 7.2, source page form(2rheolef), and you're welcome, go assemble something gorgeous πβ¨
π¦ where this page comes from
- debian trixie: librheolef-dev 7.2-4 Β· GPL-3.0-or-later
- ubuntu noble: librheolef-dev 7.2-3build5 Β· GPL-3.0-or-later
- ubuntu questing: librheolef-dev 7.2-4build1
- π girlified by deepseek-ai/DeepSeek-V4.1-Flash on : a language model's rewrite of the original, under its terms