Discrete exterior calculus

In mathematics, the discrete exterior calculus (DEC) is the extension of the exterior calculus to discrete spaces including graphs and finite element meshes. DEC methods have proved to be very powerful in improving and analyzing finite element methods: for instance, DEC-based methods allow the use of highly non-uniform meshes to obtain accurate results. Non-uniform meshes are advantageous because they allow the use of large elements where the process to be simulated is relatively simple, as opposed to a fine resolution where the process may be complicated (e.g., near an obstruction to a fluid flow), while using less computational power than if a uniformly fine mesh were used.

The discrete exterior derivative

Stokes' theorem relates the integral of a differential (''n'' − 1)-form ''ω'' over the boundary ∂''M'' of an ''n''-dimensional manifold ''M'' to the integral of d''ω'' (the exterior derivative of ''ω'', and a differential ''n''-form on ''M'') over ''M'' itself:

:$\int_ \mathrm \omega = \int_ \omega.$

One could think of differential ''k''-forms as linear operators that act on ''k''-dimensional "bits" of space, in which case one might prefer to use the bra–ket notation for a dual pairing. In this notation, Stokes' theorem reads as

:$\langle \mathrm \omega \mid M \rangle = \langle \omega \mid \partial M \rangle.$

In finite element analysis, the first stage is often the approximation of the domain of interest by a triangulation, ''T''. For example, a curve would be approximated as a union of straight line segments; a surface would be approximated by a union of triangles, whose edges are straight line segments, which themselves terminate in points. Topologists would refer to such a construction as a simplicial complex. The boundary operator on this triangulation/simplicial complex ''T'' is defined in the usual way: for example, if ''L'' is a directed line segment from one point, ''a'', to another, ''b'', then the boundary ∂''L'' of ''L'' is the formal difference ''b'' − ''a''.

A ''k''-form on ''T'' is a linear operator acting on ''k''-dimensional subcomplexes of ''T''; e.g., a 0-form assigns values to points, and extends linearly to linear combinations of points; a 1-form assigns values to line segments in a similarly linear way. If ''ω'' is a ''k''-form on ''T'', then the discrete exterior derivative d''ω'' of ''ω'' is the unique (''k'' + 1)-form defined so that Stokes' theorem holds:

:$\langle \mathrm{d} \omega \mid S \rangle = \langle \omega \mid \partial S \rangle.$

For every (''k'' + 1)-dimensional subcomplex of ''T'', ''S''. Other concepts such as the discrete wedge product and the discrete Hodge star can also be defined.

See also

*Discrete differential geometry
*Discrete Morse theory
*Topological combinatorics
*Discrete calculus

References

Discrete Calculus
Grady, Leo J., Polimeni, Jonathan R., 2010
Hirani Thesis on Discrete Exterior CalculusConvergence of discrete exterior calculus approximations for Poisson problems
E. Schulz & G. Tsogtgerel, Disc. Comp. Geo. 63(2), 346 - 376, 2020
On geometric discretization of elasticity
Arash Yavari, J. Math. Phys. 49, 022901 (2008), DOI:10.1063/1.2830977
Discrete Differential Geometry: An Applied Introduction
Keenan Crane, 2018

Finite element method
Multilinear algebra