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{{Expert-subject|Mathematics|date=February 2009}} | |||
In [[mathematics]], the '''discrete exterior calculus''' ('''DEC''') is the extension of the [[exterior algebra|exterior calculus]] to [[discrete mathematics|discrete]] spaces including [[graph theory|graphs]] and [[finite element method|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 form|differential (''n'' − 1)-form]] ''ω'' over the [[boundary (topology)|boundary]] ∂''M'' of an ''n''-[[dimension]]al manifold ''M'' to the integral of d''ω'' (the [[exterior derivative]] of ''ω'', and a differential ''n''-form on ''M'') over ''M'' itself: | |||
:<math>\int_{M} \mathrm{d} \omega = \int_{\partial M} \omega.</math> | |||
One could think of differential ''k''-forms as [[linear operator]]s 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 | |||
:<math>\langle \mathrm{d} \omega | M \rangle = \langle \omega | \partial M \rangle.</math> | |||
In finite element analysis, the first stage is often the approximation of the domain of interest by a [[triangulation (topology)|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 ''S'' is a (''k'' + 1)-dimensional subcomplex of ''T'' and ''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: | |||
:<math>\langle \mathrm{d} \omega | S \rangle = \langle \omega | \partial S \rangle.</math> | |||
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]] | |||
==References== | |||
*[http://multires.caltech.edu/~keenan/pdf/DGPDEC.pdf SIGGRAPH 2013 Course Notes] | |||
*[http://www.springer.com/computer/image+processing/book/978-1-84996-289-6 Discrete Calculus], Grady, Leo J., Polimeni, Jonathan R., ISBN 978-1-84996-289-6, 2010 | |||
*[http://math.berkeley.edu/~pugh/colloquium_abstracts/harrison.html Discrete Exterior Calculus with Convergence to the Smooth Continuum] | |||
*[http://etd.caltech.edu/etd/available/etd-05202003-095403/unrestricted/thesis_hirani.pdf Hirani Thesis on Discrete Exterior Calculus] | |||
*[http://link.aip.org/link/doi/10.1063/1.2830977 On geometric discretization of elasticity], Arash Yavari, J. Math. Phys. 49, 022901 (2008), DOI:10.1063/1.2830977 | |||
[[Category:Finite element method]] | |||
[[Category:Multilinear algebra]] |
Revision as of 21:13, 10 August 2013
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 dω (the exterior derivative of ω, and a differential n-form on M) over M itself:
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
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 S is a (k + 1)-dimensional subcomplex of T and ω is a k-form on T, then the discrete exterior derivative dω of ω is the unique (k + 1)-form defined so that Stokes' theorem holds:
Other concepts such as the discrete wedge product and the discrete Hodge star can also be defined.
See also
References
- SIGGRAPH 2013 Course Notes
- Discrete Calculus, Grady, Leo J., Polimeni, Jonathan R., ISBN 978-1-84996-289-6, 2010
- Discrete Exterior Calculus with Convergence to the Smooth Continuum
- Hirani Thesis on Discrete Exterior Calculus
- On geometric discretization of elasticity, Arash Yavari, J. Math. Phys. 49, 022901 (2008), DOI:10.1063/1.2830977