A finite element specifies a reference region, a finite-dimensional space of local trial functions, and degrees of freedom that uniquely determine each such function. Assembling compatible copies over a finite element mesh gives a global trial space. For a one-dimensional linear element, the region is an interval, the functions are affine functions, and the degrees of freedom are the endpoint values.
The quadratic Lagrange triangle uses degree-at-most-two polynomials on a nondegenerate triangle, with point evaluation at its three polygon vertices and three edge midpoints as the six finite element degrees of freedom. If are the affine functions of its barycentric coordinate system, the cardinal shape functions are
At a polygon vertex, one coordinate in the barycentric coordinate system is one and the others vanish; at an edge midpoint, two are and the third is zero. These values prove the cardinal property. Since , this is an unisolvent finite element. Matching the two endpoint values and midpoint value on a shared edge of a polygon matches the whole quadratic restriction, producing a continuous global conforming finite element space.
A finite element with local shape space and finite element degrees of freedom is unisolvent when each possible list of values determines exactly one member of . By the rank-nullity theorem, it suffices to show that for every implies . Equivalently, one may construct a cardinal basis with . Such a basis is linearly independent by applying each , and its size makes it span ; then .
A finite element degree of freedom is one of the linear functionals chosen to specify a local shape function in a finite-dimensional vector space . Examples are point evaluation functionals and edge or cell integrals. The finite element is an unisolvent finite element when the complete list gives a bijection from to the corresponding list of real values.

Articles by others on the same topic (0)

There are currently no matching articles.