In mathematics, particularly numerical analysis, the Bramble-Hilbert lemma, named after James H. Bramble and Stephen R. Hilbert, bounds the error of an approximation of a function by a polynomial of order at most in terms of derivatives of of order . Both the error of the approximation and the derivatives of are measured by norms on a bounded domain in . This is similar to classical numerical analysis, where, for example, the error of linear interpolation can be bounded using the second derivative of . However, the Bramble-Hilbert lemma applies in any number of dimensions, not just one dimension, and the approximation error and the derivatives of are measured by more general norms involving averages, not just the maximum norm.
Additional assumptions on the domain are needed for the Bramble-Hilbert lemma to hold. Essentially, the boundary of the domain must be "reasonable". For example, domains that have a spike or a slit with zero angle at the tip are excluded. Lipschitz domains are reasonable enough, which includes convex domains and domains with continuously differentiable boundary.
The main use of the Bramble-Hilbert lemma is to prove bounds on the error of interpolation of function by an operator that preserves polynomials of order up to , in terms of the derivatives of of order . This is an essential step in error estimates for the finite element method. The Bramble-Hilbert lemma is applied there on the domain consisting of one element.
The one dimensional case
Before stating the lemma in full generality, it is useful to look at some simple special cases. In one dimension and for a function that has derivatives on interval , the lemma reduces to
:
where is the space of all polynomials of order at most .
In the case when , , , and is twice differentiable, this means that there exists a polynomial of degree one such that for all ,
:
This inequality also follows from the well-known error estimate for linear interpolation by choosing as the linear interpolant of .
tatement of the lemma
Suppose is a bounded domain in , , with boundary and diameter . is the Sobolev space of all function on with weak derivatives of order up to in . Here, is a multiindex, and denotes the derivative times with respect to , times with respect to , and so on. The Sobolev seminorm on consists of the norms of the highest order derivatives,
: