Maximum Entropy Approximation
AIP Conf. Proc. -- November 23, 2005 -- Volume 803, pp. 337-344
BAYESIAN INFERENCE AND MAXIMUM ENTROPY METHODS IN SCIENCE AND ENGINEERING: 25th International Workshop on Bayesian Inference and Maximum Entropy Methods in Science and Engineering;
doi:10.1063/1.2149812
Issue Date: 23 November 2005
You are not logged in. Log in
In this paper, the construction of scattered data approximants is studied using the principle of maximum entropy. For under-determined and ill-posed problems, Jaynes's principle of maximum information-theoretic entropy is a means for least-biased statistical inference when insufficient information is available. Consider a set of distinct nodes {xi}
in Rd, and a point p with coordinate x that is located within the convex hull of the set {xi}. The convex approximation of a function u(x) is written as: uh(x) = 
i(x)ui, where {
i}
0 are known as shape functions, and uh must reproduce affine functions (d = 2): 
i = 1, 
ixi = x, 
iyi = y. We view the shape functions as a discrete probability distribution, and the linear constraints as the expectation of a linear function. For n > 3, the problem is under-determined. To obtain a unique solution, we compute
i by maximizing the uncertainty H(
) = 
i log
i, subject to the above three constraints. In this approach, only the nodal coordinates are used, and neither the nodal connectivity nor any user-defined parameters are required to determine
ithe defining characteristics of a mesh-free Galerkin approximant. Numerical results for {
i}
are obtained using a convex minimization algorithm, and shape function plots are presented for different nodal configurations. ©2005 American Institute of Physics

i(x)ui, where {
i}
0 are known as shape functions, and uh must reproduce affine functions (d = 2): 
i = 1, 
ixi = x, 
iyi = y. We view the shape functions as a discrete probability distribution, and the linear constraints as the expectation of a linear function. For n > 3, the problem is under-determined. To obtain a unique solution, we compute
i by maximizing the uncertainty H(
) = 
i log
i, subject to the above three constraints. In this approach, only the nodal coordinates are used, and neither the nodal connectivity nor any user-defined parameters are required to determine
ithe defining characteristics of a mesh-free Galerkin approximant. Numerical results for {
i}| Permalink: |
http://link.aip.org/link/?APCPCS/803/337/1 |
There are no references.






