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PNNL-13501 - Pacific Northwest National Laboratory

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Figure 5a. OSO volume rendering of a 1240 atom portion of<br />

the protein with empirical formula C382H632N115O106S5.<br />

This macromolecule will be used for charge density<br />

distribution modeling by Tjerk Straatsma. This work<br />

requires extremely fast Poisson solves on minimal surfaces.<br />

Figure 5b. The adaptive average Laplacian surface<br />

enclosing the 1240 atom macromolecule built using NWGrid<br />

and NWPhys. This is a minimal surface with the property<br />

that the local average curvature of any point on the surface<br />

grid is nearly flat relative to its nearest neighbor points. The<br />

surface has the minimal surface area to enclosed volume<br />

ratio.<br />

The TRUEGRID package (XYZ Scientific Applications,<br />

Inc., Livermore, California) for generating structured<br />

grids. Each of these codes contains full-physics<br />

capability and is quite complex, so that we continue to<br />

invest extensive efforts toward learning to run these<br />

codes.<br />

We have models in development of SST S-SX embedded<br />

with single-shell tanks, a 1240 atom biomolecule, two ion<br />

trap experiments designed by Dr. Steven Barlow (EMSL),<br />

and a local atmospheric flow through a mountain ravine<br />

in New Mexico. We also have demonstrated that these<br />

grid technologies may be used in molecular modeling<br />

studies, for example, protein folding, and in systematic<br />

extension of hydrodynamics to the molecular scale.<br />

The computational applied mathematics that underlies the<br />

areas of reactive transport and computational chemistry<br />

includes PDEs, stochastic analysis, and numerical<br />

methods. These applications require the fast and accurate<br />

solution of quasi-linear and nonlinear PDEs derived from<br />

equilibrium and nonequilibrium phenomena that are<br />

formulated as coupled dynamical systems composed of<br />

reaction-diffusion equations. In terms of mathematical<br />

techniques, the difficulties lie in the development of<br />

methods to manipulate discontinuous functions and<br />

derivatives, as well as multidimensional singularities and<br />

couplings. Many of the mathematical challenges in<br />

solving these problems have a common origin in the<br />

inherent geometry of the physics, and include highly<br />

oscillatory coefficients, steep gradients, or extreme<br />

curvatures at the moving and mixing shock fronts at<br />

interfaces that are singular analytically.<br />

To simulate the physical process more accurately, new<br />

mathematical formulations of the physical problem, its<br />

inherent geometry, its boundary conditions and solution<br />

techniques, such as that developed previously by us, were<br />

developed in conjunction with applications, grids, and<br />

algorithmic and computational implementations. We<br />

continued this work in FY 2000, with increasing emphasis<br />

on geometrically faithful gridding, and plan to initiate an<br />

investigation of stochastic grids. In FY 2000, we hired<br />

Dr. Harold E. Trease and established NWGrid and<br />

NWPhys as the flagship codes for the Applied<br />

Mathematics Group within Theory, Modeling and<br />

Simulation at EMSL.<br />

Summary and Conclusions<br />

It is our intention to identify and analyze the inherent<br />

assumptions in each model and analyze the ramifications<br />

of those assumptions on the appropriateness of the<br />

presently used solution techniques, as well as the<br />

constraints that they impose on the integration process of<br />

the information generated/shared by the multiscale<br />

physical chemistry models. It is our belief that when the<br />

invariant geometry of a problem is captured and<br />

maintained throughout an analysis, the greatest fidelity of<br />

the results will be achieved and the physical mechanisms<br />

of information transport across temporal and spatial scales<br />

will be revealed. Our focus is on capturing the relevant<br />

physics/chemistry—selection of the particular numerical<br />

solution scheme is to be based in the inherent geometric<br />

constraints of the problem to ensure preservation of<br />

invariants. Subsequently, we will begin to unify the<br />

models via a mid-scale model that will capture the<br />

fundamental physics and chemistry of the problem of<br />

interest.<br />

Computational Science and Engineering 115

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