Phone: 780-641-1600
Fax: 780-641-1601
Email: nintinfo@nrc.gc.ca
11421 Saskatchewan Drive
Edmonton,
Alberta,
T6G 2M9
Canada
From electronic structure and molecular interactions, through statistical-physical theory, towards modelling of system functioning
The Theory and Modelling researchers at NINT are developing theory, modelling, and simulation of nanosystems on multiple length and time scales. Our approach integrates the following levels, from the electronic structure to system functioning:
Integral Equation Theory of Molecular Liquids (3) is a statistical physical theory that bridges the gap between the atomistic simulations (2) and the system functioning level (4). The integral equation theory takes proper account of molecular interactions in condensed matter systems, such as molecular liquids and solutions, complex fluids, polymers in melts and solutions, biomolecules and supramolecules in solution, solid solutions, defects in crystals, and disordered materials.
A challenge of nanotechnology is that the essential properties of nanosystems are determined by molecular interactions, whereas the overall length and time scales are usually very large. For instance, the relaxation time in liquid crystals can vary from microseconds to minutes, depending on the environment. Our bottom-up approach enables efficient simulation of nanosystems at realistic length and time scales, while staying on ab-initio grounds.
Approach
We use integral equation theory to provide realistic physical and chemical description of solutions, complex liquids, and other disordered systems, including nanoporous materials, solid solutions, and defects in crystals. This approach employs atomistic force fields, such as the Optimized Potential for Liquid Simulation (OPLS) or Assisted Model Building with Energy Refinement (AMBER). By solving integro-differential equations for the correlation functions in condensed matter, the formalism yields the structure of the system, statistically averaged over the ensemble of all possible configurations. The thermodynamic functions (such as the free energy, entropy, compressibility, partial molar volume, etc.) are in turn derived analytically from the correlation functions. The method properly accounts for chemical specificities of the species involved.
A crucial advantage of the integral equation approach is that it samples the phase space of the system on arbitrarily large volume and time scales. This overcomes the well-known limitations of molecular simulations which treat individual trajectories of a finite number of particles in a finite, quite limited time frame.
In the three-dimensional form, this theory provides a detailed solvation structure of molecules and supramolecular clusters in solution and at interfaces.
We self-consistently integrate the statistical physical theory with the other levels in our bottom-up approach. This yields computationally efficient simulation of nanosystems.
Examples:
SCF Kohn-Sham DFT / 3D-RISM-KH
RISM-KH / Kinetic MC
Research Interests