Related Experiment Video
Updated: Feb 27, 2026

Multiscale Sampling of a Heterogeneous Water/Metal Catalyst Interface using Density Functional Theory and Force-Field Molecular Dynamics
Published on: April 12, 2019
A Quadrupolar Fullerene Model System for Benchmarking Enhanced Sampling of Trapped Waters in Free Energy Calculations
Swapnil Wagle1, David L Mobley1,2
1Department of Pharmaceutical Sciences, University of California, Irvine, California 92697, United States.
None:
Enhanced sampling methods, such as hybrid Monte Carlo/molecular dynamics (MC/MD), grand canonical MC/MD, nonequilibrium candidate MC/MD, etc., are widely used to sample the slow rearrangement of interfacial water molecules in binding free energy calculations. However, direct comparison of the accuracies of these methods is oftentimes challenging due to differences in studied systems, simulation parameters, and system setup across studies. To overcome this challenge, we introduce a novel and well-defined model system for benchmarking water sampling methods: a closed, custom-defined C90 fullerene. Our C90 fullerene inherently adopts a distorted oblate-spheroidal geometry rather than being spherical; essentially, C90 is large enough to be almost a miniature, capped nanotube, unlike its C60 "buckyball" sibling. Unlike conventional fullerenes with nonpolar, hydrophobic cavities, our custom-defined fullerene incorporates some level of polarity in the form of modest partial charges, creating a quadrupolar cavity that energetically favors water binding. In our quadrupolar fullerene, positive and negative partial charges are distributed around the polar and the equatorial regions, respectively, on its approximate oblate spheroidal geometry. Due to a significant free energy barrier imposed by the fullerene wall, water exchange between the cavity and bulk solvent is essentially impossible on MD time scales. To allow solvent water to equilibrate in the cavity, we introduce a solvent inlet, by performing Hamiltonian replica exchange (i.e., HREX) simulations, which reveal that the quadrupolar fullerene cavity can accommodate a maximum of two waters. From these HREX simulations, we also identify the water binding sites inside the cavity and their occupancies, which show that fullerene conformations with 2 or 1 waters inside the cavity are dominant, with nearly equal free energies. We further validate a nonequilibrium switching (NES) protocol for computing water displacement free energies, by removing a water from the conformations with 2 waters inside the cavity and comparing with the relevant free energies from the HREX simulations. Our NES free energies agree within statistical error with those obtained from HREX. Our findings establish the quadrupolar fullerene as a well-defined, reproducible test system for rigorously benchmarking current as well as future enhanced sampling techniques targeting slow water sampling in confined environments.
More Related Videos
13:58Probing C84-embedded Si Substrate Using Scanning Probe Microscopy and Molecular Dynamics
Published on: September 28, 2016
08:44Measurements of Long-range Electronic Correlations During Femtosecond Diffraction Experiments Performed on Nanocrystals of Buckminsterfullerene
Published on: August 22, 2017
Related Concept Videos
Valence Bond Theory
Structure of Benzene: Molecular Orbital Model
Molecular Geometry and Dipole Moments
Hückel's Rule Diagram of π MOs: Frost Circle
A Frost circle is constructed by drawing a polygon whose number of edges is equal to the number of carbons of the given cyclic system, with one of the vertices pointing down. Then, a circle is drawn enclosing the polygon so that...
Mass Analyzers: Common Types
Molecular Models