Next: Introduction
Up: NAMD 2.12b1 User's Guide
Previous: Contents
Contents
Index
- Graph of van der Waals potential with and without switching
- Graph of electrostatic potential with and without shifting function
- Graph of electrostatic split between short and long range forces
- Example of cutoff and pairlist distance uses
- Graph showing a slice of a ramp potential, showing the effect of
mgridforcevoff
- Graphical representation of a Colvars configuration.
- Dual topology description for an alchemical simulation.
Case example of the mutation of alanine into serine.
The lighter color denotes the non-interacting, alternate
state.
- Convergence of an FEP calculation. If the ensembles representative
of states
and
are too disparate, equation (66) will
not converge (a).
If, in sharp contrast, the configurations of
state
form a subset of the ensemble of configurations
characteristic of state
, the simulation is expected
to converge (b).
The difficulties reflected in case (a) may be
alleviated by the introduction of mutually overlapping intermediate
states that connect
to
(c). It should be
mentioned that in practice, the kinetic contribution,
,
is assumed to be identical for state
and state
.
- Relationship of user-defined
to coupling of electrostatic or vdW interactions to a simulation, given specific values of alchElecLambdaStart or alchVdwLambdaEnd.
- Sample TI data (
against
). The blue shaded
area shows the integral with fine sampling close to the end point. The red area
shows the difference when
values are more sparse. In this example,
insufficient sampling before
0.1 can result in a large overestimation
of the integral. Beyond
0.2, sparser sampling is justified as dE/d
is not
changing quickly.
- Schematics of the aMD method. When the original potential (thick line) falls below a threshold energy
(dashed line),
a boost potential is added. The modified energy profiles (thin lines) have smaller barriers separating adjacent
energy basins.
http://www.ks.uiuc.edu/Research/namd/