Skip to content

Commit 6d3fde6

Browse files
committed
implement some change suggested by Cecilia
1 parent e1f4254 commit 6d3fde6

1 file changed

Lines changed: 16 additions & 11 deletions

File tree

lammps-tutorials.tex

Lines changed: 16 additions & 11 deletions
Original file line numberDiff line numberDiff line change
@@ -2418,6 +2418,16 @@ \subsubsection{Stretching the PEG molecule}
24182418
include element names in the dump file and simplify visualization.}
24192419
\end{note}
24202420

2421+
\begin{note}
2422+
{\color{blue}
2423+
Microstates collected during a simulation in the form of a trajectory
2424+
can be analyzed within LAMMPS using the \lmpcmd{rerun} command. This is
2425+
particularly useful, for example, for computing properties not set up in
2426+
the original simulation without having to run it again. A possible use of
2427+
the \lmpcmd{rerun} command is estimating the self-diffusion coefficient
2428+
by using the \lmpcmd{compute msd} command~\cite{frenkel2023understanding}.}
2429+
\end{note}
2430+
24212431
\subsection{Tutorial 4: Nanosheared electrolyte}
24222432
\label{sheared-confined-label}
24232433

@@ -4228,9 +4238,9 @@ \subsubsection{Method 1: Free sampling}
42284238
\paragraph{The limits of free sampling}
42294239

42304240
Increasing the value of $U_0$ reduces the average number of atoms in the central
4231-
region, making it difficult to achieve a high-resolution free energy profile.
4232-
For example, running the same simulation with $U_0 = 10 \epsilon$,
4233-
corresponding to $U_0 \approx 10 k_\text{B} T$, results in no atoms exploring
4241+
region, making it difficult to achieve a high-resolution free energy profile
4242+
{\color{blue} within reasonable simulation times}. For example, running the same
4243+
simulation with $U_0 = 10 \epsilon$, corresponding to $U_0 \approx 10 k_\text{B} T$, results in no atoms exploring
42344244
the central part of the simulation box during the simulation.
42354245
In such a case, employing an enhanced sampling method is recommended, as done in the next section.
42364246

@@ -4699,21 +4709,16 @@ \subsubsection{Simulating the reaction}
46994709
react R2 all 1 0 3.0 mol3 mol4 M-P.rxnmap &
47004710
react R3 all 1 0 5.0 mol5 mol6 P-P.rxnmap
47014711
\end{lstlisting}
4702-
% CA: can someone confirm my changes added in this paragraph? I am unsure of them
4703-
% as I literally just figured it out to write them. (PS: I just realized that some
4704-
% of it may be redundant with the note, but I would still leave it as the reader
4705-
% will have the full information.
47064712
With the \lmpcmd{stabilization} keyword, the \lmpcmd{fix bond/react} command will
47074713
stabilize the atoms involved in the reaction using the \lmpcmd{fix nve/limit}
47084714
command with a maximum displacement of $0.03\,\mathrm{\AA{}}$.
47094715
{\color{blue}The \lmpcmd{fix nve/limit} command functions similar to
47104716
\lmpcmd{fix nve}, but restricts how far atoms can move in a single time step, even with
47114717
very large forces.}
47124718
By default, each reaction is stabilized for 60 time steps. Each \lmpcmd{react} keyword
4713-
corresponds to a reaction, e.g.,~a transformation of \lmpcmd{mol1} into \lmpcmd{mol2}
4714-
based on the atom map \lmpcmd{M-M.rxnmap}. Implementation details about each reaction,
4715-
such as the reaction distance cutoffs and the frequency with which to search for
4716-
reaction sites, are also specified in this command.
4719+
corresponds to a reaction, e.g.,~a transformation of \lmpcmd{mol1} into \lmpcmd{mol2}.
4720+
Implementation details about each reaction, such as the reaction distance cutoffs
4721+
and the frequency with which to search for reaction sites, are also specified in this command.
47174722

47184723
\begin{figure}
47194724
\centering

0 commit comments

Comments
 (0)