vp.liquids.md_nve
Molecular dynamics of Lennard-Jones atoms at constant N, V and E: velocity Verlet in a periodic cubic box, the potential cut and shifted at r_cut. A run returns the block and run averages of the energy, pressure and temperatures (cut-and-shifted, and with long-range corrections as an estimate for the full potential), the heat capacity from the kinetic energy's fluctuations, the fluctuation of the conserved energy, the final configuration, and, when it samples the trajectory, g(r), the velocity autocorrelation function, the mean-square displacement and the diffusion coefficient from each.
Part of the distribution vipyr-liquids; it runs from a checkout of the
repository. Planned on PyPI as pip install vipyr-liquids.
Signature
vp.liquids.md_nve(*, n=256, density=0.75, temperature=1.0, r_cut=2.5, dt=0.005, nblock=10, nstep=1000, neighbors="all", seed=1, r_start=zeros(0, DIM), v_start=zeros(0, DIM), box_start=0.0, sample=0, gr_dr=0.02, nt=200, origin_interval=10) Parameters
- n : int, default
256 - The number of atoms, 4 nc^3 for the fcc start (32, 108, 256, 500, 864, ...); ignored when r_start is given. Range: >= 32, <= 100000.
- density : float, default
0.75 - The number density N / V; sets the box side when r_start is not given. Range: > 0.
- temperature : float, default
1.0 - The temperature of the starting velocities (3N - 3 degrees of freedom). Range: > 0.
- r_cut : float, default
2.5 - The potential's cutoff, in sigma; at most half the box. Range: > 0.
- dt : float, default
0.005 - The time step, in units of sigma sqrt(m / epsilon). Range: > 0.
- nblock : int, default
10 - The number of blocks the run is averaged in. Range: >= 1, <= 100000.
- nstep : int, default
1000 - The steps per block (upstream's default is 20000). Range: >= 0, <= 100000000.
- neighbors : str, default
"all" - How pairs are found: "all" pairs, "link" lists of cells (needs a box of 3 r_cut or more), or "verlet" lists. Range: one of all, link, verlet.
- seed : int, default
1 - The seed of the starting velocities' random numbers. Range: >= 0, <= 2147483646.
- r_start : ndarray[float64], default
zeros(0, DIM) - A starting configuration (N, 3), in sigma, instead of the fcc lattice; box_start must come with it. Range: rank 2.
- v_start : ndarray[float64], default
zeros(0, DIM) - The starting velocities (N, 3) that go with r_start. Range: rank 2.
- box_start : float, default
0.0 - The box side of r_start, in sigma. Range: >= 0.
- sample : int, default
0 - Every this many steps, the configuration goes into g(r) and the correlation functions; 0: none. Range: >= 0, <= 100000000.
- gr_dr : float, default
0.02 - The bin width of g(r), in sigma. Range: > 0.
- nt : int, default
200 - The correlation functions run over 0 to nt samples apart. Range: >= 1, <= 1000000.
- origin_interval : int, default
10 - A time origin every this many samples. Range: >= 1, <= 1000000.
Returns
A frozen MDResult. Iterating it gives the fields below in order; it also has
params, tests, log and check().
- box : float
- The box side, in sigma.
- rho : float
- The number density N / V.
- e_cs : float
- The energy per atom, cut-and-shifted potential, kinetic plus potential (conserved).
- e_cs_err : float
- Its standard error from the block averages (the scatter of a conserved quantity's block means).
- p_cs : float
- The pressure, cut-and-shifted potential.
- p_cs_err : float
- Its standard error from the block averages.
- e_full : float
- The energy per atom with the long-range correction: an estimate for the full potential.
- e_full_err : float
- Its standard error.
- p_full : float
- The pressure with the long-range correction.
- p_full_err : float
- Its standard error.
- t_kin : float
- The kinetic temperature, 2 K / (3N - 3).
- t_kin_err : float
- Its standard error.
- t_config : float
- The configurational temperature, |F|^2 / (lap U - 2 F.H.F / |F|^2).
- t_config_err : float
- Its standard error.
- cv_cs : float
- The heat capacity per atom from the fluctuations of the kinetic energy (Lebowitz, Percus and Verlet).
- cv_cs_err : float
- Its standard error.
- conserved_msd : float
- The mean-square deviation of the energy per atom within a block, averaged over blocks: zero for exact dynamics, about dt^4 for velocity Verlet.
- blocks : ndarray[float64]
- The block averages, one row per block, columns e_cs, p_cs, e_full, p_full, t_kin, t_config, cv_cs, conserved_msd (rank 2).
- initial : ndarray[float64]
- The same eight variables at the start (the last two are fluctuation terms of one step).
- energy_series : ndarray[float64]
- E_cs at every step.
- r_final : ndarray[float64]
- The final positions (N, 3), in sigma, in the box centered on the origin (rank 2).
- v_final : ndarray[float64]
- The final velocities (N, 3) (rank 2).
- verlet_rebuilds : int
- How many times the Verlet list was built (neighbors = "verlet").
- gr_r : ndarray[float64]
- The midpoints of the g(r) bins, in sigma.
- gr : ndarray[float64]
- G(r) at those midpoints.
- vacf : ndarray[float64]
- The velocity autocorrelation function <v(0) . v(t)> at corr_time.
- rvcf : ndarray[float64]
- <v(0) . (r(t) - r(0))>, whose derivative is the VACF and whose limit is 3 D.
- msd : ndarray[float64]
- The mean-square displacement <|r(t) - r(0)|^2>.
- d_vacf : float
- The diffusion coefficient, one third of the integral of the VACF over the range.
- d_msd : float
- The diffusion coefficient, one sixth of the slope of the MSD over the second half of the range.
- corr_time : ndarray[float64]
- The times of the correlation functions: 0 to nt samples, sample dt apart.
Raises
- vipyr.ParameterError
- A ValueError: an argument outside its range, choices, rank or shape, or one of a group given without the rest; its .param names the argument.
- TypeError
- An argument of the wrong type, or an unknown keyword.
- vipyr.VivBuildError
- An ImportError: no C compiler, or the program's C does not build.
- RuntimeError
- The program stops with its own message (a combination it rejects, or no convergence where the program treats that as an error).
Examples
import vipyr as vp
# 108 atoms at density 0.75 from an fcc lattice at T = 1, 2 blocks of 100 steps
r = vp.liquids.md_nve(n=108, nblock=2, nstep=100)
print(r.e_cs, r.p_cs, r.p_cs_err, r.t_kin, r.conserved_msd)
assert r.check() -3.9319204101307355 -1.3108089735137647 0.3095019039543647 0.6025736821262984 1.730485088557998e-08Each example ran as written when these pages were generated, and the output shown is what it printed.
Checked against
- Eos
- Thol et al., Journal of Physical and Chemical Reference Data 45, 023101 (2016) and International Journal of Thermophysics 36, 25 (2015), as eos_lj computes them
- Tests
- ports/liquids/test_liquids.py: every tolerance is stated beside its check
- Upstream
- md_nve_lj (and its md_nve_lj_ll and md_nve_lj_vl builds) of https://github.com/Allen-Tildesley/examples at 4818bc82, built with gfortran -O2 by ports/liquids/oracle/build.py; same bits from the same start
Credits
- A port of the examples of Allen and Tildesley's Computer Simulation of Liquids, which are CC0-1.0.
Source
- Manifest: ports/liquids/md_nve.export.toml
- Viv: ports/liquids/md_nve.viv
- The defs it reaches and the calls between them: map of the code