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lammps/doc/src/angle_mesocnt.rst
2022-09-14 16:29:10 -04:00

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.. index:: angle_style mesocnt
angle_style mesocnt command
===========================
Syntax
""""""
.. code-block:: LAMMPS
angle_style mesocnt
Examples
""""""""
.. code-block:: LAMMPS
angle_style mesocnt
angle_coeff 1 buckling C 10 10 20.0
angle_coeff 4 harmonic C 8 4 10.0
angle_coeff 2 buckling custom 400.0 50.0 5.0
angle_coeff 1 harmonic custom 300.0
Description
"""""""""""
.. versionadded:: 15Sep2022
The *mesocnt* angle style uses the potential
.. math::
E = K_\text{H} \Delta \theta^2, \qquad |\Delta \theta| < \Delta
\theta_\text{B} \\
E = K_\text{H} \Delta \theta_\text{B}^2 +
K_\text{B} (\Delta \theta - \Delta \theta_\text{B}), \qquad |\Delta
\theta| \geq \Delta \theta_\text{B}
where :math:`\Delta \theta = \theta - \pi` is the bending angle of the
nanotube, :math:`K_\text{H}` and :math:`K_\text{B}` are prefactors for
the harmonic and linear regime respectively and :math:`\Delta
\theta_\text{B}` is the buckling angle. Note that the usual 1/2 factor
for the harmonic potential is included in :math:`K_\text{H}`.
The style implements parameterization presets of :math:`K_\text{H}`,
:math:`K_\text{B}` and :math:`\Delta \theta_\text{B}` for mesoscopic
simulations of carbon nanotubes based on the atomistic simulations of
:ref:`(Srivastava) <Srivastava_2>` and buckling considerations of
:ref:`(Zhigilei) <Zhigilei1_1>`.
The following coefficients must be defined for each angle type via the
:doc:`angle_coeff <angle_coeff>` command as in the examples above, or
in the data file or restart files read by the :doc:`read_data
<read_data>` or :doc:`read_restart <read_restart>` commands:
* mode = *buckling* or *harmonic*
* preset = *C* or *custom*
* additional parameters depending on preset
If mode *harmonic* is chosen, the potential is simply harmonic and
does not switch to the linear term when the buckling angle is
reached. In *buckling* mode, the full piecewise potential is used.
Preset *C* is for carbon nanotubes, and the additional parameters are:
* chiral index :math:`n` (unitless)
* chiral index :math:`m` (unitless)
* :math:`r_0` (distance)
Here, :math:`r_0` is the equilibrium distance of the bonds included in
the angle, see :doc:`bond_style mesocnt <bond_mesocnt>`.
In harmonic mode with preset *custom*, the additional parameter is:
* :math:`K_\text{H}` (energy)
Hence, this setting is simply a wrapper for :doc:`bond_style harmonic
<bond_harmonic>` with an equilibrium angle of 180 degrees.
In harmonic mode with preset *custom*, the additional parameters are:
* :math:`K_\text{H}` (energy)
* :math:`K_\text{B}` (energy)
* :math:`\Delta \theta_\text{B}` (degrees)
:math:`\Delta \theta_\text{B}` is specified in degrees, but LAMMPS
converts it to radians internally; hence :math:`K_\text{H}` is
effectively energy per radian\^2 and :math:`K_\text{B}` is energy per
radian.
----------
In *buckling* mode, this angle style adds the *buckled* property to
all atoms in the simulation, which is an integer flag indicating
whether the bending angle at a given atom has exceeded :math:`\Delta
\theta_\text{B}`. It can be accessed as an atomic variable, e.g. for
custom dump commands, as *i_buckled*.
.. note::
If the initial state of the simulation contains buckled nanotubes
and :doc:`pair_style mesocnt <pair_mesocnt>` is used, the
*i_buckled* atomic variable needs to be initialized before the
pair_style is defined by doing a *run 0* command straight after the
angle_style command. See below for an example.
If CNTs are already buckled at the start of the simulation, this
script will correctly initialize *i_buckled*:
.. code-block:: LAMMPS
angle_style mesocnt
angle_coeff 1 buckling C 10 10 20.0
run 0
pair_style mesocnt 60.0
pair_coeff * * C_10_10.mesocnt 1
Restrictions
""""""""""""
This angle style can only be used if LAMMPS was built with the
MOLECULE and MESONT packages. See the :doc:`Build package
<Build_package>` doc page for more info.
Related commands
""""""""""""""""
:doc:`angle_coeff <angle_coeff>`
Default
"""""""
none
----------
.. _Srivastava_2:
**(Srivastava)** Zhigilei, Wei, Srivastava, Phys. Rev. B 71, 165417
(2005).
.. _Zhigilei1_1:
**(Zhigilei)** Volkov and Zhigilei, ACS Nano 4, 6187 (2010).