git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@2906 f3b2605a-c512-4ea7-a41b-209d697bcdaa
This commit is contained in:
@ -781,11 +781,11 @@ profile consistent with the applied shear strain rate.
|
|||||||
<A NAME = "4_14"></A><H4>4.14 Extended spherical and aspherical particles
|
<A NAME = "4_14"></A><H4>4.14 Extended spherical and aspherical particles
|
||||||
</H4>
|
</H4>
|
||||||
<P>Typical MD models treat atoms or particles as point masses.
|
<P>Typical MD models treat atoms or particles as point masses.
|
||||||
Sometimes, however, it is desirable to have a model where the
|
Sometimes, however, it is desirable to have a model with finite-size
|
||||||
particles are extended spherioids or extended aspherical paticles such
|
particles such as spherioids or aspherical ellipsoids. The difference
|
||||||
as an ellipsoid. The difference is that such particles have a moment
|
is that such particles have a moment of inertia, rotational energy,
|
||||||
of inertia, rotational energy, and angular momentum. Rotation is
|
and angular momentum. Rotation is induced by torque from interactions
|
||||||
induced by torque from interactions with other particles.
|
with other particles.
|
||||||
</P>
|
</P>
|
||||||
<P>LAMMPS has several options for running simulations with these kinds of
|
<P>LAMMPS has several options for running simulations with these kinds of
|
||||||
particles. The following aspects are discussed in turn:
|
particles. The following aspects are discussed in turn:
|
||||||
@ -798,14 +798,14 @@ particles. The following aspects are discussed in turn:
|
|||||||
</UL>
|
</UL>
|
||||||
<H5>Atom styles
|
<H5>Atom styles
|
||||||
</H5>
|
</H5>
|
||||||
<P>There are 3 <A HREF = "atom_style.html">atom styles</A> that define extended
|
<P>There are 3 <A HREF = "atom_style.html">atom styles</A> that allow for definition of
|
||||||
particles: granular, dipole, ellipsoid.
|
finite-size particles: granular, dipole, ellipsoid.
|
||||||
</P>
|
</P>
|
||||||
<P>Granular particles are extended spheriods and each particle can have a
|
<P>Granular particles are spheriods and each particle can have a unique
|
||||||
unique diameter and mass (or density). These particles store
|
diameter and mass (or density). These particles store an angular
|
||||||
an angular velocity (omega) and can be acted upon by torque.
|
velocity (omega) and can be acted upon by torque.
|
||||||
</P>
|
</P>
|
||||||
<P>Dipole particles are extended spheriods with a point dipole and each
|
<P>Dipolar particles are typically spheriods with a point dipole and each
|
||||||
particle type has a diamater and mass, set by the <A HREF = "shape.html">shape</A>
|
particle type has a diamater and mass, set by the <A HREF = "shape.html">shape</A>
|
||||||
and <A HREF = "mass.html">mass</A> commands. These particles store an angular
|
and <A HREF = "mass.html">mass</A> commands. These particles store an angular
|
||||||
velocity (omega) and can be acted upon by torque. They also store an
|
velocity (omega) and can be acted upon by torque. They also store an
|
||||||
@ -817,31 +817,36 @@ to initialize the orientation of dipole moments.
|
|||||||
ellipsoidal shape and mass, defined by the <A HREF = "shape.html">shape</A> and
|
ellipsoidal shape and mass, defined by the <A HREF = "shape.html">shape</A> and
|
||||||
<A HREF = "mass.html">mass</A> commands. These particles store an angular momentum
|
<A HREF = "mass.html">mass</A> commands. These particles store an angular momentum
|
||||||
and their orientation (quaternion), and can be acted upon by torque.
|
and their orientation (quaternion), and can be acted upon by torque.
|
||||||
They do not store an angular velocity (omega) which can be in a
|
They do not store an angular velocity (omega), which can be in a
|
||||||
different direction than angular momentum. The <A HREF = "set.html">set</A> command
|
different direction than angular momentum, rather they compute it as
|
||||||
can be used to initialize the orientation of ellipsoidal particles and
|
needed. Ellipsoidal particles can also store a dipole moment if an
|
||||||
has a brief explanation of quaternions.
|
<A HREF = "atom_style.html">atom_style hybrid ellipsoid dipole</A> is used. The
|
||||||
|
<A HREF = "set.html">set</A> command can be used to initialize the orientation of
|
||||||
|
ellipsoidal particles and has a brief explanation of quaternions.
|
||||||
</P>
|
</P>
|
||||||
<P>Note that if one of these atom styles is used (or multiple styles via
|
<P>Note that if one of these atom styles is used (or multiple styles via
|
||||||
the <A HREF = "atom_style.html">atom_style hybrid</A> command), not all particles in
|
the <A HREF = "atom_style.html">atom_style hybrid</A> command), not all particles in
|
||||||
the system are required to be extended or aspherical. For example, if
|
the system are required to be finite-size or aspherical. For example,
|
||||||
the 3 shape parameters are set to the same value, the particle will be
|
if the 3 shape parameters are set to the same value, the particle will
|
||||||
a spheroid rather than an ellipsoid. If the dipole moment is set to
|
be a spheroid rather than an ellipsoid. If the 3 shape parameters are
|
||||||
zero, the particle will not have a point dipole associated with it.
|
all set to 0.0 or if the diameter is set to 0.0, it will be a point
|
||||||
The pair styles used to compute pairwise interactions will typically
|
particle. If the dipole moment is set to zero, the particle will not
|
||||||
compute the correct interaction in these simplified (cheaper) cases.
|
have a point dipole associated with it. The pair styles used to
|
||||||
<A HREF = "pair_hybrid.html">Pair_style hybrid</A> can be used to insure the correct
|
compute pairwise interactions will typically compute the correct
|
||||||
|
interaction in these simplified (cheaper) cases. <A HREF = "pair_hybrid.html">Pair_style
|
||||||
|
hybrid</A> can be used to insure the correct
|
||||||
interactions are computed for the appropriate style of interactions.
|
interactions are computed for the appropriate style of interactions.
|
||||||
Likewise, using groups to partition particles (ellipsoid versus
|
Likewise, using groups to partition particles (ellipsoid versus
|
||||||
spheroid versus point particles) will allow you to use the appropriate
|
spheroid versus point particles) will allow you to use the appropriate
|
||||||
time integrators and temperature computations for each class of
|
time integrators and temperature computations for each class of
|
||||||
particles. See the doc pages for various commands for details.
|
particles. See the doc pages for various commands for details.
|
||||||
</P>
|
</P>
|
||||||
<P>Also note that for <A HREF = "dimension.html">2d simulations</A>, extended spheroids
|
<P>Also note that for <A HREF = "dimension.html">2d simulations</A>, finite-size
|
||||||
and ellipsoids are still treated as 3d particles, rather than as disks
|
spheroids and ellipsoids are still treated as 3d particles, rather
|
||||||
or ellipses. This means they still have a moment of inertia for a 3d
|
than as disks or ellipses. This means they have the same moment of
|
||||||
extended object. When their temperature is coomputed, the correct
|
inertia for a 3d extended object. When their temperature is
|
||||||
degrees of freedom are used for rotation in a 2d versus 3d system.
|
coomputed, the correct degrees of freedom are used for rotation in a
|
||||||
|
2d versus 3d system.
|
||||||
</P>
|
</P>
|
||||||
<H5>Pair potentials
|
<H5>Pair potentials
|
||||||
</H5>
|
</H5>
|
||||||
@ -927,8 +932,8 @@ particles as a rigid body, computes its inertia tensor, sums the total
|
|||||||
force and torque on the rigid body each timestep due to forces on its
|
force and torque on the rigid body each timestep due to forces on its
|
||||||
constituent particles, and integrates the motion of the rigid body.
|
constituent particles, and integrates the motion of the rigid body.
|
||||||
</P>
|
</P>
|
||||||
<P>(NOTE: 6/08 the feature described in the following paragraph has
|
<P>(NOTE: the feature described in the following paragraph has not yet
|
||||||
not yet been released. It will be soon.)
|
been released. It will be soon.)
|
||||||
</P>
|
</P>
|
||||||
<P>If any of the constituent particles of a rigid body are extended
|
<P>If any of the constituent particles of a rigid body are extended
|
||||||
particles (spheroids or ellipsoids), then their contribution to the
|
particles (spheroids or ellipsoids), then their contribution to the
|
||||||
|
|||||||
@ -774,11 +774,11 @@ An alternative method for calculating viscosities is provided via the
|
|||||||
4.14 Extended spherical and aspherical particles :link(4_14),h4
|
4.14 Extended spherical and aspherical particles :link(4_14),h4
|
||||||
|
|
||||||
Typical MD models treat atoms or particles as point masses.
|
Typical MD models treat atoms or particles as point masses.
|
||||||
Sometimes, however, it is desirable to have a model where the
|
Sometimes, however, it is desirable to have a model with finite-size
|
||||||
particles are extended spherioids or extended aspherical paticles such
|
particles such as spherioids or aspherical ellipsoids. The difference
|
||||||
as an ellipsoid. The difference is that such particles have a moment
|
is that such particles have a moment of inertia, rotational energy,
|
||||||
of inertia, rotational energy, and angular momentum. Rotation is
|
and angular momentum. Rotation is induced by torque from interactions
|
||||||
induced by torque from interactions with other particles.
|
with other particles.
|
||||||
|
|
||||||
LAMMPS has several options for running simulations with these kinds of
|
LAMMPS has several options for running simulations with these kinds of
|
||||||
particles. The following aspects are discussed in turn:
|
particles. The following aspects are discussed in turn:
|
||||||
@ -791,14 +791,14 @@ rigid bodies composed of extended particles :ul
|
|||||||
|
|
||||||
Atom styles :h5
|
Atom styles :h5
|
||||||
|
|
||||||
There are 3 "atom styles"_atom_style.html that define extended
|
There are 3 "atom styles"_atom_style.html that allow for definition of
|
||||||
particles: granular, dipole, ellipsoid.
|
finite-size particles: granular, dipole, ellipsoid.
|
||||||
|
|
||||||
Granular particles are extended spheriods and each particle can have a
|
Granular particles are spheriods and each particle can have a unique
|
||||||
unique diameter and mass (or density). These particles store
|
diameter and mass (or density). These particles store an angular
|
||||||
an angular velocity (omega) and can be acted upon by torque.
|
velocity (omega) and can be acted upon by torque.
|
||||||
|
|
||||||
Dipole particles are extended spheriods with a point dipole and each
|
Dipolar particles are typically spheriods with a point dipole and each
|
||||||
particle type has a diamater and mass, set by the "shape"_shape.html
|
particle type has a diamater and mass, set by the "shape"_shape.html
|
||||||
and "mass"_mass.html commands. These particles store an angular
|
and "mass"_mass.html commands. These particles store an angular
|
||||||
velocity (omega) and can be acted upon by torque. They also store an
|
velocity (omega) and can be acted upon by torque. They also store an
|
||||||
@ -810,31 +810,36 @@ Ellipsoid particles are aspherical. Each particle type has an
|
|||||||
ellipsoidal shape and mass, defined by the "shape"_shape.html and
|
ellipsoidal shape and mass, defined by the "shape"_shape.html and
|
||||||
"mass"_mass.html commands. These particles store an angular momentum
|
"mass"_mass.html commands. These particles store an angular momentum
|
||||||
and their orientation (quaternion), and can be acted upon by torque.
|
and their orientation (quaternion), and can be acted upon by torque.
|
||||||
They do not store an angular velocity (omega) which can be in a
|
They do not store an angular velocity (omega), which can be in a
|
||||||
different direction than angular momentum. The "set"_set.html command
|
different direction than angular momentum, rather they compute it as
|
||||||
can be used to initialize the orientation of ellipsoidal particles and
|
needed. Ellipsoidal particles can also store a dipole moment if an
|
||||||
has a brief explanation of quaternions.
|
"atom_style hybrid ellipsoid dipole"_atom_style.html is used. The
|
||||||
|
"set"_set.html command can be used to initialize the orientation of
|
||||||
|
ellipsoidal particles and has a brief explanation of quaternions.
|
||||||
|
|
||||||
Note that if one of these atom styles is used (or multiple styles via
|
Note that if one of these atom styles is used (or multiple styles via
|
||||||
the "atom_style hybrid"_atom_style.html command), not all particles in
|
the "atom_style hybrid"_atom_style.html command), not all particles in
|
||||||
the system are required to be extended or aspherical. For example, if
|
the system are required to be finite-size or aspherical. For example,
|
||||||
the 3 shape parameters are set to the same value, the particle will be
|
if the 3 shape parameters are set to the same value, the particle will
|
||||||
a spheroid rather than an ellipsoid. If the dipole moment is set to
|
be a spheroid rather than an ellipsoid. If the 3 shape parameters are
|
||||||
zero, the particle will not have a point dipole associated with it.
|
all set to 0.0 or if the diameter is set to 0.0, it will be a point
|
||||||
The pair styles used to compute pairwise interactions will typically
|
particle. If the dipole moment is set to zero, the particle will not
|
||||||
compute the correct interaction in these simplified (cheaper) cases.
|
have a point dipole associated with it. The pair styles used to
|
||||||
"Pair_style hybrid"_pair_hybrid.html can be used to insure the correct
|
compute pairwise interactions will typically compute the correct
|
||||||
|
interaction in these simplified (cheaper) cases. "Pair_style
|
||||||
|
hybrid"_pair_hybrid.html can be used to insure the correct
|
||||||
interactions are computed for the appropriate style of interactions.
|
interactions are computed for the appropriate style of interactions.
|
||||||
Likewise, using groups to partition particles (ellipsoid versus
|
Likewise, using groups to partition particles (ellipsoid versus
|
||||||
spheroid versus point particles) will allow you to use the appropriate
|
spheroid versus point particles) will allow you to use the appropriate
|
||||||
time integrators and temperature computations for each class of
|
time integrators and temperature computations for each class of
|
||||||
particles. See the doc pages for various commands for details.
|
particles. See the doc pages for various commands for details.
|
||||||
|
|
||||||
Also note that for "2d simulations"_dimension.html, extended spheroids
|
Also note that for "2d simulations"_dimension.html, finite-size
|
||||||
and ellipsoids are still treated as 3d particles, rather than as disks
|
spheroids and ellipsoids are still treated as 3d particles, rather
|
||||||
or ellipses. This means they still have a moment of inertia for a 3d
|
than as disks or ellipses. This means they have the same moment of
|
||||||
extended object. When their temperature is coomputed, the correct
|
inertia for a 3d extended object. When their temperature is
|
||||||
degrees of freedom are used for rotation in a 2d versus 3d system.
|
coomputed, the correct degrees of freedom are used for rotation in a
|
||||||
|
2d versus 3d system.
|
||||||
|
|
||||||
Pair potentials :h5
|
Pair potentials :h5
|
||||||
|
|
||||||
@ -920,8 +925,8 @@ particles as a rigid body, computes its inertia tensor, sums the total
|
|||||||
force and torque on the rigid body each timestep due to forces on its
|
force and torque on the rigid body each timestep due to forces on its
|
||||||
constituent particles, and integrates the motion of the rigid body.
|
constituent particles, and integrates the motion of the rigid body.
|
||||||
|
|
||||||
(NOTE: 6/08 the feature described in the following paragraph has
|
(NOTE: the feature described in the following paragraph has not yet
|
||||||
not yet been released. It will be soon.)
|
been released. It will be soon.)
|
||||||
|
|
||||||
If any of the constituent particles of a rigid body are extended
|
If any of the constituent particles of a rigid body are extended
|
||||||
particles (spheroids or ellipsoids), then their contribution to the
|
particles (spheroids or ellipsoids), then their contribution to the
|
||||||
|
|||||||
Reference in New Issue
Block a user