lgca.nove_base.NoVE_LGCA_base¶
- class lgca.nove_base.NoVE_LGCA_base(nodes=None, dims=None, restchannels=1, density=0.1, bc='periodic', seed=None, capacity=None, propagation=True, **kwargs)¶
Bases:
LGCA_base,ABCBase class for LGCA without volume exclusion.
- apply_abc()¶
Apply absorbing boundary conditions.
Update
self.nodes, using the shadow border nodes and respecting the geometry.
- apply_inflowbc()¶
Apply inflow boundary conditions.
Update
self.nodes, using the shadow border nodes and respecting the geometry.
- apply_pbc()¶
Apply periodic boundary conditions.
Update
self.nodes, using the shadow border nodes and respecting the geometry.
- apply_rbc()¶
Apply reflecting boundary conditions.
Update
self.nodes, using the shadow border nodes and respecting the geometry.
- abstract property c: ndarray¶
(Class attribute.) Array of the velocity channel vectors. Dimensions:
(dims, lgca.velocitychannels), where dims is 1 or 2 depending on the geometry.
- calc_entropy(base=None)¶
Calculate entropy of the lattice. :type base: :param base: base of the logarithm, defaults to 2 :return: entropy according to information theory as scalar
- calc_flux(nodes)¶
Calculate the flux vector for all lattice sites in nodes.
The elements of the flux vectors are computed as the dot product between the LGCA’s neighborhood vectors and the velocity channel configuration in nodes.
- Parameters:
nodes (
numpy.ndarray) – Lattice configuration to compute the flux for. Must have more than or the same number of dimensions asself.nodesandnodes.shape[-1] >= self.velocitychannels. Is typicallyself.nodes.- Returns:
Array of flux vectors at each lattice site. Dimensions:
nodes.shape[:-1] + (len(self.c),).
- calc_mean_alignment()¶
Calculate the mean alignment measure. The mean alignment is a measure for local alignment of particle orientation in the lattice. It is calculated as the agreement in direction between the flux of a lattice site and the flux of the director field summed up and normalized over all lattice sites. .. note:: This is buggy! :return: Local alignment parameter: ranging from -1 (antiparallel alignment) through 0 (no alignment) to 1 (parallel alignment)
- calc_normalized_entropy(base=None)¶
Calculate entropy of the lattice normalized to maximal possible entropy. :type base: :param base: base of the logarithm, defaults to 2 :return: normalized entropy as scalar
- calc_permutations()¶
Initialize lazy computation structures for permutations. Only compute permutations when actually needed.
- calc_polar_alignment_parameter()¶
Calculate the polar alignment parameter. The polar alignment parameter is a measure for global agreement of particle orientation in the lattice. It is calculated as the magnitude of the sum of the velocities of all particles normalized by the number of particles. :return: Polar alignment parameter of the lattice from 0 (no alignment) to 1 (complete alignment)
- get_flux_permutations(n_particles)¶
Get flux permutations for
n_particles.
- get_permutations(n_particles)¶
Get permutations for
n_particles.- Parameters:
n_particles (int) – Number of occupied channels.
- Returns:
Array of permutations for
n_particles.
- abstractmethod gradient(qty)¶
Compute the gradient of qty along all axes.
- Parameters:
qty (
numpy.ndarray) – Quantity to take the gradient of. Needs to have the same number of dimensions asself.nodes. Ifqty.shape == self.nodes.shape[:-1]the result can be indexed with the LGCA coordinates (see example).- Returns:
Computed gradient. Dimensions:
qty.shape + (len(self.c),). Ifselfandqtyare 2D arrays,gradient(qty)[...,0]is the gradient in x direction andgradient(qty)[...,1]the gradient in y direction.
Notes
The gradient is calculated using
numpy.gradient()with stepwidth h=0.5 (s.t. no normalization takes place). It is computed as the central finite difference with equidistant support points and supports one-sided differences at the boundaries.In most cases this yields the simple difference between the two closest array elements in the given direction. For example, the gradient at position 1 of
np.array([1, 2, 4])would be (4 - 1)/(2 * 0.5) = 3.Examples
If the input quantity has the same x (and y) dimensions as the LGCA’s nodes, the gradient at each node position can be accessed the same way as the node itself.
>>> from lgca import get_lgca >>> import numpy as np >>> # define a square LGCA to illustrate dimensions >>> lgca = get_lgca(geometry='square', dims=(2,3)) >>> lgca.nodes.shape # (xdim, ydim, number of channels) (4, 5, 4) >>> my_qty = np.array([[0,0,0,0,0], >>> [1,1,1,1,1], >>> [2,2,2,3,2], >>> [3,3,3,3,3]]) >>> my_qty.shape # (xdim, ydim) (4, 5) >>> grad = lgca.gradient(my_qty) >>> grad.shape # (xdim, ydim, number of dimensions) (4, 5, 2) >>> # address like internal LGCA fields: first dimension is x (printed vertically), >>> # second dimension is y (printed horizontally), this can be a bit confusing >>> for coord in lgca.coord_pairs: >>> if np.any(grad[coord]>2): >>> print("Gradient at index", coord, "is ", grad[coord]) >>> print("Configuration at index ", coord, " is ", lgca.nodes[coord], >>> ", with cell density ", lgca.cell_density[coord]) Gradient at index (1, 3) is [3. 0.] Configuration at index (1, 3) is [False False False True] , with cell density 1
The first element of the gradient holds the gradient in x direction, the second element the gradient in y direction. Note that
(1, 3)is the index corresponding to a logical non-border coordinate(0, 2)if the interaction radius is 1. This is relevant for defining a custom field qty: Only the field values at non-border indices will be “felt” by the particles in the LGCA if the interaction is defined accordingly, but border nodes can be used to specify the field’s boundary conditions.The gradient in x direction is 3 = (3 - 0)/1. In y direction it is 0 = (1 - 1)/1.
- abstractmethod init_coords()¶
Initialize LGCA coordinates. These are used to index the lattice nodes. In the implementation, set
self.nonborder,self.xcoords,self.ycoords, andself.coord_pairsto meaningful and consistent values.Must match what is done in
set_dims()andinit_nodes(). For the attribute types seelgca.base.LGCA_base.
- abstractmethod init_nodes(density, nodes=None, **kwargs)¶
Initialize LGCA lattice configuration. Create the lattice and then assign particles to channels in the nodes. In the implementation, set
self.nodes.Must match what is done in
set_dims()andinit_coords(). For arguments and attribute types seelgca.base.LGCA_base.
- abstract property interactions: list¶
(Class attribute.) List of interaction functions suitable for this type of LGCA.
- print_interactions()¶
Print the list of pre-implemented interactions for this LGCA type.
- print_nodes()¶
Print the full lattice configuration as integers.
- abstractmethod propagation()¶
Perform the transport step of the LGCA: Move particles through the lattice according to their velocity.
Propagate the particles by updating
self.nodes, respecting the geometry. Boundary conditions are enforced later byapply_boundaries().
- random_reset(density)¶
Populate the lattice from a Poisson distribution with mean
densityper node.
- set_bc(bc)¶
Set the boundary conditions.
Selects a method which is called every timestep to enforce boundary conditions. The methods to select from are implemented in the derived classes. The chosen one is assigned to
self.apply_boundaries().- Parameters:
bc ({'absorbing', 'reflecting', 'periodic', 'inflow'}) – Boundary conditions. Not all bc are supported in all geometries (yet).
- abstractmethod set_dims(dims=None, nodes=None, restchannels=0)¶
Set LGCA dimensions. In the implementation, set
self.K,self.restchannelsandself.dimsto meaningful and consistent values.Must match what is done in
init_coords()andinit_nodes(). For arguments and attribute types seelgca.base.LGCA_base.
- set_interaction(**kwargs)¶
Set the interaction rule and respective needed parameters.
Set
self.interactionand possibly add entries inself.interaction_params. Do not use this to specify a custom interaction. In order to do this (as of now),self.interactionandself.interaction_paramsmust be manipulated directly from an external script.- Parameters:
kwargs['interaction'] (str, default='random_walk') – Name of the predefined interaction in
lgca.interactions.**kwargs – Interaction parameters.
- set_r_int(r)¶
Change the interaction radius. Update shadow border nodes accordingly.
This has effects on
self.nodes, the coordinates and the computed fields.- Parameters:
r (int) – New interaction radius.
- timeevo(timesteps=100, record=False, recordN=False, recorddens=True, showprogress=True, recordorderparams=False, recordpertype=False)¶
Perform a simulation of the LGCA for timesteps timesteps.
Different quantities can be recorded during the simulation, e.g. the total number of particles at each timestep. They are stored in LGCA attributes.
- Parameters:
timesteps (int, default=100) – How long the simulation should be performed.
record (bool, default=False) – Record the full lattice configuration for each timestep in
self.nodes_t.recorddens (bool, default=True) – Record the number of particles at each lattice site for each timestep in
self.dens_t.recordN (bool, default=False) – Record the total number of particles in the lattice for each timestep in
self.n_t.recordpertype (bool, default=False) – Record the number of particles in velocity channels/resting channels at each lattice site for each timestep in
self.velcells_tandself.restcells_t, respectively.showprogress (bool, default=True) – Show a simple progress bar with a percentage of performed timesteps in the standard output.
- timestep()¶
Update the state of the LGCA from time k to k+1. Includes the interaction and propagation steps.
- total_population()¶
Calculate the amount of particles in the lattice.
- Returns:
Total population size.
- update_dynamic_fields()¶
Update “fields” from the current LGCA state that store important variables to compute other dynamic steps.
Computes
self.cell_density, number of particles at each lattice node.
- abstract property velocitychannels: int¶
(Class attribute.) Number of velocity channels.