Source code for pycalphad.core.calculate

The calculate module contains a routine for calculating the
property surface of a system.

import itertools
from collections import OrderedDict
import numpy as np
from numpy import broadcast_to
import pycalphad.variables as v
from pycalphad import ConditionError
from pycalphad.codegen.callables import build_phase_records
from pycalphad.core.cache import cacheit
from pycalphad.core.light_dataset import LightDataset
from pycalphad.core.phase_rec import PhaseRecord
from pycalphad.core.utils import endmember_matrix, extract_parameters, \
    filter_phases, generate_dof, instantiate_models, point_sample, \
    unpack_components, unpack_condition, unpack_kwarg

def _sample_phase_constitution(phase_name, phase_constituents, sublattice_dof, comps,
                               variables, sampler, fixed_grid, pdens):
    Sample the internal degrees of freedom of a phase.


    ndarray of points
    # Eliminate pure vacancy endmembers from the calculation
    vacancy_indices = list()
    for idx, sublattice in enumerate(phase_constituents):
        active_in_subl = sorted(set(phase_constituents[idx]).intersection(comps))
        is_vacancy = [spec.number_of_atoms == 0 for spec in active_in_subl]
        subl_va_indices = list(idx for idx, x in enumerate(is_vacancy) if x == True)
    if len(vacancy_indices) != len(phase_constituents):
        vacancy_indices = None
    # Add all endmembers to guarantee their presence
    points = endmember_matrix(sublattice_dof,
    if fixed_grid is True:
        # Sample along the edges of the endmembers
        # These constitution space edges are often the equilibrium points!
        em_pairs = list(itertools.combinations(points, 2))
        lingrid = np.linspace(0, 1, pdens)
        extra_points = [first_em * lingrid[np.newaxis].T +
                        second_em * lingrid[::-1][np.newaxis].T
                        for first_em, second_em in em_pairs]
        points = np.concatenate(list(itertools.chain([points], extra_points)))

    # Sample composition space for more points
    if sum(sublattice_dof) > len(sublattice_dof):
        points = np.concatenate((points,
    # Filter out nan's that may have slipped in if we sampled too high a vacancy concentration
    # Issues with this appear to be platform-dependent
    points = points[~np.isnan(points).any(axis=-1)]
    # Ensure that points has the correct dimensions and dtype
    points = np.atleast_2d(np.asarray(points, dtype=np.float_))
    return points

def _compute_phase_values(components, statevar_dict,
                          points, phase_record, output, maximum_internal_dof, broadcast=True,
                          parameters=None, fake_points=False,
    Calculate output values for a particular phase.

    components : list
        Names of components to consider in the calculation.
    statevar_dict : OrderedDict {str -> float or sequence}
        Mapping of state variables to desired values. This will broadcast if necessary.
    points : ndarray
        Inputs to 'func', except state variables. Columns should be in 'variables' order.
    phase_record : PhaseRecord
        Contains callable for energy and phase metadata.
    output : string
        Desired name of the output result in the Dataset.
    maximum_internal_dof : int
        Largest number of internal degrees of freedom of any phase. This is used
        to guarantee different phase's Datasets can be concatenated.
    broadcast : bool
        If True, broadcast state variables against each other to create a grid.
        If False, assume state variables are given as equal-length lists (or single-valued).
    parameters : OrderedDict {str -> float or sequence}, optional
        Maps SymPy symbols to a scalar or 1-D array. The arrays must be equal length.
        The corresponding PhaseRecord must have been initialized with the same parameters.
    fake_points : bool, optional (Default: False)
        If True, the first few points of the output surface will be fictitious
        points used to define an equilibrium hyperplane guaranteed to be above
        all the other points. This is used for convex hull computations.

    Dataset of the output attribute as a function of state variables

    None yet.
    if broadcast:
        # Broadcast compositions and state variables along orthogonal axes
        # This lets us eliminate an expensive Python loop
        statevars = np.meshgrid(*itertools.chain(statevar_dict.values(),
                                    sparse=True, indexing='ij')[:-1]
        points = broadcast_to(points, tuple(len(np.atleast_1d(x)) for x in statevar_dict.values()) + points.shape[-2:])
        statevars = list(np.atleast_1d(x) for x in statevar_dict.values())
        statevars_ = []
        for statevar in statevars:
            if (len(statevar) != len(points)) and (len(statevar) == 1):
                statevar = np.repeat(statevar, len(points))
            if (len(statevar) != len(points)) and (len(statevar) != 1):
                raise ValueError('Length of state variable list and number of given points must be equal when '
        statevars = statevars_
    pure_elements = [list(x.constituents.keys()) for x in components]
    pure_elements = sorted(set([el.upper() for constituents in pure_elements for el in constituents]))
    pure_elements = [x for x in pure_elements if x != 'VA']
    # func may only have support for vectorization along a single axis (no broadcasting)
    # we need to force broadcasting and flatten the result before calling
    bc_statevars = np.ascontiguousarray([broadcast_to(x, points.shape[:-1]).reshape(-1) for x in statevars])
    pts = points.reshape(-1, points.shape[-1])
    dof = np.ascontiguousarray(np.concatenate((bc_statevars.T, pts), axis=1))
    phase_compositions = np.zeros((dof.shape[0], len(pure_elements)), order='F')

    param_symbols, parameter_array = extract_parameters(parameters)
    parameter_array_length = parameter_array.shape[0]
    if parameter_array_length == 0:
        # No parameters specified
        phase_output = np.zeros(dof.shape[0], order='C')
        phase_record.obj_2d(phase_output, dof)
        # Vectorized parameter arrays
        phase_output = np.zeros((dof.shape[0], parameter_array_length), order='C')
        phase_record.obj_parameters_2d(phase_output, dof, parameter_array)

    for el_idx in range(len(pure_elements)):
        phase_record.mass_obj_2d(phase_compositions[:, el_idx], dof, el_idx)

    max_tieline_vertices = len(pure_elements)
    if isinstance(phase_output, (float, int)):
        phase_output = broadcast_to(phase_output, points.shape[:-1])
    if isinstance(phase_compositions, (float, int)):
        phase_compositions = broadcast_to(phase_output, points.shape[:-1] + (len(pure_elements),))
    phase_output = np.asarray(phase_output, dtype=np.float_)
    if parameter_array_length <= 1:
        phase_output.shape = points.shape[:-1]
        phase_output.shape = points.shape[:-1] + (parameter_array_length,)
    phase_compositions = np.asarray(phase_compositions, dtype=np.float_)
    phase_compositions.shape = points.shape[:-1] + (len(pure_elements),)
    if fake_points:
        output_shape = points.shape[:-2] + (max_tieline_vertices,)
        if parameter_array_length > 1:
            output_shape = output_shape + (parameter_array_length,)
            concat_axis = -2
            concat_axis = -1
        phase_output = np.concatenate((broadcast_to(largest_energy, output_shape), phase_output), axis=concat_axis)
        phase_names = np.concatenate((broadcast_to('_FAKE_', points.shape[:-2] + (max_tieline_vertices,)),
                                      np.full(points.shape[:-1], phase_record.phase_name, dtype='U' + str(len(phase_record.phase_name)))), axis=-1)
        phase_names = np.full(points.shape[:-1], phase_record.phase_name, dtype='U'+str(len(phase_record.phase_name)))
    if fake_points:
        phase_compositions = np.concatenate((np.broadcast_to(np.eye(len(pure_elements)), points.shape[:-2] + (max_tieline_vertices, len(pure_elements))), phase_compositions), axis=-2)

    coordinate_dict = {'component': pure_elements}
    # Resize 'points' so it has the same number of columns as the maximum
    # number of internal degrees of freedom of any phase in the calculation.
    # We do this so that everything is aligned for concat.
    # Waste of memory? Yes, but the alternatives are unclear.
    # In each case, first check if we need to do this...
    # It can be expensive for many points (~14s for 500M points)
    if fake_points:
        desired_shape = points.shape[:-2] + (max_tieline_vertices + points.shape[-2], maximum_internal_dof)
        expanded_points = np.full(desired_shape, np.nan)
        expanded_points[..., len(pure_elements):, :points.shape[-1]] = points
        desired_shape = points.shape[:-1] + (maximum_internal_dof,)
        if points.shape == desired_shape:
            expanded_points = points
            # TODO: most optimal solution would be to take pre-extended arrays as an argument and remove this
            # This still copies the array, but is more efficient than filling
            # an array with np.nan, then copying the existing points
            append_nans = np.full(desired_shape[:-1] + (desired_shape[-1] - points.shape[-1],), np.nan)
            expanded_points = np.append(points, append_nans, axis=-1)
    if broadcast:
        coordinate_dict.update({key: np.atleast_1d(value) for key, value in statevar_dict.items()})
        output_columns = [str(x) for x in statevar_dict.keys()] + ['points']
        output_columns = ['points']
    if parameter_array_length > 1:
        parameter_column = ['samples']
        coordinate_dict['param_symbols'] = [str(x) for x in param_symbols]
        parameter_column = []
    data_arrays = {'X': (output_columns + ['component'], phase_compositions),
                   'Phase': (output_columns, phase_names),
                   'Y': (output_columns + ['internal_dof'], expanded_points),
                   output: (['dim_'+str(i) for i in range(len(phase_output.shape) - (len(output_columns)+len(parameter_column)))] + output_columns + parameter_column, phase_output)
    if not broadcast:
        # Add state variables as data variables rather than as coordinates
        for sym, vals in zip(statevar_dict.keys(), statevars):
            data_arrays.update({sym: (output_columns, vals)})
    if parameter_array_length > 1:
        data_arrays['param_values'] = (['samples', 'param_symbols'], parameter_array)
    return LightDataset(data_arrays, coords=coordinate_dict)

[docs]def calculate(dbf, comps, phases, mode=None, output='GM', fake_points=False, broadcast=True, parameters=None, to_xarray=True, **kwargs): """ Sample the property surface of 'output' containing the specified components and phases. Model parameters are taken from 'dbf' and any state variables (T, P, etc.) can be specified as keyword arguments. Parameters ---------- dbf : Database Thermodynamic database containing the relevant parameters. comps : str or sequence Names of components to consider in the calculation. phases : str or sequence Names of phases to consider in the calculation. mode : string, optional See 'make_callable' docstring for details. output : string, optional Model attribute to sample. fake_points : bool, optional (Default: False) If True, the first few points of the output surface will be fictitious points used to define an equilibrium hyperplane guaranteed to be above all the other points. This is used for convex hull computations. broadcast : bool, optional If True, broadcast given state variable lists against each other to create a grid. If False, assume state variables are given as equal-length lists. points : ndarray or a dict of phase names to ndarray, optional Columns of ndarrays must be internal degrees of freedom (site fractions), sorted. If this is not specified, points will be generated automatically. pdens : int, a dict of phase names to int, or a seq of both, optional Number of points to sample per degree of freedom. Default: 2000; Default when called from equilibrium(): 500 model : Model, a dict of phase names to Model, or a seq of both, optional Model class to use for each phase. sampler : callable, a dict of phase names to callable, or a seq of both, optional Function to sample phase constitution space. Must have same signature as 'pycalphad.core.utils.point_sample' grid_points : bool, a dict of phase names to bool, or a seq of both, optional (Default: True) Whether to add evenly spaced points between end-members. The density of points is determined by 'pdens' parameters : dict, optional Maps SymPy Symbol to numbers, for overriding the values of parameters in the Database. Returns ------- Dataset of the sampled attribute as a function of state variables Examples -------- None yet. """ # Here we check for any keyword arguments that are special, i.e., # there may be keyword arguments that aren't state variables pdens_dict = unpack_kwarg(kwargs.pop('pdens', 2000), default_arg=2000) points_dict = unpack_kwarg(kwargs.pop('points', None), default_arg=None) callables = kwargs.pop('callables', {}) sampler_dict = unpack_kwarg(kwargs.pop('sampler', None), default_arg=None) fixedgrid_dict = unpack_kwarg(kwargs.pop('grid_points', True), default_arg=True) parameters = parameters or dict() if isinstance(parameters, dict): parameters = OrderedDict(sorted(parameters.items(), key=str)) if isinstance(phases, str): phases = [phases] if isinstance(comps, (str, v.Species)): comps = [comps] comps = sorted(unpack_components(dbf, comps)) if points_dict is None and broadcast is False: raise ValueError('The \'points\' keyword argument must be specified if broadcast=False is also given.') nonvacant_components = [x for x in sorted(comps) if x.number_of_atoms > 0] all_phase_data = [] largest_energy = 1e10 # Consider only the active phases list_of_possible_phases = filter_phases(dbf, comps) if len(list_of_possible_phases) == 0: raise ConditionError('There are no phases in the Database that can be active with components {0}'.format(comps)) active_phases = {name: dbf.phases[name] for name in filter_phases(dbf, comps, phases)} if len(active_phases) == 0: raise ConditionError('None of the passed phases ({0}) are active. List of possible phases: {1}.'.format(phases, list_of_possible_phases)) models = instantiate_models(dbf, comps, list(active_phases.keys()), model=kwargs.pop('model', None), parameters=parameters) if isinstance(output, (list, tuple, set)): raise NotImplementedError('Only one property can be specified in calculate() at a time') output = output if output is not None else 'GM' # Implicitly add 'N' state variable as a string to keyword arguements if it's not passed if kwargs.get('N') is None: kwargs['N'] = 1 if np.any(np.array(kwargs['N']) != 1): raise ConditionError('N!=1 is not yet supported, got N={}'.format(kwargs['N'])) # TODO: conditions dict of StateVariable instances should become part of the calculate API statevar_strings = [sv for sv in kwargs.keys() if getattr(v, sv) is not None] # If we don't do this, sympy will get confused during substitution statevar_dict = dict((v.StateVariable(key), unpack_condition(value)) for key, value in kwargs.items() if key in statevar_strings) # Sort after default state variable check to fix gh-116 statevar_dict = OrderedDict(sorted(statevar_dict.items(), key=lambda x: str(x[0]))) phase_records = build_phase_records(dbf, comps, active_phases, statevar_dict, models=models, parameters=parameters, output=output, callables=callables, build_gradients=False, build_hessians=False, verbose=kwargs.pop('verbose', False)) str_statevar_dict = OrderedDict((str(key), unpack_condition(value)) for (key, value) in statevar_dict.items()) maximum_internal_dof = max(len(models[phase_name].site_fractions) for phase_name in active_phases) for phase_name, phase_obj in sorted(active_phases.items()): mod = models[phase_name] phase_record = phase_records[phase_name] points = points_dict[phase_name] variables, sublattice_dof = generate_dof(phase_obj, mod.components) if points is None: points = _sample_phase_constitution(phase_name, phase_obj.constituents, sublattice_dof, comps, tuple(variables), sampler_dict[phase_name] or point_sample, fixedgrid_dict[phase_name], pdens_dict[phase_name]) points = np.atleast_2d(points) fp = fake_points and (phase_name == sorted(active_phases.keys())[0]) phase_ds = _compute_phase_values(nonvacant_components, str_statevar_dict, points, phase_record, output, maximum_internal_dof, broadcast=broadcast, parameters=parameters, largest_energy=float(largest_energy), fake_points=fp) all_phase_data.append(phase_ds) # speedup for single-phase case (found by profiling) if len(all_phase_data) > 1: concatenated_coords = all_phase_data[0].coords data_vars = all_phase_data[0].data_vars concatenated_data_vars = {} for var in data_vars.keys(): data_coords = data_vars[var][0] points_idx = data_coords.index('points') # concatenation axis arrs = [] for phase_data in all_phase_data: arrs.append(getattr(phase_data, var)) concat_data = np.concatenate(arrs, axis=points_idx) concatenated_data_vars[var] = (data_coords, concat_data) final_ds = LightDataset(data_vars=concatenated_data_vars, coords=concatenated_coords) else: final_ds = all_phase_data[0] if to_xarray: return final_ds.get_dataset() else: return final_ds